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—
1a
Notes Notes
1–1aPage 1a1–1bPage Chapter 1 – Introduction to Psychrometry
Learning Outcomes
Learning Outcomes:
When you have studied this chapter you should be able to:
1 Explain what is meant by the term ‘Psychrometry’.
2. Relate ‘Dalton’s law of Partial Pressures’ to the term
‘Atmospheric Pressure’.
3. Explain what is meant by the term ‘Saturated Vapour
Pressure’.
4. Use a ‘Psychrometric Chart to find:
a. A saturated vapour pressure for a given
temperature.
Find, for a given air sample, the following:
b. The moisture content
c. The percentage saturation
d. The relative humidity.
5. Explain what is meant by the ‘wet-bulb’ temperature and
its use in the ‘psychrometric equation’.
6. Show how the Psychrometric Chart is used to determine:
a. Dew-point temperature
b. Specific Enthalpy
Suggested StudyTime:
(a) For study of chapter material;
(i) Initial on-screen study 1 hour
(ii) Printing of notes and subsequent
in-depth study 2 hours
(b) For completion of the quick revision study guide
½ hour
Total estimated study time 3½ hours
Introduction
to
Psychrometry
Chapter 1
Chapter 1
Introduction to
Psychrometry
—
2a
Notes Notes
1–2aPage 2a1–2bPage Chapter 1 – Introduction to Psychrometry
Chapter Contents
Item page
Learning Outcomes 1-1b
Introduction to Psychrometry 1-3a
The Atmosphere 1-3a
Water Vapour 1-4a
Saturated Vapour Pressure 1-5a
Psychrometric Chart (Theory) 1-5b
Moisture content 1-6a
Relative humidity 1-6b
Percentage saturation 1-7a
Relationship between g, m and rh 1-7b
Comparision of percentage saturation & rh 1-8a
Wet-bulb temperature 1-8b
1. The Sling Wet-bulb 1-8b
2. The Screen Wet-bulb 1-8b
The Psychrometric Equation 1-9a
Dew-point temperature 1-10b
Specific enthalpy 1-11a
Specific volume 1-12a
Density 1-12a
Psychrometric chart 1-13
Quick Revision Study Guide 1-14a
Chapter Notes 1-15a
—
3a
Notes Notes
1–3aPage 3a1–3bPage Chapter 1 – Introduction to Psychrometry
Introduction to Psychrometry
The Atmosphere
Psychrometry is the study of atmospheric air and its asso-
ciated water vapour. Air comprises a mixture of gases†1.1
of which
nitrogen makes up 78%, oxygen 21% and carbon dioxide and
the inert gases (such as argon, neon, krypton, helium etc.) the
remainder. These are known as the dry gases of the atmosphere.
Principle Dry Atmospheric Gases
VIDEOEO
See
Notes
Gas A at
partial pressure
PA
Gas B at
partial pressure
Pb
Gas A + B at
total pressure
PA
+ PB
Dalton’s Law, illustrates that if two gases are combined
into the same volume, the total pressure is the sum of the
individual partial gas pressures.
In a vessel open to the
atmosphere, it is the weight
of the atmospheric gases
above the earth’s surface
that produce the pressure†1.2
of the atmosphere.
- 1200˚C
- 1200˚C
- 1150˚C
- 1100˚C
- 900˚C
- 200˚C
- 75˚C
- 60˚C
- 60˚C
+ 20˚C
400km
350km
300km
250km
200km
150km
100km
50kmSTRATOSPHERE
TROPOPAUSE
TROPOSPHERE
IONOSPHERE
Clouds,
Winds
No Clouds,
No Winds
ApproximateTemperature
Height
The Earth’s Atmosphere
See
Notes
In the air mixture, the dry gases and associated water va-
pour behave according to ‘Dalton’s law of Partial Pressures’. That
is they behave independently of one another and the pressure each
exerts combine to produce an overall ‘atmospheric pressure’.
0
10
20
30
40
50
60
70
80
Nitrogen Oxygen Carbon Dioxide
MolecularWeight %Atmosphere
—
4a
Notes Notes
1–4aPage 4a1–4bPage Chapter 1 – Introduction to Psychrometry
Since at normal temperatures and pressures we are unable
to condense these gases out from the atmosphere, for the purpose
of psychrometry, this mixture of gases can be treated as if it were
a single ‘ideal’ or perfect gas behaving as a single element known
as ‘dry air’.
Note: Psychrometry is a specialised area of thermodynam-
ics but obviosuly has applications in air conditioning. None the
less, in order to fully appreciate the material within this course
you need to be familiar with the gas laws, the first law of thermo-
dynamics and the concepts of internal energy, enthalpy and other
gas properties. For those of you who lack this experience I have
included within the extra notes - ‘Thermodynamics Refresher, a
brief set of notes covering these topics which you are advised to
study before continuing.
A consequence to Dalton’s law of Partial Pressure is that
the total enthalpy of a mixture of gases will equal the sum of the
enthalpies of each component part, i.e.:
h = m1
.h1
+ m2
. h2
+ m3
.h3
+ .... etc.
Water Vapour
In addition to these dry gases, the air also contains varying
amounts of water vapour. At normal temperatures and pressures,
water is able to exist in both a liquid and a gaseous (or vapour)
form, but it cannot be treated in the same way as the other gases
of the atmosphere because its quantity, and hence proportion are
continually varying.
Water vapour is said to be associated with dry air and the
more vapour associated with the dry gases, the more humid the
air. At sea level, atmospheric pressure is normally within the
range 95 to 105 Pa, but this depends upon weather conditions.
The agreed international standard atmosphere has a pressure of
101.325 kPa (1013.25 mbar) and this reduces at the rate
0.013 kPa per metre of height above sea level and increases at
the same rate below sea level.
The water vapour is completely independent of the dry
atmospheric gases, and its behaviour is not affected by their pres-
ence of absence, but for any given temperature there is a maxi-
mum amount of vapour that can be absorbed or associated with a
given volume of air. In addition, although the actual quantity of
water is quite small, it can have a dramatic effect on our percep-
tion of comfort.
(Under certain conditions the mass of water vapour will
change due to condensation or evaporation (known as dehu-
midification and humidification respectively), but the mass of
dry air will remain constant. It is therefore convenient to relate
all properties of the mixture to the mass of dry air rather than to
the combined mass of air and water vapour).Xtra
Basic
Thermodynamics
SOLID LIQUID
GAS
Melting
Freezing
Evaporating
Condensing
Particles in a solid normally have
no motion relative to each other
except vibration about a fixed
position. If we increase the energy
content, particles can break the
bonds which bind them and the
solid melts
Particles in a liquid do not occupy
fixed positions, but they are not
completely free.The particles can
slide over one another allowing the
liquid to flow.
