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Assessment regarding energy saving and decoupling for different AHU
(air handling unit) and control strategies in the hot-humid climatic
region of Iraq
Raad Z. Homod*
Department of Petroleum and Gas Engineering, University of Basrah, Qarmat Ali Campus, 61004 Basrah, Iraq
a r t i c l e i n f o
Article history:
Received 31 January 2014
Received in revised form
9 July 2014
Accepted 16 July 2014
Available online 12 August 2014
Keywords:
Decoupling HVAC system
Improving control performance
PMV model
HVAC energy efficiency
Optimal thermal comfort
a b s t r a c t
In a hot and humid climate, HVAC (heating, ventilating and air conditioning) systems go through rigorous
coupling procedures as a result of indoor conditions, which are significantly affected by the outdoor
environment. Hence, a traditional method for addressing a coupling setback in HVAC systems is to add a
reheating coil. However, this technique consumes a significant amount of energy. Three different stra-
tegies are designed in a hot and humid climate region, such as Basra, for AHUs (air handling unit), and
their evaluations of decoupling are compared. The first and second strategies use the same feedback
control references (temperature and relative humidity), except the second one also uses a reheating coil
and a wet main cooling coil. The AHU (air handling unit) of the third (proposed) strategy is equipped
with a dry main cooling coil and a wet pre-cooling coil to dehumidify fresh air, which allows the
controller to handle the coupling problem. Furthermore, the proposed strategy utilises the PMV (pre-
dicted mean vote) index as a feedback control reference to increase optimisation parameters that provide
more flexibility in meeting the thermal comfort sensation. The adaptive control algorithm of nonlinear
multivariable systems is adopted to coordinate these three policies of optimisation. The results of the
three strategies show that the proposed scheme achieved the desired thermal comfort, superior per-
formance, adaptation, robustness and implementation without using a reheating coil.
© 2014 Elsevier Ltd. All rights reserved.
1. Introduction
In recent decades, studies on the parameters of HVAC (heating,
ventilating and air conditioning) systems, such as the temperature,
PMV (predicted mean vote), HVAC system structure volume and
control strategies, have demonstrated high performance in HVAC
systems, particularly in regard to saving energy [1]. Temperature is
commonly used as the thermal comfort control objective in early
HVAC systems [2,3]. However, temperature alone does not ensure a
person's thermal comfort [4]. Temperature and relative humidity
are coupled; hence, it is difficult to control both factors when each
has its own strict set point [5]. But, the demands for modern HVAC
systems regarding highly systematic products, material integration
and energy integration have resulted in strictly coupled processes.
This coupling has exposed many of the uninvited characteristics of
HVAC systems, which are reflected in the limitations of the classical
controllers, such as PID (Proportional Integral Derivative), that are
used to manipulate the AHU (air handling unit) inputs. Further-
more, the currently used PID tuning techniques are inadequate
when dealing with MIMO (multi-input, multi-output) processes
[6,7]. PI (Proportional Integral) and PID controllers are commonly
used in HVAC systems due to their simplicity in structure and their
relative effectiveness; additionally, the units can be easily under-
stood, which makes them practical to implement [8].
Usually, the decoupling method is adopted to release or alleviate
the coupling of two or more of the control objectives in two or more
of the interlaced loops, which is a difficult task for most of the plant
model because all of the decoupling techniques have limitations
[9,10]. The conventional solution includes adding a reheating coil to
address this coupling setback. However, the use of a reheating coil
increases the power consumption through the control of the RH
(relative humidity) in the conditioned space when the thermal
comfort is maintained at an acceptable level [11,12]. Generally, two
types of decoupling control systems are currently used: static and
dynamic. Static decouplers are effective when high response con-
trols are not required to oversee the processes [13]. Additionally,
the design of static decouplers is straightforward, and their
implementation is based on the inverse process of steady state
* Tel.: þ964 7821731696; fax: þ964 60 389212116.
E-mail addresses: raadahmood@yahoo.com, raad.homod@uobasrah.edu.iq.
Contents lists available at ScienceDirect
Energy
journal homepage: www.elsevier.com/locate/energy
http://dx.doi.org/10.1016/j.energy.2014.07.047
0360-5442/© 2014 Elsevier Ltd. All rights reserved.
Energy 74 (2014) 762e774
gains. However, static decouplers may not always be able to provide
satisfactory control performance. In contrast, dynamic decouplers
require detailed process models, but they provide better perfor-
mance than static decouplers provide [14,15]. For practical opera-
tions, the emphasis is typically placed on suitability and causality
needs, which makes precise configurations difficult to achieve,
especially for high-dimensional MIMO processes. To settle these
difficulties, most of these methodologies focus on TITO (two input
and two output) systems [16,17]. The main shortcoming of the
dynamic methods lies in the complexities of the decoupler ele-
ments, which are obtained from the apparent process model. The
difficulty becomes greater for sophisticated plants because the
technique incorporates the determinant of the model transfer
function [18]. Additionally, the requirement for the decoupler is
that all of its elements must be proper, causal and stable [19]. A few
studies in the literature have focused on the inverted decoupling
methods that are used to reduce variable interactions in the process
[18e22]. Gagnon [10] demonstrated that the performance of
inverted decoupling depends on the scheme of implementation.
When inverted, decoupling is implemented with a lead-lag and
delay function process, and the control performance retreats.
Normalised decoupling control design methodology was used by
Shen [23]. For this type of decoupling, the ETF (equivalent transfer
function) of each element in the transfer function matrix was
required to derive the closed-loop of the plant model, including the
algorithm of the control system. Then, the decoupler was obtained
by multiplying the inverse of the ETF by a stable, proper and causal
ideal-diagonal transfer function.
This paper seeks to analyse and discover the paramount choice
of controlled parameters in the HVAC systems, which are reflected
in optimisation controller performances. However, the controller's
performance is related to buildings' energy efficiency, which is
most directly affected by the decoupling problem. Therefore, in this
study, the extensive and elaborate models of a building that has
HVAC system components are used to simulate a real system.
Deriving the matrices of decoupling, inverted decoupling or ETF
from such a complex model is challenging because all of its ele-
ments must be proper, causal and stable. In concision, the HVAC
control systems use both temperature and RH as references instead
of using temperature only, which is what the earlier mode did.
Because temperature and RH are coupled, it is difficult to control
them separately for a certain desired value [11].
Nomenclature
Symbols
A surface area, m2
C heat capacitance, J/C
dEs/dt rate of change in storage energy of the system, J/s
E;
in energy rate entering the system, J/s
E:
out energy rate leaving the system, J/s
M mass, kg
Cp specific heat, J/kgC
m: mass flow rate, kg/s
Mcp heat capacitance, J/C
T temperature, Co
u humidity ratio, kgw/kgda
h latent heat/heat transfer coefficient, J/kg, W/(m2C)
Q:
cooling load, WC
CF surface cooling factor, W/m2
U construction U-factor, W/(m2C)
DT cooling design temperature difference, C
OFt, OFb, OFr opaque-surface cooling factors
DR cooling daily range, C
CFfen surface cooling factor, W/m2
UNFRC fenestration U-factor, W/(m2C)
PXI peak exterior irradiance, W/m2
SHGC solar heat gain coefficient
IAC interior shading attenuation coefficient
FFs fenestration solar load factor
Et, Eb, ED peak total, diffuse, and direct irradiance, W/m2
Tx transmission of the exterior attachment
Fshd fraction of the fenestration shaded by overhangs or fins
L site latitude, N
SLF shade line factor
Doh depth of the overhang, m
Xoh vertical distance from the top of the fenestration to the
overhang, m
Fcl shade fraction closed (0e1)
j exposure (surface azimuth), measured as degrees from
south
V;
volumetric flow rate, L/s
DF infiltration driving force, L/(s cm2
)
 thermal resistance, C/W
Noc number of occupants
Nbr number of bedrooms
aroof roof solar absorbance
t time constant, s
I infiltration coefficient
Du indooreoutdoor humidity ratio difference, kgw/kgda
Subscripts
m air in mixing box
r room/return
o outside
os outside supply
i inside
He heat exchanger
a air
w water
aHe air in the heat exchanger
L leakage
Win water input
Wout water output
Wl wall
room inside room
out outside room
g glass
fg heat of vaporization
Opq opaque
inf infiltration
fen fenestration
f indoor and outdoor
t at time t
flue flue effective
es exposed
ul unit leakage
ig internal gains
l latent
s sensible/supply
fur furniture
cl closed
R.Z. Homod / Energy 74 (2014) 762e774 763
It is possible to solve a problem in which the variables of tem-
perature and relative humidity are coupled. The first modification in
AHUs is the addition of a fresh air pre-cooling coil that is used to
alleviate the coupling intensity, which is particularly necessary in
humid climates. The second modification for control objectives is the
increase of the optimisation parameters of the output controller by
adding a model of the PMV index in order to evaluate indoor thermal
comfort. Next, decoupling and reduction in energy are simulated by
comparing three different systems under real weather conditions
within certain set point comfort limits. The first system is a con-
ventional system in which the objective is to achieve the tempera-
ture and relative humidity that are within the limits of the desired
conditions. The second system is similar to the first, with the only
difference being the addition of a reheating coil and a wet main
cooling coil in AHUs that are used to solve the coupling problem.
However, these additional reheating and wet main cooling coils
double the energy consumption of the unit due to the addition of
two processes: an implemented sub-cooling process that reduces the
RH and reheating the supplied air in order to meet the desired levels
of thermal comfort. The third system is the same as the first, but it
has an additional pre-cooling coil and controller objective where a
PMV model is added to facilitate the controller optimisation for four
outputs (i.e., the dry bulb temperature, the radiant temperature, the
relative air velocity and the relative humidity for an indoor condi-
tioned space). Controller (TSKFIS (TakagieSugenoeKang fuzzy
inference system)) optimisation is achieved by manipulating the five
AHU inputs (control outputs), which are in the form of the flow rate
of chilled water for the pre-cooling coil and the main cooling coil, the
flow rate of the supply air (fresh air and return air) and the fan speed
of the supply air. Additionally, the PMV model strategy does not
require the use of a reheating coil for decoupling purposes.
The main contribution of this paper is to address the coupling
problem, which arises in the hot and humid climatic region of
South Iraq, by modifying the AHU and applying the algorithm of the
adaptive multi-variable control TSKFF (the Takagi-SugenoeKang
fuzzy forward).
2. Control system design
The present paper attempts to address the shortfall on energy
savings and decoupling for buildings with HVAC control systems in
the hot and humid climatic region of Iraq. Careful assessments in
simulated environments are considered. The PMV model is added
to enable controller decoupling of temperature and RH. Increasing
manipulation parameters are used to compensate for any bounded
variations that may arise due to the limitation of the dampers
range. This is considered as a limitation because the HVAC control
systems have set upper and lower control limits for the dampers
range in order to maintain ventilation for acceptable indoor air
quality, according to the ANSI/ASHRAE 62 standard [24].