Energy supplied to a liquid
allows the particles to break
free of each other and
become a gas. If energy is
removed from the gas it will
again condense to a liquid
The States of
Matter
—
5a
Notes Notes
1–5aPage 5a1–5bPage Chapter 1 – Introduction to Psychrometry
Saturated Vapour Pressure (PSS
)†1.3
Heat is a form of internal energy. This is a thermodynamic
property†1.4
and represents the internal energy of the molecules.
With increase temperature there is an increase in molecular activ-
ity and thus more water can escape from the liquid into the gas as
water vapour or steam. After a while however, even at this in-
creased temperature, the air will become fully saturated with water
vapour so that no more water can evaporate unless we again in-
crease the temperature.
The pressure produced by the water vapour in this fully
saturated condition is known as the saturated vapour pressure
(pss
) and since at a given temperature the air cannot absorb more
water than its saturated condition, the saturated vapour pressure
is the maximum pressure of water vapour that can occur at any
given temperature.
Eventually of course, if we continue to supply heat the
water will boil, and this will occur when the saturated vapour
pressure is equal to the atmospheric pressure.
Psychrometric Chart
There is a fixed relationship†1.5
between saturated vapour
pressure and temperature, for example;
See
Notes
See
Notes
100
80
60
40
20
0
20
Normal air temperature, as you might expect, can be meas-
ured by a normal mercury-in-glass thermometer
Temperature (°C) 10.0 20.0 30.0 40.0 50.0 60.0
Pressure (Pa) 1.23 2.34 4.24 7.38 12.33 19.92
and this relationship forms the basis for the psychrometric chart
(click adjacent symbol), which is essentially a plot of vapour pres-
sure against air temperature.
This is known as the Dry-bulb temperature (tdb
) because
the bulb of the thermometer is kept dry (as opposed to the wet-bulb
thermometer which we will introduce later). Vapour pressure (ps
) is
the actual pressure of vapour existing at any particular location
and time and temperature and is a property of the moisture con-
tent of the air.
Psychro
Chart
temperature
moisturecontent
vapourpressure
saturation
vapour
pressure
Saturation moisture content †1.6
against temperature
Although the CIBSE
Psychrometric Chart
is derived on the basis
of the relationship
between vapour
pressure and
temperature, the
published chart does
not show vapour
pressure but rather
shows moisture
(vapour) content
against temperature
as this is more useful
to the user.
—
6a
Notes Notes
1–6aPage 6a1–6bPage Chapter 1 – Introduction to Psychrometry
Moisture content (g)
Dry-bulb temperature and vapour pressure are the two ba-
sic parameters which determine the humid condition of atmos-
pheric air, but other properties can be derived from them and
likewise, they can be derived from other properties. In practice
we are not really interested in the pressure exerted by the vapour
in a mixture of air and water vapour, but we do need to know the
quantity of water that exists at any time. One way of measuring
this amount in by the moisture content and can be expressed in
kg of water vapour per kg of dry air (kg/kg of dry air). [The term
‘humidity ratio’ was used in the past, but is not common today].
g = mass of water vapour (kg) = ms
mass of dry air (kg) ma
The moisture content is shown on the right-hand side of the
psychrometric chart (click adjacent symbol).
Percentage saturation (µµµµµ)
Percentage saturation is a useful guide to comfort as the
human body tends to respond to relative saturation rather than
moisture content, and is the ratio between the actual moisture
content of the sample (gs
) and the moisture content of a sample
of saturated air (gss
), at the same temperature.
Psychro
Chart
temperature
moisturecontent
saturation
moisture
content
For user convenience, the
Psychrometric Chart is
scaled in moisture content ○
○
○
○
temperature
moisturecontent
100% saturation
t
gs
ssg
% sat
Definition of percentage
saturation
µµµµµ = gs
x 100 (%)
gss
○ ○ ○ ○ ○ ○ ○
µ (%) = moisture content of sample x 100 (kg)
moisture content of saturated air (kg)
= gs
x 100
gss
The property is shown on the psychrometric chart and to
make the chart easier to use, the chart also includes lines of con-
stant percentage saturation (click adjacent symbol).
Psychro
Chart
—
7a
Notes Notes
1–7aPage 7a1–7bPage Chapter 1 – Introduction to Psychrometry
Relative humidity (rh)
Although percentage saturation is the preferred method of
expressing the humidity ratio, relative humidity is another method
of measuring the amount of water vapour present in the air, and
is a hangover from the days of ‘imperial’ measurement. It is the
ratio of the vapour pressure of an air sample to the saturated va-
pour pressure at the same temperature, and is usually expressed
as a percentage.
Relationship between g, µµµµµ and rh
We are now in a position to derive useful expressions for
moisture content and percentage saturation in terms of partial
pressure and hence compare percentage saturation with relative
humidity.
If we consider the humid air mixture, the moisture (va-
pour) content of the air can be expressed either as a specific value
or as a ratio, as we noted before, of the mass of vapour to the
mass of dry air.
Thus by definition g = ms
ma
but from the perfect gas laws: µ = p .V so that
R .T
µa
= pa
. Va
and µs
= ps
. Vs
Ra
. Ta
Rs
. Ts
Thus we can also define moisture content as:
g = ps
. Vs
x Ra
. Ta
pa
. Va
Rs
. Ts
but for a mixture, the volumes and the temperatures must be equal,
i.e. Vs
= Va
and Ts
= Ta
so that the above formula can be simplied
to:
g = ps
x Ra
pa
Rs
But since we know the value of the gas constants, a ratio can be
found for Ra
/ Rs
, so that g = 0.622 ps
pa
and we also know from Dalton’s Law of partial pressure that
pa
= patm
†1.8
– ps
and finally therefore: g = 0.622 ps
(patm
– ps
)
See
Notes
rh (%) = partial pressure of water vapour in sample x 100 (Pa)
partial pressure of water vapour in saturated air (Pa)
= ps
x 100
pss
(at the same dry-bulb temperature)
Percentage saturation or relative humidity are frequently
used in specifications as a requirement of air humidity condi-
tions†1.7
. However, as the relationship between vapour pressure
and moisture content is not quite linear, their will always be a
slight (but not usually significant) difference between them.
See
Notes
temperature
moisturecontent
vapourpressure
saturation
vapour pressure
= 100% r.h.
t
ps
ssp
% r.h. = p x 100%
p
s
ss
Definition of relative humidity
Although the
Psychrometric
Chart is scaled in
terms of moisture
content, this is for
convience,we could
determine vapour
pressure from:
g = 0.622 x ps
pa
—
8a
Notes Notes
1–8aPage 8a1–8bPage Chapter 1 – Introduction to Psychrometry
Comparision of percentage saturation and rh
From the previous definition, we know that
Wet-bulb temperature (twb
)
The wet-bulb temperature, as the name implies, is the air
temperature measured by a thermometer with a bulb covered with
a muslin cloth sleeve and kept moist with distilled or clean water.
It was devised as a means of assessing the humidity of the air, but
as the actual reading is influenced by air movement, there are
two variations of this temperature.
1. The Sling Wet-bulb
The ‘sling wet-bulb’ temperature reading obtained in mov-
ing air†1.10
– preferably above 2 m/s. It can be obtained by whirl-
ing a ‘sling hygrometer’ or by using the more cumberson, but
more accurate ‘Assman hygrometer’ which is fan-assisted.
µ = gs
x 100 %
gss
but using the above expression derived from moisture content,
we can also express the percentage saturation as:
µ = ps
. (patm
- pss
) x 100 %
pss
. (patm
- ps
)
Compare this to the definition of relative humidity:
rh (φ) = ps
x 100 %
pss
Since patm
is very much bigger than ps
or pss
, then the relative
humidity is very nearly equal to the percentage saturation. i.e.
j
Although relative humidity and percentage saturation are
useful guides to comfort, it is not always practical to measure
them directly. In fact measurement of humid air has always been
a problem and the most practical method is to use a wet-bulb
thermometer†1.9
.
See
Notes
See
Notes
VIDEOEO
Sling Hygrometer
Assman
Hygrometer
2. The Screen Wet-bulb
The screen wet-bulb tempera-
ture is the reading obtained in still
air. This is usually used for mete-
orological data and is obtained from a wet-bulb thermometer in-
stalled into a ‘Stevenson Screen’ (from which this type of meas-
urement gets its name). This is a slatted enclosure, designed to
screen direct radiation from the instruments, but equipped with
wet and dry-bulb thermometers and maximum and minimum ther-
mometers.
Of the two methods of reading wet-bulb, the sling reading
is considered to be more accurate and is therefore preferred by
air-conditioning engineers.
—
9a
Notes Notes
1–9aPage 9a1–9bPage Chapter 1 – Introduction to Psychrometry
The Psychrometric Equation
The psychrometric equation links the dry-bulb and the wet-
bulb temperatures to their corresponding vapour pressures and to
the atmospheric pressure.
Consider air flowing across the bulb of a wet-bulb ther-
mometer:
At the surface of the muslin sleeve the air is considered to
be at saturation moisture content (gss
’)†1.11
, so that the latent heat
gain is proportional to the difference in moisture content between
the film of air surrounding the muslin sleeve and the surrounding
air, i.e. to ( gss
’ – gs
).
Similary, the sensible heat lost is proportional to the tem-
perature difference between the bulb and the ambient tempera-
ture, i.e. to (t – t’), and since one process is the cause of the other
we may equate them as:
B . (gss
’ - gs
) = C . (t - t’) – (equation 1)
where B and C are constants which relate to surface area and
latent heat. But from our earlier equation for moisture content,
we known that:
gs
= 0.622 ps
patm
– ps
and
gss
’ = 0.622 pss
’
patm
– pss
’
and since ps
and pss
’ are both very small compared to patm
we may re-write these equations more simply as:
g = 0.622 ps
and gss
’ = 0.622 pss
’
patm
patm
Hence by substituting these expressions for moisture content into
our equation 1, we get:
0.622 . B . (pss
’ – ps
) = C . (t – t’)
patm
From which we obtain:
ps
= pss
’ – patm
. A . (t – t’).
where A is known as the psychrometric constant and the differ-
ence between the dry-bulb and the wet-bulb temperatures (t – t’)
is known as the wet-bulb depression.
See
Notes
Wet-bulb thermometer
123123123123
123
123123
20
0
20
air-flow
muslin
sleeve
ambient air
with properties: t, ps
, gs
air around muslin sleeve with
properties: t’, pss
’, gss
’
Moisture will be evaporated from the muslin cloth sleeve
around the bulb and will be taken up (associated) with the sur-
rounding air. For this evaporation to take place heat must be
supplied and this can only come from the surrounding air, i.e the
latent heat of evaporation gained by the moisture on the surface
of the muslin as it associates with the air, must equal the sensible
heat lost from the surrounding air, in other words there must be a
drop in the wet-bulb temperature to compensate for the increase
in mosture content to the air around it.
—
10a
Notes Notes
1–10aPage 10a1–10bPage Chapter 1 – Introduction to Psychrometry
Now the rate of moisture evaporation is different if the air
is above or below freezing point (0°C) and between still and
moving air (a standard speed of 2 m/s is used, but between about
2 m/s and 20 m/s the effect of air velocity is practically constant).
Different values of the psychrometric constant are therefore quoted
to cater for these conditions:
Dew-point temperature (tdp
)
The dew-point temperature is a very important property in
air-conditioning†1.12
as it determines if water will be condensed
from air when it is cooled. This occurs when a sample of air is
cooled to the point where its vapour pressure reaches its satu-
rated vapour pressure. For example, suppose air is being cooled
at constant vapour pressure (i.e. constant moisture content). Even-
tually, the temperature of the air will reach a point where the air is
fully saturated (on our psychrometric chart – the ‘saturation line)
and if the temperature drops lower than this point, water vapour
will begin to condense. This point in known as the dew-point
temperature (tdp
) and again can be represented on our
psychrometric chart (click adjacent symbol).
dry-bulb temperature
moisturecontent
100% saturation
Lines of constant
wet-bulb temperature
Lines of Constant
Wet-bulbTemperature
Psychro
Chart
Psychrometric Constants
Sling: A = 6.66 x 10- 4
(K - 1
) for t’ greater than 0 °C
A = 5.94 x 10 - 4
(K - 1
) for t’ less than 0 °C
Screen: A = 7.99 x 10 - 4
(K - 1
) for t’ greater than 0 °C
A = 7.20 x 10 - 4
(K - 1
) for t’ less than 0 °C
Wet-bulb temperature is also shown on a psychrometeric
chart and to assist with humidification processes (those which
increase the moisture content), they are shown as lines of con-
stant wet-bulb temperature (click adjacent symbol).
Note: When working with the psychrometric equation, it is im-
portant to remember that the saturated vapour pressure (pss
’) is
taken at the wet-bulb temperature.
See
Notes
Psychro
Chart
temperature
moisturecontent
100% saturation
t
ga
A
dp
dew-point temperature
of air at condition A
Dew-pointTemperature
We should also realise that moist air does not need to be
cooled to its dew-point for condensation to occur. Any surface
with a temperature below the dew-point of the moist air will, of
course, get wet and it is important to appreciate this when trying
to avoid problems of condensation.
—
11a
Notes Notes
1–11aPage 11a1–11bPage Chapter 1 – Introduction to Psychrometry
Specific enthalpy (h)
Enthalpy (see Thermofluids Refresher, page C-5a) is a
measure of energy, but although in psychrometry it is only the
heat energy which is of interest, this is still referred to an enthalpy.