2.1. TSKFF controller
The industry standard PID controller exhibits the inability to
control the objectives of the HVAC system that have inherently
adverse characteristics, such as a nonlinear, large-scale system with
a large thermal inertia, a pure lag time, constraints and factors of
uncertain disturbances. Additionally, the indoor thermal comfort
must be decoupled from the temperature and relative humidity.
Hence, fuzzy logic controllers are used due to their flexibility and
intuitive use [25] in controlling the aforementioned characteristics.
2.1.1. Basic description of the control system
The most important motivation for adopting this type of
controller is due to it being able to treat multi-controlled variables
because it converts a TSKFIS (TakagieSugenoeKang fuzzy inference
system) model into a memory layers parameters (TKS) model. The
output routine of the classical TSKFIS model requires numerical and
logical operation tasks, and these tasks take a long time to be
completed. However, the TSK model uses the gradient algorithm,
which is a faster online tuning method that requires less mathe-
matical manipulations than other traditional methods, such as the
backpropagation method for neural networks. The most important
aspect of online tuning is that it can tune a multivariable controller
with multiple outputs; this tuner can improve the controller's
ability to deal with MIMO models that possess a large-scale
nonlinear aspect, are heavily coupled, have a pure lag time,
contain large thermal inertia, possess uncertain disturbance factors
and have constraints, which are common properties in HVAC sys-
tems. For the purpose of this study, each strategy of the control
structure is developed by upgraded layers of memory in order to
coordinate the modification of AHUs, which follows a change in the
online tuning system.
2.1.2. Model identification architecture
The main concept of the TSKFF (Takagi-SugenoeKang fuzzy
forward) structure is based on obtaining the consequent parame-
ters by mapping them from the antecedent space to the consequent
space. The obtained parameters of the consequent space are
organised as layers in the memory space. The parameters in these
layers function to the inputs of the model. These inputs calculate the
outputs' data set, which can be clustered into seven groups within a
time frame of 24 h, where each cluster for each output is repre-
sented by TSK rules. The outputs Yj(X) must fit the data set. This can
be achieved by modulating the nonlinear equation for each output
yi. The modulation can be attained by tuning the parameters ai and
bi. The offline tuning method is performed by using the GNMNR
(GausseNewton Method for the Nonlinear Regression) algorithm,
which has the capability to express the knowledge that is acquired
from inputeoutput data in the form of layers of parameters. The
Equation of the final model's outputs is characterised by aggre-
gating the clusters' outputs and obtaining the singleton fuzzy
model, which belongs to a general class of the universal model
output. Subsequently, the outputs Yj(X) can be obtained as follows:
Yj ðX Þ ¼
XN
i
uiai

1 À eÀbix

(1)
where X ¼ [x1, x2 … xm]T
is the input variables vector, i is a rule
number subscript, ai and bi are the Tagaki-SugenoeKang parame-
ters functions, ui is the basis function (weight), and j is the cluster
number subscript.
The TSK model can be structured in layers f (x; ai bi) and the
weights framework that is shown in Fig. 1 where f (x; ai bi) is a
nonlinear function of the TSK parameters and the independent
variable x.
The TSKFF is modelled by collecting training data from the
building and the HVAC system equipment. Learning of the pa-
rameters in the TSKFF model is accomplished by the offline GNMNR
algorithm. One of the advantages that the GNMNR algorithm offers
is the real-time implementation of computational cost reduction.
This is possible because the proposed method requires a lower
number of iterations to perform the learning/training procedure;
therefore, the tuning time will be reduced when it is implemented
in real-time [5]. The controller method is realised by the TSKFF feed
forward model to increase the response and time steady state
control for the HVAC system. Additionally, the feed forward model
is tuned online by using the gradient algorithm to enhance the
stability and to reject the disturbances and uncertain factors. By
using the gradient algorithm, a faster online tuning method is
R.Z. Homod / Energy 74 (2014) 762e774764
found that requires less mathematical manipulations than other
methods do, such as the backpropagation method for neural net-
works. The most important aspect of this online tuning is that it can
tune a multivariable controller with multiple outputs [11].
2.2. Decoupling problem and objectives' setting
The cooling coils in AHUs are categorised into dry and wet types.
The temperature and relative humidity of air that is introduced to
the AHU that has a dry cooling coil are characterised by coupling
loops due to the constant air humidity ratio. Once the temperature
is decreased, the relative humidity will be increased and vice versa.
The thermal comfort can be controlled through the PMV index by
using this type of AHU, with either air temperature or air relative
humidity being a control variable (but not with both being control
variables at the same time). The rest of the PMV variables are
considered to be disturbances. It is desirable to control temperature
and relative humidity independently and accurately in certain in-
door conditions. In these cases, the AHU with a wet cooling coil is
used; both temperature and RH are varied independently based on
the flow rates of air and chilled water. It is impossible to set one
variable without affecting the other when the design of the AHU
does not take into account the coupling dynamics between these
variables; therefore, the importance of decoupling techniques that
are used to implement an appropriate AHU is realised.
The proposed strategy is implementing a twin cooling coil AHU
and an advanced multi-variable control system. The pre-cooling
coil (wet) is equipped to cool and dehumidify the fresh air intake.
The main cooling coil (dry) is used to cool the supply air. The deeply
chilled water is only necessary for (pre-cooling coil) removing the
moisture from the fresh air. The main cooling coil requires
moderately cool water, according to the building load. This type of
order helps in save energy for buildings with HVAC systems
because higher chilled water temperatures indicate better COPs
(coefficients of performance). Furthermore, the use of the PMV
index (the indoor air temperature, the radiant temperature, the
relative air velocity and the relative humidity for an indoor condi-
tion space) as a desired objective enables the control system to
optimise the input plant by controlling air velocity and manipu-
lating the flow rate of fresh air in regard to thermal comfort levels.
The main difference between the proposed strategy and the
other two strategies is in their control objectives of the operating
system and AHU equipment. The AHU for the conventional strategy
is similar to what it is for proposed strategy, but there are two
differences: first, it does not contain a pre-cooling coil, and second,
the controlled variables include two variables that have restricted
values. These variables are temperature and relative humidity; both
of them are set at desired specific values. The objective of this
control strategy acts as a control reference of the online tuning that
reflected negatively on its performance due to stiff references and a
limited number of input plant variables that are used for optimi-
sation. The controlled variables for the third (adding the reheating
coil) strategy are similar to those of the conventional strategy, but
the difference is that the AHU is equipped with a wet main cooling
coil and a reheating coil to consolidate the controller for the
decoupling problem.
The objectives of this paper are to:
1. Assess the feasibility of using the proposed strategy in a South
Iraq climate
2. Characterise the energy savings and decoupling of the proposed
system
3. Test the potential of the controller for multi-objective optimi-
sation in the HVAC system.
These aims will be achieved by comparing three scenarios of the
AHU control system in order to assess the decoupling problem and
energy savings of the simulated HVAC system.
3. Analysis of energy and mass flows of a building
The purpose of the control strategy is to minimise the total
power consumption of the HVAC system by optimising the vari-
ables of the indoor thermal comfort (i.e., the indoor air tempera-
ture, the radiant temperature, the relative air velocity and the
relative humidity for the indoor condition space). Generally, the
electric power consumption of the HVAC system is a function of the
COP (coefficient of performance) of the chillers, the EER (energy
efficiency ratio) of the building and the cooling load of the building.
The EER and COP are constants for a specified building and chiller,
respectively, whereas the total cooling loads of the building vary,
depending on the disturbances and the controllable variables.
Therefore, the total electric power consumption can be summarised
by Equation (2) [26,27]:
EP ¼
XN
i
chli
copi
þ EPAHU ¼
TBCL
EER
(2)
where EP is the total electric power consumption, N is the number
of chillers, chl is the chiller power, EPAHU is the electric power that is
consumed by AHU, and TBCL is the total building's cooling load.
From Equation (2), it can clearly be observed that the EP can be
derived by using two different methods that are based on the
energy and mass balance equations of the building's fabric (the
right term of Equation (2)) and of the AHU subsystems' equipment
(the middle term of Equation (2)). Therefore, the theories
regarding the conservation of energy and mass are applied to
thermally analyse and model the overall behaviour of an HVAC
system. These theories are based on the fact that in the control
volume of any subsystem, energy is transferred from/to a sub-
system by two types of processes: mass transfer and conventional
Fig. 1. Schematic diagram of the TSK model as layers of memory.
R.Z. Homod / Energy 74 (2014) 762e774 765
heat transfer (conduction, convection and radiation). These pro-
cesses are dominant in HVAC systems. In this research study, the
system is subdivided into the building's and the AHU's control
volumes. The building's energy and mass transfer can be demon-
strated by Fig. 2. To evaluate the sensible heat gain of the building,
the following thermal balance equation is applied to the building's
control volume:
The term on the left side of Equation (3) denotes the output of
the AHU, which represents the heat and mass that is transferred to
the building's control volume. On the right side of Equation (3), the
first part (the accumulation or storage of energy) represents the
thermal mass that is stored in the inner wall, indoor air and
furniture, while the second part (the difference between the input
and output of energy) represents other inputs/outputs to the con-
trol volume of the building.
The latent heat gain of the building is related to the moisture
transfer, which can be evaluated by applying the conservation of
time-dependent mass law to the control volume of the building,
which is shown in Equation (4);
The term on the left side of Equation (4) is the rate of moisture
that is absorbed by the AHU. On the right side of Equation (4), the
first part (the rate of moisture change) is the change in the rate of
air moisture in the building at time interval dt, and the other terms
are related to the indoor input/output and the generated moisture.