Enthalpy is an extensive property, i.e its value depends upon the
amount of substance present. An intensive property is therefore
more useful since it does not depend upon the amount of mate-
rial present. It is usually obtained by dividing the extensive prop-
erty by its mass and is then known as specific property. Thus the
specific enthalpy (h), is a measure of the heat energy (sensible
and latent) of 1 kg of dry air plus its associated water vapour
(measured in units of kJ/kg) relative to zero°C and zero moisture
content.
To calculate the specific enthalpy for an air sample we can
use Dalton’s Law of Partial Pressures, i.e.,
h = h1
+ h2
+ h3
where the specific enthalpy for each part of the air-mixture is
given by: h = mass x specific heat x ∆t.
Thus for example, to calculate the specific enthalpy for air
at a dry-bulb temperature of 20°C and a moisture content of
0.005 kg/kg, we can proceed as follows:
Taking as our sample, 1 kg of dry air and its associated
moisture content, the enthalpy of the dry air is given by:
h1
= 1 x 1.005 x 20 = 20.1 kJ/kgK,
where 1 is the mass of dry air,
1.005 is the specific heat of dry air and
20 is the air temperature relative to 0°C.
similarly the sensible heat energy of the moisture content is given
by: h2
= 0.005 x 1.89 x 20 = 0.189
where 0.005 is the moisture content
1.89 is the specific heat of water vapour and
20 is the air temperature relative to 0°C.
Finally, the water vapour is considered to have evaporated at 0°C.
We therefore have to include the latent heat of evaporation for
the moisture content. Thus the latent heat energy of the moisture
content is given by:
h3
= 0.005 x 2501 = 12.505
where 0.005 is the moisture content and
2501 is the latent heat of evaporation at 0°C†1.13
.
Thus the total enthalpy is given by h1
+ h2
+ h3
= 20.1 + 0.189 + 12.505 = 32.794 = 32.8 kJ/kg
However, specific enthalpy can be determined much more
quickly by direct reading from the psychrometric chart.
Enthalpy scales are located ‘around the edges’ of the chart
(click adjacent symbol), and there are no lines of constant enthalpy.
To therefore obtain the specific enthalpy of an air condi-
tion, a straight edge is used to join the corresponding enthalpy
marks above to 100% saturation line with those on either the
bottom, or the right-hand side of the chart (click on adjacent video
symbol).
Psychro
Chart
VIDEOEO
specific enthalpy
specificenthalpy
Specific Enthalpy
at edges of chart
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
See
Notes
—
12a
Notes Notes
1–12aPage 12a1–12bPage Chapter 1 – Introduction to Psychrometry
See
Notes
Psychro
Chart
In addition to the temperatures already noted, the following
psychrometric parameters may also be required.
Specific volume (v)
The specific volume, is the volume of unit mass of dry air
at a given temperature normally expressed as m3
/kg and is also
shown in the psychrometric chart (click adjacent symbol).
Note: that the specific volume is a measure of dry air, since the addi-
tion of any associated water vapour has no effect on the volume (Dalton’s
Law).
Thus, with the exception of vapour pressure and saturation
vapour pressure, all these psychrometric parameters are brought
together on the psychrometric chart, from which any two are suf-
ficient to indentify an air condition, the others then being read
from the chart as required (see chart overleaf).
In practice only two combinations†1.15
are used;
dry-bulb temperature
moisturecontent
100% saturation
Lines of
constant volume
Lines of Constant Volume
Density (ρρρρρ)
The density of air is taken for a moist air sample and there-
fore includes the mass of the associated water vapour. The spe-
cific volume however, is defined in terms of dry air and thus the
specific volume is not the reciprocal of density.
The exact relationship is given by:
ρ = (1 + g)
v
In practice however, the difference is very small and can be
ignored†1.14
.
dry-bulb (tdb
) and wet-bulb (twb
) temperature
for measurements
and
dry-bulb temperature (tdb
) and percentage saturation (µµµµµ)
[or relative humidity (rh)]
for specifications.
See
Notes
90 80 70 60 50 40 30 20
PERCENTAGE SATURATION
0.75
0.80
0.85
0.90
SPECIFIC VOLUME m
3 /kg
-10 -5 0 5 10 15 20 25 30 35 40 45 50 55 60
DRY – BULB TEMPERATURE ˚C
30
25
20
15
10
5
0
-5
-10
W
ET-BULB
TEM
PERATURE
˚C
(SLING
)
0.000
0.001
0.002
0.003
0.004
0.005
0.006
0.007
0.008
0.009
0.010
0.011
0.012
0.013
0.014
0.015
0.016
0.017
0.018
0.019
0.020
0.021
0.022
0.023
0.024
0.025
0.026
0.027
0.028
0.029
0.030
MOISTURECONTENTkg/kg
-10 -5 0 5 10 15
-20 25 30 35 40-20 25 30 35 40
-45 50 55 60 65
SPECIFIC ENTHALPY kJ/kg
70758085
9590100105110
120115125130135135140
-10
-5
0
5
10
15
20
25
30
35
40
45
50
55
60
65
70
75
80
85
90
95
100
105
110
105
120 125 130 135 140
SPECIFIC
ENTHALPY
kJ/kg
SENSIBLE/TOTAL HEAT
RATIO FORWATER
ADDED AT 30˚C
0.1 0
0
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
0.9
0.8
0.7
0.6
0.5
0.4
0.3
0.2
0.1
BASED ON A BAROMETRIC
PRESSURE OF 101.325 kPa
CIBSE
PSYCHROMETRIC
CHART
svp g rh% sat wb dew h v
—
14a
Notes Notes
1–14aPage 14a1–14bPage Chapter 1 – Introduction to Psychrometry
Quick Revision Study Guide 1
The following questions are intended as a quick study question-
naire to ensure you have grasped the general principles of this
chapter.
It is intended that your answers should be, short-phrased, quick
answers or sketches to the questions.
For suggested solutions to these questions, please refer to the
Denco Website: www. denco.co.uk
1. 0.01 kg of steam with a specific enthalpy of 2,700 kJ/kg
is mixed with 2.0 kg of dry air with a specific enthalpy of
20 kJ/kg. What is the specific enthalpy of the mixture?
2. Moist air has a dry-bulb temperature of 30°C, and a
wet-bulb temperature of 20°C.
Use a Psychrometric Chart to find
a. The percentage saturation
b. The moisture content
c. The enthalpy
d. The specific volume
e. The dew-point temperature
3. Moist air at 25°C dry-bulb and 50% saturation, undergoes
a process so that its condition is changed to 40°C dry-
bulb and 30% saturation. Use a Psychrometric Chart to
determine the change in specific enthalpy for the process.
4. The air inside a room during winter is at 20°C db and 40%
saturation. If the temperature of the inside surface of a
window is 9°C, will condensation form on the window
glass?
5. A sling psychrometer measured the dry and wet-bulb
temperatures of moist air as 27°C and 19°C respectively.
Determine the moisture content from the relevant
equation, given that:
(i) pss
at 19°C is 2.196 kPa,
(ii) the psychrometric constant is 6.66 x 10-4
K-1
—
15a
Notes Notes
1–15aPage 15a1–15bPage Chapter 1 – Introduction to Psychrometry
Chapter Notes
†1-1: Air;
is a mixture containing a group of gases of nearly constant pro-
portions (% of atmosphere):
Nitrogen (N2
) 78.804 Methane (CH4
) 0.0002
Oxygen (O2
) 20.964 Krypton (Kr) 0.000114
Argon (Ar) 0.934 Hydrogen (H2
) 0.00005
Neon (Ne) 0.0018 Nitrous Oxide (N2
O) 0.00005
Helium (He) 0.000524 Xenon (Xe) 0.0000087
and a group of gases present in proportions, variable both in time
and space (% of atmosphere):
Water Vapour (H2
O) 0 – 7
Carbon Dioxide (CO2
) 0.01 – 0.1 (Average about 0.032)
Ozone (O3
) 0 – 0.01
Sulphur Dioxide (SO2
) 0 – 0.0001
Nitrogen Dioxide (NO2
) 0 – 0.000002
(Ref Encylopaedia Britannica CD-ROM, 1998 Edition).
†1-2: Pressure;
force per unit area, i.e. the force spread over a particular area, is
measured in newtons and area in square metres. So pressure is
measured in newtons per square metre but it can also be meas-
ured in pascal (symbol Pa, where 1 Pa = 1 N/m2
).
Traditionally, it has also been common to express atmospheric
pressure in units of bar or millibar, where 10 bar = 105
Pa,
(Bar: from the Greek meaning weight, thus a ‘barometer’ [a word
again derived from the Greek meaning weight + measure], is an
instrument to measure the weight or pressure of the atmosphere).
†1.3: Subscripts;
it is normal to apply the following subscripts:
s refers to water vapour (steam), eg Ps
a refers to dry air, eg Pa
ss refers to a saturated condition for water vapour in air, eg Pss
†1.4: Internal Energy;
is the molecular energy possesed by a material and includes the
kinetic energy of the molecules due to vibration and the potential
energy associated with the forces between them.
Two terms can be used as a measure of this energy -
the Internal Energy (symbol: U; unit:J) and the
Specific Internal Energy (symbol: u; unit: J/kg).
†1.5: Saturated Vapour Pressure vs Temperature;
there is no simple relationship between temperature and saturated
vapour pressure. The following equations have been developed
by the National Engineering Laboratory as close curve fits to
empirically measured data:
For water above 0°C
Log10
Pssw
= 28.59 - 8.2 log10
T + 0.00248 T - 3142
T
where Pssw
is the saturated vapour pressure (bar) of vapour over water
at an absolute temperature of T (K).
For ice below 0°C
Log10
Pssi
= 10.538 - 2664
T
where Pssw
is the saturated vapour pressure (bar) of vapour over ice at
an absolute temperature of T (K).
†1.6: Moisture Content;
is really a misnomer since what we are really referring to is ‘va-
pour’ content, but the term has used by the industry as such for
many years and so we just have to accept the inaccuracy of the
wording.
—
16a
Notes Notes
1–16aPage 16a1–16bPage Chapter 1 – Introduction to Psychrometry
†1.7: Relative Humidity - to a Base of Pressure;
you will note that the relative humidity is based upon pressure,
not mass of water vapour and is the traditional method of stating
humidity as the ‘sling psychrometer’ (see page 1-8b) gave a meas-
ure of vapour pressure.
†1.8: Atmospheric pressure;
patm
= pa
+ ps
†1.9: Psychrometer;
the word ‘Psychrometer’ is originally from the Greek meaning
‘cold’ + ‘meter’, i.e. literally meaning a measurer of cold. Its
current meaning is two thermometers, mounted on the same scale,
with indications of wet-bulb and dry-bulb temperatures. Hence
the word ‘Psychrometry’ is the determination of the degree of
humidity in the atmosphere by means of a psychrometer and is
therefore used to define the study of atmospheric air and its asso-
ciated water vapour.
†1.10: Use of Wet-bulb in Air Conditioning Duct;
a sling wet-bulb reading may also be obtained by installing a
wet-bulb thermometer in a duct through which air is flowing at a
reasonable velocity.
†1.11 Note the use of the dash ( ’ ) symbol to indicate that the
reading is a wet-bulb reading.
†1.12 Dew-point Instruments;
there are commercial instruments which can measure the dew-
point temperature directly. However, it is more usual to obtain a
value by reference to tables of humid air properties, or to deter-
mine its value from the psychrometric chart using the measure-
ments of other air properties.
†1.13: Latent heat;
values for temperatures other than zero °C, can be found from
standard tables for the ‘Thermodynamic Properties of Saturated
Liquid Water and Dry Saturated Steam’, more commonly known
as ‘Steam Tables’.
†1.14: Air Density and Specific Volume;
Although the difference between air density and the reciprocal of
specific volume is small, it should be recognised that a differ-
ence does exist where this relates to different areas of work. For
example, when measuring air-flow rates through pressure drop
devices, it is usual to use air density. On the other hand, for air-
conditioning load calculations, it is usual to use specific volume.
†1.15: CIBSE psychrometric chart;
the CIBSE psychrometric chart is strictly correct only for a total
pressure of 101.325 kPa (i.e standard atmospheric pressure).
Charts are available for other pressures, or correction factors may
be used such as those quoted in the CIBSE Guide C1.
In addition, the principal axes of the chart are not, as is often
assumed, dry-bulb temperature and moisture content, but
enthalpy and moisture content. If you look carefully at a com-
mercial psychrometric chart, you will see that the dry-bulb tem-
perature lines are not quite parallel, nor vertical.