To evaluate the sensible and latent heat gains of the building, it is
necessary to calculate the left-hand sides of Equations (3) and (4),
which can be obtained by applying the laws of conservation of energy
and mass to the control volume of the AHU. The AHU is subdivided
into three subsystems: the mixing air chamber, the pre-cooling coil
and the main cooling coil. Energy is only consumed in the pre-cooling
and main coolingcoils,socalculations for the energyand mass control
volumes are applied on these two subsystems, as follows:
The term “energy absorbed by the coil” in Equation (5) refers to
the sensible and latent heat load that is exerted by the pre-cooling
coil. On the right side of the equation, the first term (energy
accumulation in the metal mass of the coil) refers to the rate of
change for the heat storage in the coil mass, while the second term
(the sensible energy delivered by air) refers to the sensible cooling
load of the fresh air, and the third term (the latent energy delivered
by moisture withdrawal) refers to the latent energy that is absorbed
by the coil due to the condensation of moisture. The third term on
the right side of Equation (5) can be evaluated by applying the law
of mass conservation to the air flow stream that is used for the pre-
cooling coil. The following is obtained:
By using the same procedure as was used for the pre-cooling coil
to obtain the sensible and latent heating loads for the dynamic
subsystem equations, the main cooling coil can be written mathe-
matically by using the time-dependent equation of the control
volume, as follows:
_Qs
z}|{
Cooling load
¼ _Qair þ _Qfur
zfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflffl{Accumulation or storage of energy
þ _Qopq þ _Qfen þ _Qslab þ _Qinf þ _Qig;s
zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
Difference between input and output of energy
(3)
_ms
À
ur;t À us;t
Ázfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflffl{
rate of moisture withdrawal by AHU
¼
dMrur;t
dt
zfflfflfflffl}|fflfflfflffl{
rate of moisture change
þ
_Qig;l
hfg
zffl}|ffl{
rate of moisture generation
þ _minf uo;t À _mrur;t
zfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflffl{
rate of moisture transfer
(4)
_mw;tcpw
À
Two;t À Twin;t
Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
energy absorbed by the coil
¼ MHecpHe
dTh;t
dt
zfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflffl{
energy accumulation in the metal mass of coil
þ _mo;tcpa
À
To;t À Tos;t
Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
sensible energy delivered by air
þ _mo;t

uo;t À uos;t

hfg
zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
latent energy delivered by air dehumidification
(6)
_mw;tcpw
À
Two;t À Twin;t
Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
energy absorbed by the coil
¼ MHecpHe
dTh;t
dt
zfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflffl{
energy accumulation in the metal mass of coil
þ _mo;tcpa
À
To;t À Tos;t
Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
sensible energy delivered by air
þ _mcon:;thfg
zfflfflfflfflfflffl}|fflfflfflfflfflffl{
latent energy delivered by moisture withdrawal
(5)
R.Z. Homod / Energy 74 (2014) 762e774766
The rate of thermal energy transfer (the sensible cooling load)
from the building by the mechanical ventilation air flow (Qvent) is
calculated by using Equation (8).
_Qvent ¼ _ms;tcpa

Tr;t À Ts;t

(8)
The power of the air supply system in the mechanical ventila-
tion state (the transmission power) is mainly from the power
supply for the fan, which can be calculated by the application of the
law of conservation of energy on the control volume of the AHU.
This equation can be calculated as follows [27]:
_Qfan ¼ _ms;tcpa

Ts;t À To;t

(9)
According to the energy balance for the indoor conditioned
space of Equation (3), the values of thermal energy flow from (1)
opaque-surfaces, (2) transparent fenestration surfaces, (3) infiltra-
tion, (4) indoor load and (5) ventilation are calculated by using the
steady state conditions of Equation (3), whereby all of the thermal
energy flow values are equal to the cooling load that is extracted by
the HVAC systems or the mechanical ventilation, which equals the
left-hand side of Equation (3); in turn, Equation (3) can be calcu-
lated by summing Equations (6)e(9).
The instantaneous cooling load of the building can be obtained
from the simulation process after modelling the HVAC system.
Additionally, the instantaneous cooling loads of the building
directly impact the outputs of the controller signals. Therefore, the
method of calculation that is employed in this research study is
based on the output signals of the controller. The output signals of
the controller manipulate the valves of the pre-cooling coil, the
main cooling coil, the reheating coil and the dampers of the return
and fresh air to track the objective of the HVAC system. The valves
and dampers are designed according to the heating/cooling load of
the building. The opening position of the valves and dampers is
recorded as a percentage of the fullest extent (as shown in Fig. 3)
that represents the main cooling coil valve's opening position over
24 h. The percentage of the opening position is related to the
maximum flow rate of the valves and dampers. This signal opening
position is implemented in Matlab to obtain the energy con-
sumption of the HVAC system.
The advantage of using Matlab/Simulink is in the ability to use a
graphical programming language that is based on different block
categories with different properties of each block. Matlab and its
Fig. 3. The control signal percentage for the main cooling coil's chilled water valve for each of the three strategies.
Fig. 2. Representation of building energy and mass transfer for prototypical buildings
with HVAC systems.
_mmw;tcpw
À
Two;t À Twin;t
Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
energy absorbed by the coil
¼ MmHecpHe
dTh;t
dt
zfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflffl{
energy accumulation in the metal mass of coil
þ _mm;tcpa
À
Tm;t À Ts;t
Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
sensible energy delivered by air
þ _mm;t

um;t À us;t

hfg
zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{
latent energy delivered by air dehumidification
(7)
R.Z. Homod / Energy 74 (2014) 762e774 767
toolboxes are adopted to perform all of the identification processes
and simulations in this work, as well as in our previous works
[28e31]. System identification and control system toolboxes were
used to identify and build the model, while the fuzzy logic toolbox
was used for the TSK model identification. The obtained models are
then introduced in the Matlab/Simulink environment for simula-
tion and analysis. These categories include the input/output,
transfer functions, arithmetic functions, state space models and
data handling. The building model is represented in the form of
ODE (ordinary differential equation) solvers, which are automati-
cally configured during the Simulink model's run-time. The algo-
rithm of the controller is designed by using Matlab m-files,
parameter layer memory and S-functions, which are based on on-
line parameter tuning. The technique for calculating the cooling
loads is easily implementable, whereby the thermal balance
equation is derived from the arithmetic functions, from which the
energy consumption can be obtained.
4. Simulation results and discussion
4.1. Physical and theoretical model description
The simulated building model is a typical one-story house with
a simple structure. The house consists of heavyweight construction
(brick and concrete) that measures 4.5 m in height, with 248.6 m2
of gross ground floor area. The net floor area of the entire building is
195.3 m2
, excluding the garage area; the gross exposed area of the
windows and wall is 126.2 m2
, while the net area of the exterior
wall is 108.5 m2
. The overall volume of the house, excluding the
garage and suspended ceiling space, is 781.2 m3
Table 1 shows the
physical properties of the components of the building. The dry bulb
temperature varies according to the spring season's climate in
Basrah city, which ranges from 18 C to 32 C, and the humidity
ratio varies from 0.01 to 0.01909 kg of moisture per kg of dry air. The
building model's transfer function and the PMV, or thermal comfort
sensor model, are presented in Appendices A and B [32,33].
To reduce the design cost, as well as the cost that is needed to
fabricate the three HVAC systems, simulation methods are imple-
mented in order to test and analyse the results. The identification
approach of the model demonstration is based on the multi-zone
model of the RLF (residential load factor) method. The identified
model is simulated by three different controller strategies in order
to study their levels of indoor thermal comfort and energy con-
sumption. The first system is a conventional control system (the
control variable objectives are temperature and relative humidity).
The second is a conventional system that includes the addition of a
reheating coil and a wet main cooling coil, while the third system is
similar to the first system, but it includes an addition of a pre-
cooling coil and a PMV index in order to measure the objective of
the controller. The three types of systems are run together in order
to study their performance and energy consumption (as shown by
the simulation block diagram in Fig. 4, which presents the simu-
lation in the evaluation of performance and energy consumption of
the three systems).
Fig. 4. Matlab blocks for the simulations of all three systems.
Table 1
Properties of the materials used for construction of the model.
Component Description Factors
Roof/ceiling Flat wood frame ceiling
(insulated with R-5.3 fiberglass)
beneath vented attic with
medium asphalt shingle roof
U ¼ 0.031 18 W=ðm2KÞ
a roof ¼ 0.85
Exterior
walls
Wood frame, exterior wood
sheathing, interior gypsum
board, R-2.3 fiberglass
insulation
U ¼ 51 W=ðm2KÞ
Doors Wood, solid core U ¼ 2.3 W=ðm2KÞ
Floor Slab on grade with heavy carpet
over rubber pad; R-0.9 edge
insulation to 1 m below grade
Rcvr ¼ 0.21 W=ðm2KÞ;
Fp ¼ 85 W=ðm2KÞ
Windows Clear double-pane glass in
wood frames. Half fixed, half
operable with insect screens
(except living room picture
window, which is fixed). 0.6 m
eave overhang on east and west
with eave edge at same height
as top of glazing for all
windows. Allow for typical
interior shading, half closed.
Fixed: U ¼ 2.84 W=ðm2KÞ;
SHGC ¼ 0.67.
Operable: U ¼ 2.87 W=ðm2KÞ;
SHGC ¼ 0.57; Tx ¼ 0.64;
IACcl ¼ 0.6
Construction Good Aul ¼ 1.4 cm2
/m2
R.Z. Homod / Energy 74 (2014) 762e774768
The mean radiant temperature is a more complicated quantity
that depends on the temperature of the surrounding surfaces, as
well as on angle factors of the surrounding surfaces. Therefore, the
plant model leads to the output of the plug-in model of the PMV
index, except the mean radiant temperature requires an interme-
diate sub-model where its output is taken into account because it is
one of the main factors that affects thermal comfort. This sub-
model estimates the mean radiant temperature by using two
methods: theoretical and numerical. For the theoretical method,
the mean radiant temperature is estimated from the measured
temperature of the surrounding walls and surfaces and the angle
factors of these surrounding surfaces. All of the indoor surfaces are
assumed to be black because most building materials have a high
emittance ε, and it is assumed that small temperature differences
exist between the surfaces of the enclosure (i.e., linear combination
of system states). Therefore, the following equation is used [34]:
MRT ¼ T1FPÀ1 þ T2FPÀ2 þ / þ TnFPÀn (10)
where MRT is the Mean Radiant Temperature, Tn is the temperature
of surface ‘n’ and Fp-n is the angle factor between a person and
surface ‘n’.
For the numerical estimation, a black-globe thermometer sensor
is used.
4.2. Decoupling results and discussion
The plant model is dynamically subjected by many thermal
disturbance factors, such as the K2 solar radiation, f4 inside sensible,
FDR fenestration, etc. Three simulation sets are conducted over 24 h
and include nominal, noise and sensor deterioration, as well as an
uncertainty operation, for the three systems' behaviours to be
observed and studied for the different conditions. The main
objective of this work is to validate the decoupling of the proposed
strategy.
4.2.1. Nominal operating conditions
Pre-cooling coils are added to the proposed AHU of the HVAC
system in order to economically control the indoor relative hu-
midity in a humid climate. Additionally, the proposed system has
four control variables for an indoor conditioned space (i.e., the
indoor-air temperature, the indoor-air velocity, the indoor-air hu-
midity and the flow rate of fresh air). These control variables are
optimised by the controller to provide economical indoor-air
Fig. 5. PMV comparisons of the results of the three different systems with different objectives and designs.
Fig. 6. Indoor temperature comparisons of the results between the three different systems with different objectives and designs.