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Denco chart

  • 1. — 1a Notes Notes 1–1aPage 1a1–1bPage Chapter 1 – Introduction to Psychrometry Learning Outcomes Learning Outcomes: When you have studied this chapter you should be able to: 1 Explain what is meant by the term ‘Psychrometry’. 2. Relate ‘Dalton’s law of Partial Pressures’ to the term ‘Atmospheric Pressure’. 3. Explain what is meant by the term ‘Saturated Vapour Pressure’. 4. Use a ‘Psychrometric Chart to find: a. A saturated vapour pressure for a given temperature. Find, for a given air sample, the following: b. The moisture content c. The percentage saturation d. The relative humidity. 5. Explain what is meant by the ‘wet-bulb’ temperature and its use in the ‘psychrometric equation’. 6. Show how the Psychrometric Chart is used to determine: a. Dew-point temperature b. Specific Enthalpy Suggested StudyTime: (a) For study of chapter material; (i) Initial on-screen study 1 hour (ii) Printing of notes and subsequent in-depth study 2 hours (b) For completion of the quick revision study guide ½ hour Total estimated study time 3½ hours Introduction to Psychrometry Chapter 1 Chapter 1 Introduction to Psychrometry
  • 2. — 2a Notes Notes 1–2aPage 2a1–2bPage Chapter 1 – Introduction to Psychrometry Chapter Contents Item page Learning Outcomes 1-1b Introduction to Psychrometry 1-3a The Atmosphere 1-3a Water Vapour 1-4a Saturated Vapour Pressure 1-5a Psychrometric Chart (Theory) 1-5b Moisture content 1-6a Relative humidity 1-6b Percentage saturation 1-7a Relationship between g, m and rh 1-7b Comparision of percentage saturation & rh 1-8a Wet-bulb temperature 1-8b 1. The Sling Wet-bulb 1-8b 2. The Screen Wet-bulb 1-8b The Psychrometric Equation 1-9a Dew-point temperature 1-10b Specific enthalpy 1-11a Specific volume 1-12a Density 1-12a Psychrometric chart 1-13 Quick Revision Study Guide 1-14a Chapter Notes 1-15a
  • 3. — 3a Notes Notes 1–3aPage 3a1–3bPage Chapter 1 – Introduction to Psychrometry Introduction to Psychrometry The Atmosphere Psychrometry is the study of atmospheric air and its asso- ciated water vapour. Air comprises a mixture of gases†1.1 of which nitrogen makes up 78%, oxygen 21% and carbon dioxide and the inert gases (such as argon, neon, krypton, helium etc.) the remainder. These are known as the dry gases of the atmosphere. Principle Dry Atmospheric Gases VIDEOEO See Notes Gas A at partial pressure PA Gas B at partial pressure Pb Gas A + B at total pressure PA + PB Dalton’s Law, illustrates that if two gases are combined into the same volume, the total pressure is the sum of the individual partial gas pressures. In a vessel open to the atmosphere, it is the weight of the atmospheric gases above the earth’s surface that produce the pressure†1.2 of the atmosphere. - 1200˚C - 1200˚C - 1150˚C - 1100˚C - 900˚C - 200˚C - 75˚C - 60˚C - 60˚C + 20˚C 400km 350km 300km 250km 200km 150km 100km 50kmSTRATOSPHERE TROPOPAUSE TROPOSPHERE IONOSPHERE Clouds, Winds No Clouds, No Winds ApproximateTemperature Height The Earth’s Atmosphere See Notes In the air mixture, the dry gases and associated water va- pour behave according to ‘Dalton’s law of Partial Pressures’. That is they behave independently of one another and the pressure each exerts combine to produce an overall ‘atmospheric pressure’. 0 10 20 30 40 50 60 70 80 Nitrogen Oxygen Carbon Dioxide MolecularWeight %Atmosphere
  • 4. — 4a Notes Notes 1–4aPage 4a1–4bPage Chapter 1 – Introduction to Psychrometry Since at normal temperatures and pressures we are unable to condense these gases out from the atmosphere, for the purpose of psychrometry, this mixture of gases can be treated as if it were a single ‘ideal’ or perfect gas behaving as a single element known as ‘dry air’. Note: Psychrometry is a specialised area of thermodynam- ics but obviosuly has applications in air conditioning. None the less, in order to fully appreciate the material within this course you need to be familiar with the gas laws, the first law of thermo- dynamics and the concepts of internal energy, enthalpy and other gas properties. For those of you who lack this experience I have included within the extra notes - ‘Thermodynamics Refresher, a brief set of notes covering these topics which you are advised to study before continuing. A consequence to Dalton’s law of Partial Pressure is that the total enthalpy of a mixture of gases will equal the sum of the enthalpies of each component part, i.e.: h = m1 .h1 + m2 . h2 + m3 .h3 + .... etc. Water Vapour In addition to these dry gases, the air also contains varying amounts of water vapour. At normal temperatures and pressures, water is able to exist in both a liquid and a gaseous (or vapour) form, but it cannot be treated in the same way as the other gases of the atmosphere because its quantity, and hence proportion are continually varying. Water vapour is said to be associated with dry air and the more vapour associated with the dry gases, the more humid the air. At sea level, atmospheric pressure is normally within the range 95 to 105 Pa, but this depends upon weather conditions. The agreed international standard atmosphere has a pressure of 101.325 kPa (1013.25 mbar) and this reduces at the rate 0.013 kPa per metre of height above sea level and increases at the same rate below sea level. The water vapour is completely independent of the dry atmospheric gases, and its behaviour is not affected by their pres- ence of absence, but for any given temperature there is a maxi- mum amount of vapour that can be absorbed or associated with a given volume of air. In addition, although the actual quantity of water is quite small, it can have a dramatic effect on our percep- tion of comfort. (Under certain conditions the mass of water vapour will change due to condensation or evaporation (known as dehu- midification and humidification respectively), but the mass of dry air will remain constant. It is therefore convenient to relate all properties of the mixture to the mass of dry air rather than to the combined mass of air and water vapour).Xtra Basic Thermodynamics SOLID LIQUID GAS Melting Freezing Evaporating Condensing Particles in a solid normally have no motion relative to each other except vibration about a fixed position. If we increase the energy content, particles can break the bonds which bind them and the solid melts Particles in a liquid do not occupy fixed positions, but they are not completely free.The particles can slide over one another allowing the liquid to flow. Energy supplied to a liquid allows the particles to break free of each other and become a gas. If energy is removed from the gas it will again condense to a liquid The States of Matter
  • 5. — 5a Notes Notes 1–5aPage 5a1–5bPage Chapter 1 – Introduction to Psychrometry Saturated Vapour Pressure (PSS )†1.3 Heat is a form of internal energy. This is a thermodynamic property†1.4 and represents the internal energy of the molecules. With increase temperature there is an increase in molecular activ- ity and thus more water can escape from the liquid into the gas as water vapour or steam. After a while however, even at this in- creased temperature, the air will become fully saturated with water vapour so that no more water can evaporate unless we again in- crease the temperature. The pressure produced by the water vapour in this fully saturated condition is known as the saturated vapour pressure (pss ) and since at a given temperature the air cannot absorb more water than its saturated condition, the saturated vapour pressure is the maximum pressure of water vapour that can occur at any given temperature. Eventually of course, if we continue to supply heat the water will boil, and this will occur when the saturated vapour pressure is equal to the atmospheric pressure. Psychrometric Chart There is a fixed relationship†1.5 between saturated vapour pressure and temperature, for example; See Notes See Notes 100 80 60 40 20 0 20 Normal air temperature, as you might expect, can be meas- ured by a normal mercury-in-glass thermometer Temperature (°C) 10.0 20.0 30.0 40.0 50.0 60.0 Pressure (Pa) 1.23 2.34 4.24 7.38 12.33 19.92 and this relationship forms the basis for the psychrometric chart (click adjacent symbol), which is essentially a plot of vapour pres- sure against air temperature. This is known as the Dry-bulb temperature (tdb ) because the bulb of the thermometer is kept dry (as opposed to the wet-bulb thermometer which we will introduce later). Vapour pressure (ps ) is the actual pressure of vapour existing at any particular location and time and temperature and is a property of the moisture con- tent of the air. Psychro Chart temperature moisturecontent vapourpressure saturation vapour pressure Saturation moisture content †1.6 against temperature Although the CIBSE Psychrometric Chart is derived on the basis of the relationship between vapour pressure and temperature, the published chart does not show vapour pressure but rather shows moisture (vapour) content against temperature as this is more useful to the user.
  • 6. — 6a Notes Notes 1–6aPage 6a1–6bPage Chapter 1 – Introduction to Psychrometry Moisture content (g) Dry-bulb temperature and vapour pressure are the two ba- sic parameters which determine the humid condition of atmos- pheric air, but other properties can be derived from them and likewise, they can be derived from other properties. In practice we are not really interested in the pressure exerted by the vapour in a mixture of air and water vapour, but we do need to know the quantity of water that exists at any time. One way of measuring this amount in by the moisture content and can be expressed in kg of water vapour per kg of dry air (kg/kg of dry air). [The term ‘humidity ratio’ was used in the past, but is not common today]. g = mass of water vapour (kg) = ms mass of dry air (kg) ma The moisture content is shown on the right-hand side of the psychrometric chart (click adjacent symbol). Percentage saturation (µµµµµ) Percentage saturation is a useful guide to comfort as the human body tends to respond to relative saturation rather than moisture content, and is the ratio between the actual moisture content of the sample (gs ) and the moisture content of a sample of saturated air (gss ), at the same temperature. Psychro Chart temperature moisturecontent saturation moisture content For user convenience, the Psychrometric Chart is scaled in moisture content ○ ○ ○ ○ temperature moisturecontent 100% saturation t gs ssg % sat Definition of percentage saturation µµµµµ = gs x 100 (%) gss ○ ○ ○ ○ ○ ○ ○ µ (%) = moisture content of sample x 100 (kg) moisture content of saturated air (kg) = gs x 100 gss The property is shown on the psychrometric chart and to make the chart easier to use, the chart also includes lines of con- stant percentage saturation (click adjacent symbol). Psychro Chart
  • 7. — 7a Notes Notes 1–7aPage 7a1–7bPage Chapter 1 – Introduction to Psychrometry Relative humidity (rh) Although percentage saturation is the preferred method of expressing the humidity ratio, relative humidity is another method of measuring the amount of water vapour present in the air, and is a hangover from the days of ‘imperial’ measurement. It is the ratio of the vapour pressure of an air sample to the saturated va- pour pressure at the same temperature, and is usually expressed as a percentage. Relationship between g, µµµµµ and rh We are now in a position to derive useful expressions for moisture content and percentage saturation in terms of partial pressure and hence compare percentage saturation with relative humidity. If we consider the humid air mixture, the moisture (va- pour) content of the air can be expressed either as a specific value or as a ratio, as we noted before, of the mass of vapour to the mass of dry air. Thus by definition g = ms ma but from the perfect gas laws: µ = p .V so that R .T µa = pa . Va and µs = ps . Vs Ra . Ta Rs . Ts Thus we can also define moisture content as: g = ps . Vs x Ra . Ta pa . Va Rs . Ts but for a mixture, the volumes and the temperatures must be equal, i.e. Vs = Va and Ts = Ta so that the above formula can be simplied to: g = ps x Ra pa Rs But since we know the value of the gas constants, a ratio can be found for Ra / Rs , so that g = 0.622 ps pa and we also know from Dalton’s Law of partial pressure that pa = patm †1.8 – ps and finally therefore: g = 0.622 ps (patm – ps ) See Notes rh (%) = partial pressure of water vapour in sample x 100 (Pa) partial pressure of water vapour in saturated air (Pa) = ps x 100 pss (at the same dry-bulb temperature) Percentage saturation or relative humidity are frequently used in specifications as a requirement of air humidity condi- tions†1.7 . However, as the relationship between vapour pressure and moisture content is not quite linear, their will always be a slight (but not usually significant) difference between them. See Notes temperature moisturecontent vapourpressure saturation vapour pressure = 100% r.h. t ps ssp % r.h. = p x 100% p s ss Definition of relative humidity Although the Psychrometric Chart is scaled in terms of moisture content, this is for convience,we could determine vapour pressure from: g = 0.622 x ps pa
  • 8. — 8a Notes Notes 1–8aPage 8a1–8bPage Chapter 1 – Introduction to Psychrometry Comparision of percentage saturation and rh From the previous definition, we know that Wet-bulb temperature (twb ) The wet-bulb temperature, as the name implies, is the air temperature measured by a thermometer with a bulb covered with a muslin cloth sleeve and kept moist with distilled or clean water. It was devised as a means of assessing the humidity of the air, but as the actual reading is influenced by air movement, there are two variations of this temperature. 1. The Sling Wet-bulb The ‘sling wet-bulb’ temperature reading obtained in mov- ing air†1.10 – preferably above 2 m/s. It can be obtained by whirl- ing a ‘sling hygrometer’ or by using the more cumberson, but more accurate ‘Assman hygrometer’ which is fan-assisted. µ = gs x 100 % gss but using the above expression derived from moisture content, we can also express the percentage saturation as: µ = ps . (patm - pss ) x 100 % pss . (patm - ps ) Compare this to the definition of relative humidity: rh (φ) = ps x 100 % pss Since patm is very much bigger than ps or pss , then the relative humidity is very nearly equal to the percentage saturation. i.e. j Although relative humidity and percentage saturation are useful guides to comfort, it is not always practical to measure them directly. In fact measurement of humid air has always been a problem and the most practical method is to use a wet-bulb thermometer†1.9 . See Notes See Notes VIDEOEO Sling Hygrometer Assman Hygrometer 2. The Screen Wet-bulb The screen wet-bulb tempera- ture is the reading obtained in still air. This is usually used for mete- orological data and is obtained from a wet-bulb thermometer in- stalled into a ‘Stevenson Screen’ (from which this type of meas- urement gets its name). This is a slatted enclosure, designed to screen direct radiation from the instruments, but equipped with wet and dry-bulb thermometers and maximum and minimum ther- mometers. Of the two methods of reading wet-bulb, the sling reading is considered to be more accurate and is therefore preferred by air-conditioning engineers.