R.Z. Homod / Energy 74 (2014) 762e774 769
conditioning that yields the desired level of thermal comfort and
indoor air quality, according to ASHRAE and ISO standards; this also
reduces the cooling load during implementation in real-time. The
other systems have two control objectives that are set at certain
desired values for the indoor conditioned space (i.e., the indoor-air
temperature and the indoor-air humidity). Fig. 4 shows the three
designs of the HVAC system. The manipulation of each TSKFF for
the five AHU inputs in the three designs of the HVAC system be-
haves differently. In the proposed system, the input feedback
sensor allows some degree of tolerance instead of requiring a
specific value for the temperature and relative humidity, which is
needed in the conventional HVAC systems. This optimisation
overcomes the coupling effects (temperature and relative humidi-
ty) perfectly by providing the desired level of thermal comfort,
which is shown in Fig. 5. In regard to Fig. 5, it can be observed that
the proposed (the model of the PMV index addition) system can
track the desired objective and can achieve outstanding perfor-
mance, while the system with the added reheating coil acts within
an acceptable thermal comfort range that has an acceptable offset
from the set point. The conventional system was found to violate
the ASHRAE Standard 55-92 [35] and ISO-7730 [36] for the desired
level of indoor thermal comfort. These standards recommend that
the acceptable levels of thermal comfort are limited to a range
between À0.5  PMV  0.5. It is evident that this violation is caused
by the coupling of temperature and relative humidity. The tem-
perature curves of all three systems are similar to the PMV trend
that is shown in the simulation results, which are tabulated in
Fig. 6. The periodic effect of the coupling factors is apparent from
05:30 o'clock to 08:00 o'clock and from 19:00 o'clock to 24:00
o'clock. The effect can be more clearly observed in the behaviour of
the relative humidity (as shown in Fig. 7), in which the conven-
tional system fluctuates within a wide range, whereas the other
systems remain in the range of approximately 50% RH. The rec-
ommended range of RH, according to the ASHRAE Standard 55-92
and ISO-7730 for the indoor comfort condition, is 40%e60%. High
humidity not only causes poor indoor air quality, but it also causes
wood decay, metal corrosion and structural deterioration [37]. The
calculations of energy consumption are based on the controller
Fig. 7. Indoor relative humidity comparisons of the results between the three different systems with different objectives and designs.
Fig. 8. PMV comparisons of the results of the three different systems based on the operating conditions of noise and sensor deterioration.
R.Z. Homod / Energy 74 (2014) 762e774770
signals. One of these signals is shown in Fig. 3. Fig. 3 shows the
results of the simulation of the control signal variation for the main
cooling coil of the chilled water valve, with respect to time. In Fig. 3,
the signals for the conventional system with a reheating coil acts
similar to a BangeBang control action. The modulating valve
continuously fluctuates between ON-OFF, which will eventually
wear out the valve and shorten its lifespan. It can be clearly
observed that the proposed system signal works very efficiently,
which provides good control performance. Figs. 5e7 show the
transient response for the initial condition. This took approximately
an hour because the plant model is dynamically affected by the
thermal mass of the building structure and slab floors, which cre-
ates a flywheel effect. The influence of this flywheel effect begins to
fade and becomes less intense after the HVAC system starts, which
can clearly be observed in the signal of valve open position in Fig. 3.
4.2.2. Operating conditions of noise and sensor deterioration
Disturbance mode has tested decoupling through its validation
of the rejection of noise and sensor deterioration. In noise and
sensor deterioration, the controlled process parameters, sensors'
gains, and noise signals are able to change in the same manner for
each system and simulation that is conducted. Here, we suppose
that sensors deteriorate with 20% fault, and the sensors' gain is
changed to 0.8 (sensor gain ¼ 1 when the sensor performance is
100%). Additionally, to test the sensitivity of the proposed method
to noise, each system is subjected to the same noisy environment
by adding a 10% NSR (noise-to-signal ratio), which refers to the
ratio of the continuous noise signal to the controlled signal. The
sensor deterioration set and subjected noise signal are applied at
the start of the simulation. Fig. 8 shows the three different systems
to try to track a PMV set point, which changes under a square wave
from À0.4, 0 and 0.4 during a 24 h time frame. By using this test,
one can clearly observe the three systems' behaviour for the PMV,
where the proposed system provides superior control performance
and does not violate the ASHRAE 55-92 and ISO-7730 Standards. In
contrast, the other systems exhibited deterioration in their per-
formances and, consequently, violated the Standards of the indoor
thermal comfort. Thus, the proposed system achieves significant
results that verify the use of decoupling parameters rather than
adding a reheating coil or using conventional decoupling methods,
Fig. 9. PMV comparisons of the results of the three different systems in regard to the operating conditions when model uncertainties are present.
Fig. 10. Psychometric chart comparisons of the results of the three different systems in regard to the operating conditions when model uncertainties are present.
R.Z. Homod / Energy 74 (2014) 762e774 771
which are extremely intricate and too impractical to solve numer-
ically when the plant system model is complicated, which is the
case for HVAC systems.
4.2.3. Operating conditions regarding the presence of model
uncertainties
In regard to robustness validation, the plant model encompasses
a wide range of operating parameters, which vary as the HVAC
systems undergo fluctuating loads due to changes in external dis-
turbances during a typical day's operation. Therefore, in the pres-
ence of uncertainties regarding the modelling of such parameters, it
becomes necessary to use a robust intelligent controller, such as
TSKFF, to obtain efficient operation in the HVAC systems. To vali-
date the robustness of the TSKFF controller, the building heat loss
coefficients, the heat transfer coefficients of the fan-coil units and
pumps and the thermal time constant are changed. Before a
simulation run begins, all of the model coefficients and the time
constant are increased by 20%. Three TSK models of controllers are
tuned based on the nominal plant model and then are integrated
into a control algorithm that manipulates AHU parameters to
control indoor thermal comfort. The conventional strategy leads to
the worst indoor ambient conditions and becomes less intense after
adding a reheating coil, which is shown in Fig. 9. However, both
strategies violate the standard limitation of ASHRAE 55-92 and ISO-
7730. The proposed scheme maintains asymptotic tracking of a
given reference signal, and it occurs in the presence of the same
parameter variations and model uncertainties when it does not use
reheating and wet main cooling coils. For validation, psychometric
charts are the most commonly used tool for indoor studies and
outdoor air conditions. Fig. 10 describes the air states cycle of
physical and thermodynamic properties for indoor conditions over
24 h. The proposed strategy seems to satisfy the TCZ (thermal
comfort zone), whereas the other strategies frequently crossover
TCZ.
4.3. Energy saving results and discussion
The purpose of the model of the PMV index addition to the
proposed system is to change the restricted conventional objective
variables (temperature and relative humidity) of an HVAC system in
Fig. 11. A comparison of the energy consumption results based on the cooling coil load variation between the three different schemes.
Fig. 12. A comparison of the results of the power consumption between the three different system schemes.
R.Z. Homod / Energy 74 (2014) 762e774772
addition to increasing its flexibility with respect to the indoor
control parameters (temperature, fresh air flow rate, indoor air
velocity and relative humidity). The model of the PMV index
addition also enables the controller to improve its performance.
The TSKFF controller exploits the flexibility of the control param-
eters by optimising the parameters through the manipulation of
the AHU parameters (inputs) to provide the desired levels of ther-
mal comfort, while simultaneously reducing the energy con-
sumption of the HVAC system.
Furthermore, the velocity of indoor air can reduce the cooling
load. This can be observed from the simulation results of the energy
that is consumed by the cooling coil load, which is shown in Fig. 11.
The simulation techniques that are used to calculate the cooling
loads are straight forward: thermal balance equations are imple-
mented by using arithmetic functions, and then the consumed
energy can be obtained by using Equations (6)e(9). The simulation
results of the consumed energy in the system with a reheating coil
reveal higher energy consumption than the consumption of the
other systems because the cooling process reduces the air tem-
perature to the sub-cooling state before the reheating process
overcomes the coupling effect and meets the demands of indoor
thermal comfort.
Although the conventional system is better in terms of energy
savings than the system that has the addition of a reheating coil, the
conventional system does not meet the desired level of indoor
thermal comfort. However, the proposed system shows more
favourable results than the other two systems with respect to
achieving the desired level of thermal comfort and reducing energy
consumption, simultaneously. Based on Fig. 11, it can be observed
that the differences in energy consumption among the three sys-
tems increase during the times periods that include the presence of
a coupling effect. The average power consumption for the three
different systems (the conventional system, the addition of a
reheating system and the proposed system) are 10.713 kW,
13.27 kW and 9.016 kW, respectively. The average power costs that
accompany the addition of a reheating system are 1.4718 times
higher than that of the proposed system. Based on the data for 24 h
of power consumption, the calculations for energy consumption for
each of the three strategies show that energy consumption in the
proposed strategy is 32.06% lower than the system with an added
reheating coil, which is shown in Fig.12. This result closely matches
the results that were obtained by Yang and Su [38] in which an
intelligent controller was developed to adjust the PMV index,
which led to saving approximately 30% more of the energy con-
sumption than the conventional methods. Furthermore, the simu-
lation of the cooling coil load output is compared to the numerical
results, which are based on the CLF/CLTDC (the cooling load factor
for the glass/corrected cooling load temperature difference)
method [39,40]. The calculation considers the effects of numerous
outdoor environmental parameters on the indoor thermal loads.
The cooling load of the building is calculated every 30 min to obtain
the absolute margin of error between the simulation results (the
proposed system) and the numerical calculation, which was found
to vary between 0.064 and 0.107 kW. To have a clearer assessment
of the error between the simulation and numerical calculations of
the cooling coil load output, in this study, the statistical index of the
coefficient of determination (r2
) was calculated based on Equation
(11) and had a value of r2
¼ 0.974.
r2
¼
½N
P
yiyi À ð
P
yiÞð
P
yiÞŠ2
h
N
 P
y2
i

À ð
P
yiÞ2

N
 P
y2
i

À ð
P
yiÞ2
i (11)
where yi is the numerical result, yi is the simulation result, and N is
the number of test samples.
5. Conclusion
In this context, the simulation results of the comparison inves-
tigated the use of a PMV model input as an objective optimisation of
controller decoupling and of reductions in the energy consumed by
an HVAC system. This was performed by considering all of the
factors that are affected by indoor thermal comfort, which are re-
flected by the PMV index. The control system that is proposed in
this work includes, as part of its structure, a PMV model for the
optimisation of the deviations in the parameters of indoor thermal
comfort and of the generation of control actions that pertain to the
AHU inputs. The task regarding the PMV index output is, therefore,
to acquire controller output signals more accurately by exploiting
the decision algorithm's flexibility for the PMV index input's ag-
gregation. The weather in Basrah, a southern city of Iraq, was
considered as a case study to test the system. The output controller
signals were adopted to obtain the energy consumption for three
different control objectives and strategies, which were evaluated
with respect to typical and modified HVAC systems. Based on the
results of the performed simulations, we can conclude that when
using the indoor PMV as a variable objective for the HVAC system,
the controller performs better and provides more energy savings,
while still attaining the desired level of indoor thermal comfort.
The multi-input of the AHU is manipulated by the TSKFF controller,
which is characterised by the optimisation of the outputs for energy
savings. Both the conventional and proposed systems show that
energy is saved in comparison to the system that has an additional
reheating coil in the AHU. The conventional HVAC system shows a
savings of up to 19% of energy usage, which is 61.5 kWh/d less than
the energy that is used by an HVAC system that has an additional
reheating coil; in contrast, the proposed strategy can save up to
32.06% of energy usage, which is 102.1 kWh/d less than the energy
that is used by the HVAC system that has an additional reheating
coil. This is because a TSKFF that is equipped with a model of PMV
index reduces the energy consumption of a building by as much as
it can by utilising the outdoor climate in controlling the rate of fresh
air flow. Meanwhile, the conventional control strategy adjusts the
temperature and relative humidity to a predefined strict set point,
which does not allow for optimisation of energy consumption for
indoor thermal comfort. An important finding of this study is that
the proposed strategy economically addressed the coupling prob-
lem in addition to providing the desired level of thermal comfort.
Furthermore, the procedure of using the PMV model and TSKFF is
straightforward and easy to implement.
Appendix A. Supplementary data
Supplementary data related to this article can be found at http://
dx.doi.org/10.1016/j.energy.2014.07.047.
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Assessment regarding energy saving and decoupling for different ahu

  • 1. Assessment regarding energy saving and decoupling for different AHU (air handling unit) and control strategies in the hot-humid climatic region of Iraq Raad Z. Homod* Department of Petroleum and Gas Engineering, University of Basrah, Qarmat Ali Campus, 61004 Basrah, Iraq a r t i c l e i n f o Article history: Received 31 January 2014 Received in revised form 9 July 2014 Accepted 16 July 2014 Available online 12 August 2014 Keywords: Decoupling HVAC system Improving control performance PMV model HVAC energy efficiency Optimal thermal comfort a b s t r a c t In a hot and humid climate, HVAC (heating, ventilating and air conditioning) systems go through rigorous coupling procedures as a result of indoor conditions, which are significantly affected by the outdoor environment. Hence, a traditional method for addressing a coupling setback in HVAC systems is to add a reheating coil. However, this technique consumes a significant amount of energy. Three different stra- tegies are designed in a hot and humid climate region, such as Basra, for AHUs (air handling unit), and their evaluations of decoupling are compared. The first and second strategies use the same feedback control references (temperature and relative humidity), except the second one also uses a reheating coil and a wet main cooling coil. The AHU (air handling unit) of the third (proposed) strategy is equipped with a dry main cooling coil and a wet pre-cooling coil to dehumidify fresh air, which allows the controller to handle the coupling problem. Furthermore, the proposed strategy utilises the PMV (pre- dicted mean vote) index as a feedback control reference to increase optimisation parameters that provide more flexibility in meeting the thermal comfort sensation. The adaptive control algorithm of nonlinear multivariable systems is adopted to coordinate these three policies of optimisation. The results of the three strategies show that the proposed scheme achieved the desired thermal comfort, superior per- formance, adaptation, robustness and implementation without using a reheating coil. © 2014 Elsevier Ltd. All rights reserved. 1. Introduction In recent decades, studies on the parameters of HVAC (heating, ventilating and air conditioning) systems, such as the temperature, PMV (predicted mean vote), HVAC system structure volume and control strategies, have demonstrated high performance in HVAC systems, particularly in regard to saving energy [1]. Temperature is commonly used as the thermal comfort control objective in early HVAC systems [2,3]. However, temperature alone does not ensure a person's thermal comfort [4]. Temperature and relative humidity are coupled; hence, it is difficult to control both factors when each has its own strict set point [5]. But, the demands for modern HVAC systems regarding highly systematic products, material integration and energy integration have resulted in strictly coupled processes. This coupling has exposed many of the uninvited characteristics of HVAC systems, which are reflected in the limitations of the classical controllers, such as PID (Proportional Integral Derivative), that are used to manipulate the AHU (air handling unit) inputs. Further- more, the currently used PID tuning techniques are inadequate when dealing with MIMO (multi-input, multi-output) processes [6,7]. PI (Proportional Integral) and PID controllers are commonly used in HVAC systems due to their simplicity in structure and their relative effectiveness; additionally, the units can be easily under- stood, which makes them practical to implement [8]. Usually, the decoupling method is adopted to release or alleviate the coupling of two or more of the control objectives in two or more of the interlaced loops, which is a difficult task for most of the plant model because all of the decoupling techniques have limitations [9,10]. The conventional solution includes adding a reheating coil to address this coupling setback. However, the use of a reheating coil increases the power consumption through the control of the RH (relative humidity) in the conditioned space when the thermal comfort is maintained at an acceptable level [11,12]. Generally, two types of decoupling control systems are currently used: static and dynamic. Static decouplers are effective when high response con- trols are not required to oversee the processes [13]. Additionally, the design of static decouplers is straightforward, and their implementation is based on the inverse process of steady state * Tel.: þ964 7821731696; fax: þ964 60 389212116. E-mail addresses: raadahmood@yahoo.com, raad.homod@uobasrah.edu.iq. Contents lists available at ScienceDirect Energy journal homepage: www.elsevier.com/locate/energy http://dx.doi.org/10.1016/j.energy.2014.07.047 0360-5442/© 2014 Elsevier Ltd. All rights reserved. Energy 74 (2014) 762e774
  • 2. gains. However, static decouplers may not always be able to provide satisfactory control performance. In contrast, dynamic decouplers require detailed process models, but they provide better perfor- mance than static decouplers provide [14,15]. For practical opera- tions, the emphasis is typically placed on suitability and causality needs, which makes precise configurations difficult to achieve, especially for high-dimensional MIMO processes. To settle these difficulties, most of these methodologies focus on TITO (two input and two output) systems [16,17]. The main shortcoming of the dynamic methods lies in the complexities of the decoupler ele- ments, which are obtained from the apparent process model. The difficulty becomes greater for sophisticated plants because the technique incorporates the determinant of the model transfer function [18]. Additionally, the requirement for the decoupler is that all of its elements must be proper, causal and stable [19]. A few studies in the literature have focused on the inverted decoupling methods that are used to reduce variable interactions in the process [18e22]. Gagnon [10] demonstrated that the performance of inverted decoupling depends on the scheme of implementation. When inverted, decoupling is implemented with a lead-lag and delay function process, and the control performance retreats. Normalised decoupling control design methodology was used by Shen [23]. For this type of decoupling, the ETF (equivalent transfer function) of each element in the transfer function matrix was required to derive the closed-loop of the plant model, including the algorithm of the control system. Then, the decoupler was obtained by multiplying the inverse of the ETF by a stable, proper and causal ideal-diagonal transfer function. This paper seeks to analyse and discover the paramount choice of controlled parameters in the HVAC systems, which are reflected in optimisation controller performances. However, the controller's performance is related to buildings' energy efficiency, which is most directly affected by the decoupling problem. Therefore, in this study, the extensive and elaborate models of a building that has HVAC system components are used to simulate a real system. Deriving the matrices of decoupling, inverted decoupling or ETF from such a complex model is challenging because all of its ele- ments must be proper, causal and stable. In concision, the HVAC control systems use both temperature and RH as references instead of using temperature only, which is what the earlier mode did. Because temperature and RH are coupled, it is difficult to control them separately for a certain desired value [11]. Nomenclature Symbols A surface area, m2 C heat capacitance, J/C dEs/dt rate of change in storage energy of the system, J/s E; in energy rate entering the system, J/s E: out energy rate leaving the system, J/s M mass, kg Cp specific heat, J/kgC m: mass flow rate, kg/s Mcp heat capacitance, J/C T temperature, Co u humidity ratio, kgw/kgda h latent heat/heat transfer coefficient, J/kg, W/(m2C) Q: cooling load, WC CF surface cooling factor, W/m2 U construction U-factor, W/(m2C) DT cooling design temperature difference, C OFt, OFb, OFr opaque-surface cooling factors DR cooling daily range, C CFfen surface cooling factor, W/m2 UNFRC fenestration U-factor, W/(m2C) PXI peak exterior irradiance, W/m2 SHGC solar heat gain coefficient IAC interior shading attenuation coefficient FFs fenestration solar load factor Et, Eb, ED peak total, diffuse, and direct irradiance, W/m2 Tx transmission of the exterior attachment Fshd fraction of the fenestration shaded by overhangs or fins L site latitude, N SLF shade line factor Doh depth of the overhang, m Xoh vertical distance from the top of the fenestration to the overhang, m Fcl shade fraction closed (0e1) j exposure (surface azimuth), measured as degrees from south V; volumetric flow rate, L/s DF infiltration driving force, L/(s cm2 ) thermal resistance, C/W Noc number of occupants Nbr number of bedrooms aroof roof solar absorbance t time constant, s I infiltration coefficient Du indooreoutdoor humidity ratio difference, kgw/kgda Subscripts m air in mixing box r room/return o outside os outside supply i inside He heat exchanger a air w water aHe air in the heat exchanger L leakage Win water input Wout water output Wl wall room inside room out outside room g glass fg heat of vaporization Opq opaque inf infiltration fen fenestration f indoor and outdoor t at time t flue flue effective es exposed ul unit leakage ig internal gains l latent s sensible/supply fur furniture cl closed R.Z. Homod / Energy 74 (2014) 762e774 763
  • 3. It is possible to solve a problem in which the variables of tem- perature and relative humidity are coupled. The first modification in AHUs is the addition of a fresh air pre-cooling coil that is used to alleviate the coupling intensity, which is particularly necessary in humid climates. The second modification for control objectives is the increase of the optimisation parameters of the output controller by adding a model of the PMV index in order to evaluate indoor thermal comfort. Next, decoupling and reduction in energy are simulated by comparing three different systems under real weather conditions within certain set point comfort limits. The first system is a con- ventional system in which the objective is to achieve the tempera- ture and relative humidity that are within the limits of the desired conditions. The second system is similar to the first, with the only difference being the addition of a reheating coil and a wet main cooling coil in AHUs that are used to solve the coupling problem. However, these additional reheating and wet main cooling coils double the energy consumption of the unit due to the addition of two processes: an implemented sub-cooling process that reduces the RH and reheating the supplied air in order to meet the desired levels of thermal comfort. The third system is the same as the first, but it has an additional pre-cooling coil and controller objective where a PMV model is added to facilitate the controller optimisation for four outputs (i.e., the dry bulb temperature, the radiant temperature, the relative air velocity and the relative humidity for an indoor condi- tioned space). Controller (TSKFIS (TakagieSugenoeKang fuzzy inference system)) optimisation is achieved by manipulating the five AHU inputs (control outputs), which are in the form of the flow rate of chilled water for the pre-cooling coil and the main cooling coil, the flow rate of the supply air (fresh air and return air) and the fan speed of the supply air. Additionally, the PMV model strategy does not require the use of a reheating coil for decoupling purposes. The main contribution of this paper is to address the coupling problem, which arises in the hot and humid climatic region of South Iraq, by modifying the AHU and applying the algorithm of the adaptive multi-variable control TSKFF (the Takagi-SugenoeKang fuzzy forward). 2. Control system design The present paper attempts to address the shortfall on energy savings and decoupling for buildings with HVAC control systems in the hot and humid climatic region of Iraq. Careful assessments in simulated environments are considered. The PMV model is added to enable controller decoupling of temperature and RH. Increasing manipulation parameters are used to compensate for any bounded variations that may arise due to the limitation of the dampers range. This is considered as a limitation because the HVAC control systems have set upper and lower control limits for the dampers range in order to maintain ventilation for acceptable indoor air quality, according to the ANSI/ASHRAE 62 standard [24]. 2.1. TSKFF controller The industry standard PID controller exhibits the inability to control the objectives of the HVAC system that have inherently adverse characteristics, such as a nonlinear, large-scale system with a large thermal inertia, a pure lag time, constraints and factors of uncertain disturbances. Additionally, the indoor thermal comfort must be decoupled from the temperature and relative humidity. Hence, fuzzy logic controllers are used due to their flexibility and intuitive use [25] in controlling the aforementioned characteristics. 2.1.1. Basic description of the control system The most important motivation for adopting this type of controller is due to it being able to treat multi-controlled variables because it converts a TSKFIS (TakagieSugenoeKang fuzzy inference system) model into a memory layers parameters (TKS) model. The output routine of the classical TSKFIS model requires numerical and logical operation tasks, and these tasks take a long time to be completed. However, the TSK model uses the gradient algorithm, which is a faster online tuning method that requires less mathe- matical manipulations than other traditional methods, such as the backpropagation method for neural networks. The most important aspect of online tuning is that it can tune a multivariable controller with multiple outputs; this tuner can improve the controller's ability to deal with MIMO models that possess a large-scale nonlinear aspect, are heavily coupled, have a pure lag time, contain large thermal inertia, possess uncertain disturbance factors and have constraints, which are common properties in HVAC sys- tems. For the purpose of this study, each strategy of the control structure is developed by upgraded layers of memory in order to coordinate the modification of AHUs, which follows a change in the online tuning system. 2.1.2. Model identification architecture The main concept of the TSKFF (Takagi-SugenoeKang fuzzy forward) structure is based on obtaining the consequent parame- ters by mapping them from the antecedent space to the consequent space. The obtained parameters of the consequent space are organised as layers in the memory space. The parameters in these layers function to the inputs of the model. These inputs calculate the outputs' data set, which can be clustered into seven groups within a time frame of 24 h, where each cluster for each output is repre- sented by TSK rules. The outputs Yj(X) must fit the data set. This can be achieved by modulating the nonlinear equation for each output yi. The modulation can be attained by tuning the parameters ai and bi. The offline tuning method is performed by using the GNMNR (GausseNewton Method for the Nonlinear Regression) algorithm, which has the capability to express the knowledge that is acquired from inputeoutput data in the form of layers of parameters. The Equation of the final model's outputs is characterised by aggre- gating the clusters' outputs and obtaining the singleton fuzzy model, which belongs to a general class of the universal model output. Subsequently, the outputs Yj(X) can be obtained as follows: Yj ðX Þ ¼ XN i uiai 1 À eÀbix (1) where X ¼ [x1, x2 … xm]T is the input variables vector, i is a rule number subscript, ai and bi are the Tagaki-SugenoeKang parame- ters functions, ui is the basis function (weight), and j is the cluster number subscript. The TSK model can be structured in layers f (x; ai bi) and the weights framework that is shown in Fig. 1 where f (x; ai bi) is a nonlinear function of the TSK parameters and the independent variable x. The TSKFF is modelled by collecting training data from the building and the HVAC system equipment. Learning of the pa- rameters in the TSKFF model is accomplished by the offline GNMNR algorithm. One of the advantages that the GNMNR algorithm offers is the real-time implementation of computational cost reduction. This is possible because the proposed method requires a lower number of iterations to perform the learning/training procedure; therefore, the tuning time will be reduced when it is implemented in real-time [5]. The controller method is realised by the TSKFF feed forward model to increase the response and time steady state control for the HVAC system. Additionally, the feed forward model is tuned online by using the gradient algorithm to enhance the stability and to reject the disturbances and uncertain factors. By using the gradient algorithm, a faster online tuning method is R.Z. Homod / Energy 74 (2014) 762e774764
  • 4. found that requires less mathematical manipulations than other methods do, such as the backpropagation method for neural net- works. The most important aspect of this online tuning is that it can tune a multivariable controller with multiple outputs [11]. 2.2. Decoupling problem and objectives' setting The cooling coils in AHUs are categorised into dry and wet types. The temperature and relative humidity of air that is introduced to the AHU that has a dry cooling coil are characterised by coupling loops due to the constant air humidity ratio. Once the temperature is decreased, the relative humidity will be increased and vice versa. The thermal comfort can be controlled through the PMV index by using this type of AHU, with either air temperature or air relative humidity being a control variable (but not with both being control variables at the same time). The rest of the PMV variables are considered to be disturbances. It is desirable to control temperature and relative humidity independently and accurately in certain in- door conditions. In these cases, the AHU with a wet cooling coil is used; both temperature and RH are varied independently based on the flow rates of air and chilled water. It is impossible to set one variable without affecting the other when the design of the AHU does not take into account the coupling dynamics between these variables; therefore, the importance of decoupling techniques that are used to implement an appropriate AHU is realised. The proposed strategy is implementing a twin cooling coil AHU and an advanced multi-variable control system. The pre-cooling coil (wet) is equipped to cool and dehumidify the fresh air intake. The main cooling coil (dry) is used to cool the supply air. The deeply chilled water is only necessary for (pre-cooling coil) removing the moisture from the fresh air. The main cooling coil requires moderately cool water, according to the building load. This type of order helps in save energy for buildings with HVAC systems because higher chilled water temperatures indicate better COPs (coefficients of performance). Furthermore, the use of the PMV index (the indoor air temperature, the radiant temperature, the relative air velocity and the relative humidity for an indoor condi- tion space) as a desired objective enables the control system to optimise the input plant by controlling air velocity and manipu- lating the flow rate of fresh air in regard to thermal comfort levels. The main difference between the proposed strategy and the other two strategies is in their control objectives of the operating system and AHU equipment. The AHU for the conventional strategy is similar to what it is for proposed strategy, but there are two differences: first, it does not contain a pre-cooling coil, and second, the controlled variables include two variables that have restricted values. These variables are temperature and relative humidity; both of them are set at desired specific values. The objective of this control strategy acts as a control reference of the online tuning that reflected negatively on its performance due to stiff references and a limited number of input plant variables that are used for optimi- sation. The controlled variables for the third (adding the reheating coil) strategy are similar to those of the conventional strategy, but the difference is that the AHU is equipped with a wet main cooling coil and a reheating coil to consolidate the controller for the decoupling problem. The objectives of this paper are to: 1. Assess the feasibility of using the proposed strategy in a South Iraq climate 2. Characterise the energy savings and decoupling of the proposed system 3. Test the potential of the controller for multi-objective optimi- sation in the HVAC system. These aims will be achieved by comparing three scenarios of the AHU control system in order to assess the decoupling problem and energy savings of the simulated HVAC system. 3. Analysis of energy and mass flows of a building The purpose of the control strategy is to minimise the total power consumption of the HVAC system by optimising the vari- ables of the indoor thermal comfort (i.e., the indoor air tempera- ture, the radiant temperature, the relative air velocity and the relative humidity for the indoor condition space). Generally, the electric power consumption of the HVAC system is a function of the COP (coefficient of performance) of the chillers, the EER (energy efficiency ratio) of the building and the cooling load of the building. The EER and COP are constants for a specified building and chiller, respectively, whereas the total cooling loads of the building vary, depending on the disturbances and the controllable variables. Therefore, the total electric power consumption can be summarised by Equation (2) [26,27]: EP ¼ XN i chli copi þ EPAHU ¼ TBCL EER (2) where EP is the total electric power consumption, N is the number of chillers, chl is the chiller power, EPAHU is the electric power that is consumed by AHU, and TBCL is the total building's cooling load. From Equation (2), it can clearly be observed that the EP can be derived by using two different methods that are based on the energy and mass balance equations of the building's fabric (the right term of Equation (2)) and of the AHU subsystems' equipment (the middle term of Equation (2)). Therefore, the theories regarding the conservation of energy and mass are applied to thermally analyse and model the overall behaviour of an HVAC system. These theories are based on the fact that in the control volume of any subsystem, energy is transferred from/to a sub- system by two types of processes: mass transfer and conventional Fig. 1. Schematic diagram of the TSK model as layers of memory. R.Z. Homod / Energy 74 (2014) 762e774 765
  • 5. heat transfer (conduction, convection and radiation). These pro- cesses are dominant in HVAC systems. In this research study, the system is subdivided into the building's and the AHU's control volumes. The building's energy and mass transfer can be demon- strated by Fig. 2. To evaluate the sensible heat gain of the building, the following thermal balance equation is applied to the building's control volume: The term on the left side of Equation (3) denotes the output of the AHU, which represents the heat and mass that is transferred to the building's control volume. On the right side of Equation (3), the first part (the accumulation or storage of energy) represents the thermal mass that is stored in the inner wall, indoor air and furniture, while the second part (the difference between the input and output of energy) represents other inputs/outputs to the con- trol volume of the building. The latent heat gain of the building is related to the moisture transfer, which can be evaluated by applying the conservation of time-dependent mass law to the control volume of the building, which is shown in Equation (4); The term on the left side of Equation (4) is the rate of moisture that is absorbed by the AHU. On the right side of Equation (4), the first part (the rate of moisture change) is the change in the rate of air moisture in the building at time interval dt, and the other terms are related to the indoor input/output and the generated moisture. To evaluate the sensible and latent heat gains of the building, it is necessary to calculate the left-hand sides of Equations (3) and (4), which can be obtained by applying the laws of conservation of energy and mass to the control volume of the AHU. The AHU is subdivided into three subsystems: the mixing air chamber, the pre-cooling coil and the main cooling coil. Energy is only consumed in the pre-cooling and main coolingcoils,socalculations for the energyand mass control volumes are applied on these two subsystems, as follows: The term “energy absorbed by the coil” in Equation (5) refers to the sensible and latent heat load that is exerted by the pre-cooling coil. On the right side of the equation, the first term (energy accumulation in the metal mass of the coil) refers to the rate of change for the heat storage in the coil mass, while the second term (the sensible energy delivered by air) refers to the sensible cooling load of the fresh air, and the third term (the latent energy delivered by moisture withdrawal) refers to the latent energy that is absorbed by the coil due to the condensation of moisture. The third term on the right side of Equation (5) can be evaluated by applying the law of mass conservation to the air flow stream that is used for the pre- cooling coil. The following is obtained: By using the same procedure as was used for the pre-cooling coil to obtain the sensible and latent heating loads for the dynamic subsystem equations, the main cooling coil can be written mathe- matically by using the time-dependent equation of the control volume, as follows: _Qs z}|{ Cooling load ¼ _Qair þ _Qfur zfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflffl{Accumulation or storage of energy þ _Qopq þ _Qfen þ _Qslab þ _Qinf þ _Qig;s zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ Difference between input and output of energy (3) _ms À ur;t À us;t Ázfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflffl{ rate of moisture withdrawal by AHU ¼ dMrur;t dt zfflfflfflffl}|fflfflfflffl{ rate of moisture change þ _Qig;l hfg zffl}|ffl{ rate of moisture generation þ _minf uo;t À _mrur;t zfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflffl{ rate of moisture transfer (4) _mw;tcpw À Two;t À Twin;t Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ energy absorbed by the coil ¼ MHecpHe dTh;t dt zfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflffl{ energy accumulation in the metal mass of coil þ _mo;tcpa À To;t À Tos;t Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ sensible energy delivered by air þ _mo;t uo;t À uos;t hfg zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ latent energy delivered by air dehumidification (6) _mw;tcpw À Two;t À Twin;t Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ energy absorbed by the coil ¼ MHecpHe dTh;t dt zfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflffl{ energy accumulation in the metal mass of coil þ _mo;tcpa À To;t À Tos;t Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ sensible energy delivered by air þ _mcon:;thfg zfflfflfflfflfflffl}|fflfflfflfflfflffl{ latent energy delivered by moisture withdrawal (5) R.Z. Homod / Energy 74 (2014) 762e774766
  • 6. The rate of thermal energy transfer (the sensible cooling load) from the building by the mechanical ventilation air flow (Qvent) is calculated by using Equation (8). _Qvent ¼ _ms;tcpa Tr;t À Ts;t (8) The power of the air supply system in the mechanical ventila- tion state (the transmission power) is mainly from the power supply for the fan, which can be calculated by the application of the law of conservation of energy on the control volume of the AHU. This equation can be calculated as follows [27]: _Qfan ¼ _ms;tcpa Ts;t À To;t (9) According to the energy balance for the indoor conditioned space of Equation (3), the values of thermal energy flow from (1) opaque-surfaces, (2) transparent fenestration surfaces, (3) infiltra- tion, (4) indoor load and (5) ventilation are calculated by using the steady state conditions of Equation (3), whereby all of the thermal energy flow values are equal to the cooling load that is extracted by the HVAC systems or the mechanical ventilation, which equals the left-hand side of Equation (3); in turn, Equation (3) can be calcu- lated by summing Equations (6)e(9). The instantaneous cooling load of the building can be obtained from the simulation process after modelling the HVAC system. Additionally, the instantaneous cooling loads of the building directly impact the outputs of the controller signals. Therefore, the method of calculation that is employed in this research study is based on the output signals of the controller. The output signals of the controller manipulate the valves of the pre-cooling coil, the main cooling coil, the reheating coil and the dampers of the return and fresh air to track the objective of the HVAC system. The valves and dampers are designed according to the heating/cooling load of the building. The opening position of the valves and dampers is recorded as a percentage of the fullest extent (as shown in Fig. 3) that represents the main cooling coil valve's opening position over 24 h. The percentage of the opening position is related to the maximum flow rate of the valves and dampers. This signal opening position is implemented in Matlab to obtain the energy con- sumption of the HVAC system. The advantage of using Matlab/Simulink is in the ability to use a graphical programming language that is based on different block categories with different properties of each block. Matlab and its Fig. 3. The control signal percentage for the main cooling coil's chilled water valve for each of the three strategies. Fig. 2. Representation of building energy and mass transfer for prototypical buildings with HVAC systems. _mmw;tcpw À Two;t À Twin;t Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ energy absorbed by the coil ¼ MmHecpHe dTh;t dt zfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflffl{ energy accumulation in the metal mass of coil þ _mm;tcpa À Tm;t À Ts;t Ázfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ sensible energy delivered by air þ _mm;t um;t À us;t hfg zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl}|fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{ latent energy delivered by air dehumidification (7) R.Z. Homod / Energy 74 (2014) 762e774 767
  • 7. toolboxes are adopted to perform all of the identification processes and simulations in this work, as well as in our previous works [28e31]. System identification and control system toolboxes were used to identify and build the model, while the fuzzy logic toolbox was used for the TSK model identification. The obtained models are then introduced in the Matlab/Simulink environment for simula- tion and analysis. These categories include the input/output, transfer functions, arithmetic functions, state space models and data handling. The building model is represented in the form of ODE (ordinary differential equation) solvers, which are automati- cally configured during the Simulink model's run-time. The algo- rithm of the controller is designed by using Matlab m-files, parameter layer memory and S-functions, which are based on on- line parameter tuning. The technique for calculating the cooling loads is easily implementable, whereby the thermal balance equation is derived from the arithmetic functions, from which the energy consumption can be obtained. 4. Simulation results and discussion 4.1. Physical and theoretical model description The simulated building model is a typical one-story house with a simple structure. The house consists of heavyweight construction (brick and concrete) that measures 4.5 m in height, with 248.6 m2 of gross ground floor area. The net floor area of the entire building is 195.3 m2 , excluding the garage area; the gross exposed area of the windows and wall is 126.2 m2 , while the net area of the exterior wall is 108.5 m2 . The overall volume of the house, excluding the garage and suspended ceiling space, is 781.2 m3 Table 1 shows the physical properties of the components of the building. The dry bulb temperature varies according to the spring season's climate in Basrah city, which ranges from 18 C to 32 C, and the humidity ratio varies from 0.01 to 0.01909 kg of moisture per kg of dry air. The building model's transfer function and the PMV, or thermal comfort sensor model, are presented in Appendices A and B [32,33]. To reduce the design cost, as well as the cost that is needed to fabricate the three HVAC systems, simulation methods are imple- mented in order to test and analyse the results. The identification approach of the model demonstration is based on the multi-zone model of the RLF (residential load factor) method. The identified model is simulated by three different controller strategies in order to study their levels of indoor thermal comfort and energy con- sumption. The first system is a conventional control system (the control variable objectives are temperature and relative humidity). The second is a conventional system that includes the addition of a reheating coil and a wet main cooling coil, while the third system is similar to the first system, but it includes an addition of a pre- cooling coil and a PMV index in order to measure the objective of the controller. The three types of systems are run together in order to study their performance and energy consumption (as shown by the simulation block diagram in Fig. 4, which presents the simu- lation in the evaluation of performance and energy consumption of the three systems). Fig. 4. Matlab blocks for the simulations of all three systems. Table 1 Properties of the materials used for construction of the model. Component Description Factors Roof/ceiling Flat wood frame ceiling (insulated with R-5.3 fiberglass) beneath vented attic with medium asphalt shingle roof U ¼ 0.031 18 W=ðm2KÞ a roof ¼ 0.85 Exterior walls Wood frame, exterior wood sheathing, interior gypsum board, R-2.3 fiberglass insulation U ¼ 51 W=ðm2KÞ Doors Wood, solid core U ¼ 2.3 W=ðm2KÞ Floor Slab on grade with heavy carpet over rubber pad; R-0.9 edge insulation to 1 m below grade Rcvr ¼ 0.21 W=ðm2KÞ; Fp ¼ 85 W=ðm2KÞ Windows Clear double-pane glass in wood frames. Half fixed, half operable with insect screens (except living room picture window, which is fixed). 0.6 m eave overhang on east and west with eave edge at same height as top of glazing for all windows. Allow for typical interior shading, half closed. Fixed: U ¼ 2.84 W=ðm2KÞ; SHGC ¼ 0.67. Operable: U ¼ 2.87 W=ðm2KÞ; SHGC ¼ 0.57; Tx ¼ 0.64; IACcl ¼ 0.6 Construction Good Aul ¼ 1.4 cm2 /m2 R.Z. Homod / Energy 74 (2014) 762e774768
  • 8. The mean radiant temperature is a more complicated quantity that depends on the temperature of the surrounding surfaces, as well as on angle factors of the surrounding surfaces. Therefore, the plant model leads to the output of the plug-in model of the PMV index, except the mean radiant temperature requires an interme- diate sub-model where its output is taken into account because it is one of the main factors that affects thermal comfort. This sub- model estimates the mean radiant temperature by using two methods: theoretical and numerical. For the theoretical method, the mean radiant temperature is estimated from the measured temperature of the surrounding walls and surfaces and the angle factors of these surrounding surfaces. All of the indoor surfaces are assumed to be black because most building materials have a high emittance ε, and it is assumed that small temperature differences exist between the surfaces of the enclosure (i.e., linear combination of system states). Therefore, the following equation is used [34]: MRT ¼ T1FPÀ1 þ T2FPÀ2 þ / þ TnFPÀn (10) where MRT is the Mean Radiant Temperature, Tn is the temperature of surface ‘n’ and Fp-n is the angle factor between a person and surface ‘n’. For the numerical estimation, a black-globe thermometer sensor is used. 4.2. Decoupling results and discussion The plant model is dynamically subjected by many thermal disturbance factors, such as the K2 solar radiation, f4 inside sensible, FDR fenestration, etc. Three simulation sets are conducted over 24 h and include nominal, noise and sensor deterioration, as well as an uncertainty operation, for the three systems' behaviours to be observed and studied for the different conditions. The main objective of this work is to validate the decoupling of the proposed strategy. 4.2.1. Nominal operating conditions Pre-cooling coils are added to the proposed AHU of the HVAC system in order to economically control the indoor relative hu- midity in a humid climate. Additionally, the proposed system has four control variables for an indoor conditioned space (i.e., the indoor-air temperature, the indoor-air velocity, the indoor-air hu- midity and the flow rate of fresh air). These control variables are optimised by the controller to provide economical indoor-air Fig. 5. PMV comparisons of the results of the three different systems with different objectives and designs. Fig. 6. Indoor temperature comparisons of the results between the three different systems with different objectives and designs. R.Z. Homod / Energy 74 (2014) 762e774 769
  • 9. conditioning that yields the desired level of thermal comfort and indoor air quality, according to ASHRAE and ISO standards; this also reduces the cooling load during implementation in real-time. The other systems have two control objectives that are set at certain desired values for the indoor conditioned space (i.e., the indoor-air temperature and the indoor-air humidity). Fig. 4 shows the three designs of the HVAC system. The manipulation of each TSKFF for the five AHU inputs in the three designs of the HVAC system be- haves differently. In the proposed system, the input feedback sensor allows some degree of tolerance instead of requiring a specific value for the temperature and relative humidity, which is needed in the conventional HVAC systems. This optimisation overcomes the coupling effects (temperature and relative humidi- ty) perfectly by providing the desired level of thermal comfort, which is shown in Fig. 5. In regard to Fig. 5, it can be observed that the proposed (the model of the PMV index addition) system can track the desired objective and can achieve outstanding perfor- mance, while the system with the added reheating coil acts within an acceptable thermal comfort range that has an acceptable offset from the set point. The conventional system was found to violate the ASHRAE Standard 55-92 [35] and ISO-7730 [36] for the desired level of indoor thermal comfort. These standards recommend that the acceptable levels of thermal comfort are limited to a range between À0.5 PMV 0.5. It is evident that this violation is caused by the coupling of temperature and relative humidity. The tem- perature curves of all three systems are similar to the PMV trend that is shown in the simulation results, which are tabulated in Fig. 6. The periodic effect of the coupling factors is apparent from 05:30 o'clock to 08:00 o'clock and from 19:00 o'clock to 24:00 o'clock. The effect can be more clearly observed in the behaviour of the relative humidity (as shown in Fig. 7), in which the conven- tional system fluctuates within a wide range, whereas the other systems remain in the range of approximately 50% RH. The rec- ommended range of RH, according to the ASHRAE Standard 55-92 and ISO-7730 for the indoor comfort condition, is 40%e60%. High humidity not only causes poor indoor air quality, but it also causes wood decay, metal corrosion and structural deterioration [37]. The calculations of energy consumption are based on the controller Fig. 7. Indoor relative humidity comparisons of the results between the three different systems with different objectives and designs. Fig. 8. PMV comparisons of the results of the three different systems based on the operating conditions of noise and sensor deterioration. R.Z. Homod / Energy 74 (2014) 762e774770
  • 10. signals. One of these signals is shown in Fig. 3. Fig. 3 shows the results of the simulation of the control signal variation for the main cooling coil of the chilled water valve, with respect to time. In Fig. 3, the signals for the conventional system with a reheating coil acts similar to a BangeBang control action. The modulating valve continuously fluctuates between ON-OFF, which will eventually wear out the valve and shorten its lifespan. It can be clearly observed that the proposed system signal works very efficiently, which provides good control performance. Figs. 5e7 show the transient response for the initial condition. This took approximately an hour because the plant model is dynamically affected by the thermal mass of the building structure and slab floors, which cre- ates a flywheel effect. The influence of this flywheel effect begins to fade and becomes less intense after the HVAC system starts, which can clearly be observed in the signal of valve open position in Fig. 3. 4.2.2. Operating conditions of noise and sensor deterioration Disturbance mode has tested decoupling through its validation of the rejection of noise and sensor deterioration. In noise and sensor deterioration, the controlled process parameters, sensors' gains, and noise signals are able to change in the same manner for each system and simulation that is conducted. Here, we suppose that sensors deteriorate with 20% fault, and the sensors' gain is changed to 0.8 (sensor gain ¼ 1 when the sensor performance is 100%). Additionally, to test the sensitivity of the proposed method to noise, each system is subjected to the same noisy environment by adding a 10% NSR (noise-to-signal ratio), which refers to the ratio of the continuous noise signal to the controlled signal. The sensor deterioration set and subjected noise signal are applied at the start of the simulation. Fig. 8 shows the three different systems to try to track a PMV set point, which changes under a square wave from À0.4, 0 and 0.4 during a 24 h time frame. By using this test, one can clearly observe the three systems' behaviour for the PMV, where the proposed system provides superior control performance and does not violate the ASHRAE 55-92 and ISO-7730 Standards. In contrast, the other systems exhibited deterioration in their per- formances and, consequently, violated the Standards of the indoor thermal comfort. Thus, the proposed system achieves significant results that verify the use of decoupling parameters rather than adding a reheating coil or using conventional decoupling methods, Fig. 9. PMV comparisons of the results of the three different systems in regard to the operating conditions when model uncertainties are present. Fig. 10. Psychometric chart comparisons of the results of the three different systems in regard to the operating conditions when model uncertainties are present. R.Z. Homod / Energy 74 (2014) 762e774 771
  • 11. which are extremely intricate and too impractical to solve numer- ically when the plant system model is complicated, which is the case for HVAC systems. 4.2.3. Operating conditions regarding the presence of model uncertainties In regard to robustness validation, the plant model encompasses a wide range of operating parameters, which vary as the HVAC systems undergo fluctuating loads due to changes in external dis- turbances during a typical day's operation. Therefore, in the pres- ence of uncertainties regarding the modelling of such parameters, it becomes necessary to use a robust intelligent controller, such as TSKFF, to obtain efficient operation in the HVAC systems. To vali- date the robustness of the TSKFF controller, the building heat loss coefficients, the heat transfer coefficients of the fan-coil units and pumps and the thermal time constant are changed. Before a simulation run begins, all of the model coefficients and the time constant are increased by 20%. Three TSK models of controllers are tuned based on the nominal plant model and then are integrated into a control algorithm that manipulates AHU parameters to control indoor thermal comfort. The conventional strategy leads to the worst indoor ambient conditions and becomes less intense after adding a reheating coil, which is shown in Fig. 9. However, both strategies violate the standard limitation of ASHRAE 55-92 and ISO- 7730. The proposed scheme maintains asymptotic tracking of a given reference signal, and it occurs in the presence of the same parameter variations and model uncertainties when it does not use reheating and wet main cooling coils. For validation, psychometric charts are the most commonly used tool for indoor studies and outdoor air conditions. Fig. 10 describes the air states cycle of physical and thermodynamic properties for indoor conditions over 24 h. The proposed strategy seems to satisfy the TCZ (thermal comfort zone), whereas the other strategies frequently crossover TCZ. 4.3. Energy saving results and discussion The purpose of the model of the PMV index addition to the proposed system is to change the restricted conventional objective variables (temperature and relative humidity) of an HVAC system in Fig. 11. A comparison of the energy consumption results based on the cooling coil load variation between the three different schemes. Fig. 12. A comparison of the results of the power consumption between the three different system schemes. R.Z. Homod / Energy 74 (2014) 762e774772
  • 12. addition to increasing its flexibility with respect to the indoor control parameters (temperature, fresh air flow rate, indoor air velocity and relative humidity). The model of the PMV index addition also enables the controller to improve its performance. The TSKFF controller exploits the flexibility of the control param- eters by optimising the parameters through the manipulation of the AHU parameters (inputs) to provide the desired levels of ther- mal comfort, while simultaneously reducing the energy con- sumption of the HVAC system. Furthermore, the velocity of indoor air can reduce the cooling load. This can be observed from the simulation results of the energy that is consumed by the cooling coil load, which is shown in Fig. 11. The simulation techniques that are used to calculate the cooling loads are straight forward: thermal balance equations are imple- mented by using arithmetic functions, and then the consumed energy can be obtained by using Equations (6)e(9). The simulation results of the consumed energy in the system with a reheating coil reveal higher energy consumption than the consumption of the other systems because the cooling process reduces the air tem- perature to the sub-cooling state before the reheating process overcomes the coupling effect and meets the demands of indoor thermal comfort. Although the conventional system is better in terms of energy savings than the system that has the addition of a reheating coil, the conventional system does not meet the desired level of indoor thermal comfort. However, the proposed system shows more favourable results than the other two systems with respect to achieving the desired level of thermal comfort and reducing energy consumption, simultaneously. Based on Fig. 11, it can be observed that the differences in energy consumption among the three sys- tems increase during the times periods that include the presence of a coupling effect. The average power consumption for the three different systems (the conventional system, the addition of a reheating system and the proposed system) are 10.713 kW, 13.27 kW and 9.016 kW, respectively. The average power costs that accompany the addition of a reheating system are 1.4718 times higher than that of the proposed system. Based on the data for 24 h of power consumption, the calculations for energy consumption for each of the three strategies show that energy consumption in the proposed strategy is 32.06% lower than the system with an added reheating coil, which is shown in Fig.12. This result closely matches the results that were obtained by Yang and Su [38] in which an intelligent controller was developed to adjust the PMV index, which led to saving approximately 30% more of the energy con- sumption than the conventional methods. Furthermore, the simu- lation of the cooling coil load output is compared to the numerical results, which are based on the CLF/CLTDC (the cooling load factor for the glass/corrected cooling load temperature difference) method [39,40]. The calculation considers the effects of numerous outdoor environmental parameters on the indoor thermal loads. The cooling load of the building is calculated every 30 min to obtain the absolute margin of error between the simulation results (the proposed system) and the numerical calculation, which was found to vary between 0.064 and 0.107 kW. To have a clearer assessment of the error between the simulation and numerical calculations of the cooling coil load output, in this study, the statistical index of the coefficient of determination (r2 ) was calculated based on Equation (11) and had a value of r2 ¼ 0.974. r2 ¼ ½N P yiyi À ð P yiÞð P yiÞŠ2 h N P y2 i À ð P yiÞ2 N P y2 i À ð P yiÞ2 i (11) where yi is the numerical result, yi is the simulation result, and N is the number of test samples. 5. Conclusion In this context, the simulation results of the comparison inves- tigated the use of a PMV model input as an objective optimisation of controller decoupling and of reductions in the energy consumed by an HVAC system. This was performed by considering all of the factors that are affected by indoor thermal comfort, which are re- flected by the PMV index. The control system that is proposed in this work includes, as part of its structure, a PMV model for the optimisation of the deviations in the parameters of indoor thermal comfort and of the generation of control actions that pertain to the AHU inputs. The task regarding the PMV index output is, therefore, to acquire controller output signals more accurately by exploiting the decision algorithm's flexibility for the PMV index input's ag- gregation. The weather in Basrah, a southern city of Iraq, was considered as a case study to test the system. The output controller signals were adopted to obtain the energy consumption for three different control objectives and strategies, which were evaluated with respect to typical and modified HVAC systems. Based on the results of the performed simulations, we can conclude that when using the indoor PMV as a variable objective for the HVAC system, the controller performs better and provides more energy savings, while still attaining the desired level of indoor thermal comfort. The multi-input of the AHU is manipulated by the TSKFF controller, which is characterised by the optimisation of the outputs for energy savings. Both the conventional and proposed systems show that energy is saved in comparison to the system that has an additional reheating coil in the AHU. The conventional HVAC system shows a savings of up to 19% of energy usage, which is 61.5 kWh/d less than the energy that is used by an HVAC system that has an additional reheating coil; in contrast, the proposed strategy can save up to 32.06% of energy usage, which is 102.1 kWh/d less than the energy that is used by the HVAC system that has an additional reheating coil. This is because a TSKFF that is equipped with a model of PMV index reduces the energy consumption of a building by as much as it can by utilising the outdoor climate in controlling the rate of fresh air flow. Meanwhile, the conventional control strategy adjusts the temperature and relative humidity to a predefined strict set point, which does not allow for optimisation of energy consumption for indoor thermal comfort. An important finding of this study is that the proposed strategy economically addressed the coupling prob- lem in addition to providing the desired level of thermal comfort. Furthermore, the procedure of using the PMV model and TSKFF is straightforward and easy to implement. Appendix A. Supplementary data Supplementary data related to this article can be found at http:// dx.doi.org/10.1016/j.energy.2014.07.047. References [1] Anastaselos D, Theodoridou I, Papadopoulos AM, Hegger M. Integrated eval- uation of radiative heating systems for residential buildings. 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