  • 9. — 9a Notes Notes 1–9aPage 9a1–9bPage Chapter 1 – Introduction to Psychrometry The Psychrometric Equation The psychrometric equation links the dry-bulb and the wet- bulb temperatures to their corresponding vapour pressures and to the atmospheric pressure. Consider air flowing across the bulb of a wet-bulb ther- mometer: At the surface of the muslin sleeve the air is considered to be at saturation moisture content (gss ’)†1.11 , so that the latent heat gain is proportional to the difference in moisture content between the film of air surrounding the muslin sleeve and the surrounding air, i.e. to ( gss ’ – gs ). Similary, the sensible heat lost is proportional to the tem- perature difference between the bulb and the ambient tempera- ture, i.e. to (t – t’), and since one process is the cause of the other we may equate them as: B . (gss ’ - gs ) = C . (t - t’) – (equation 1) where B and C are constants which relate to surface area and latent heat. But from our earlier equation for moisture content, we known that: gs = 0.622 ps patm – ps and gss ’ = 0.622 pss ’ patm – pss ’ and since ps and pss ’ are both very small compared to patm we may re-write these equations more simply as: g = 0.622 ps and gss ’ = 0.622 pss ’ patm patm Hence by substituting these expressions for moisture content into our equation 1, we get: 0.622 . B . (pss ’ – ps ) = C . (t – t’) patm From which we obtain: ps = pss ’ – patm . A . (t – t’). where A is known as the psychrometric constant and the differ- ence between the dry-bulb and the wet-bulb temperatures (t – t’) is known as the wet-bulb depression. See Notes Wet-bulb thermometer 123123123123 123 123123 20 0 20 air-flow muslin sleeve ambient air with properties: t, ps , gs air around muslin sleeve with properties: t’, pss ’, gss ’ Moisture will be evaporated from the muslin cloth sleeve around the bulb and will be taken up (associated) with the sur- rounding air. For this evaporation to take place heat must be supplied and this can only come from the surrounding air, i.e the latent heat of evaporation gained by the moisture on the surface of the muslin as it associates with the air, must equal the sensible heat lost from the surrounding air, in other words there must be a drop in the wet-bulb temperature to compensate for the increase in mosture content to the air around it.
  • 10. — 10a Notes Notes 1–10aPage 10a1–10bPage Chapter 1 – Introduction to Psychrometry Now the rate of moisture evaporation is different if the air is above or below freezing point (0°C) and between still and moving air (a standard speed of 2 m/s is used, but between about 2 m/s and 20 m/s the effect of air velocity is practically constant). Different values of the psychrometric constant are therefore quoted to cater for these conditions: Dew-point temperature (tdp ) The dew-point temperature is a very important property in air-conditioning†1.12 as it determines if water will be condensed from air when it is cooled. This occurs when a sample of air is cooled to the point where its vapour pressure reaches its satu- rated vapour pressure. For example, suppose air is being cooled at constant vapour pressure (i.e. constant moisture content). Even- tually, the temperature of the air will reach a point where the air is fully saturated (on our psychrometric chart – the ‘saturation line) and if the temperature drops lower than this point, water vapour will begin to condense. This point in known as the dew-point temperature (tdp ) and again can be represented on our psychrometric chart (click adjacent symbol). dry-bulb temperature moisturecontent 100% saturation Lines of constant wet-bulb temperature Lines of Constant Wet-bulbTemperature Psychro Chart Psychrometric Constants Sling: A = 6.66 x 10- 4 (K - 1 ) for t’ greater than 0 °C A = 5.94 x 10 - 4 (K - 1 ) for t’ less than 0 °C Screen: A = 7.99 x 10 - 4 (K - 1 ) for t’ greater than 0 °C A = 7.20 x 10 - 4 (K - 1 ) for t’ less than 0 °C Wet-bulb temperature is also shown on a psychrometeric chart and to assist with humidification processes (those which increase the moisture content), they are shown as lines of con- stant wet-bulb temperature (click adjacent symbol). Note: When working with the psychrometric equation, it is im- portant to remember that the saturated vapour pressure (pss ’) is taken at the wet-bulb temperature. See Notes Psychro Chart temperature moisturecontent 100% saturation t ga A dp dew-point temperature of air at condition A Dew-pointTemperature We should also realise that moist air does not need to be cooled to its dew-point for condensation to occur. Any surface with a temperature below the dew-point of the moist air will, of course, get wet and it is important to appreciate this when trying to avoid problems of condensation.
  • 11. — 11a Notes Notes 1–11aPage 11a1–11bPage Chapter 1 – Introduction to Psychrometry Specific enthalpy (h) Enthalpy (see Thermofluids Refresher, page C-5a) is a measure of energy, but although in psychrometry it is only the heat energy which is of interest, this is still referred to an enthalpy. Enthalpy is an extensive property, i.e its value depends upon the amount of substance present. An intensive property is therefore more useful since it does not depend upon the amount of mate- rial present. It is usually obtained by dividing the extensive prop- erty by its mass and is then known as specific property. Thus the specific enthalpy (h), is a measure of the heat energy (sensible and latent) of 1 kg of dry air plus its associated water vapour (measured in units of kJ/kg) relative to zero°C and zero moisture content. To calculate the specific enthalpy for an air sample we can use Dalton’s Law of Partial Pressures, i.e., h = h1 + h2 + h3 where the specific enthalpy for each part of the air-mixture is given by: h = mass x specific heat x ∆t. Thus for example, to calculate the specific enthalpy for air at a dry-bulb temperature of 20°C and a moisture content of 0.005 kg/kg, we can proceed as follows: Taking as our sample, 1 kg of dry air and its associated moisture content, the enthalpy of the dry air is given by: h1 = 1 x 1.005 x 20 = 20.1 kJ/kgK, where 1 is the mass of dry air, 1.005 is the specific heat of dry air and 20 is the air temperature relative to 0°C. similarly the sensible heat energy of the moisture content is given by: h2 = 0.005 x 1.89 x 20 = 0.189 where 0.005 is the moisture content 1.89 is the specific heat of water vapour and 20 is the air temperature relative to 0°C. Finally, the water vapour is considered to have evaporated at 0°C. We therefore have to include the latent heat of evaporation for the moisture content. Thus the latent heat energy of the moisture content is given by: h3 = 0.005 x 2501 = 12.505 where 0.005 is the moisture content and 2501 is the latent heat of evaporation at 0°C†1.13 . Thus the total enthalpy is given by h1 + h2 + h3 = 20.1 + 0.189 + 12.505 = 32.794 = 32.8 kJ/kg However, specific enthalpy can be determined much more quickly by direct reading from the psychrometric chart. Enthalpy scales are located ‘around the edges’ of the chart (click adjacent symbol), and there are no lines of constant enthalpy. To therefore obtain the specific enthalpy of an air condi- tion, a straight edge is used to join the corresponding enthalpy marks above to 100% saturation line with those on either the bottom, or the right-hand side of the chart (click on adjacent video symbol). Psychro Chart VIDEOEO specific enthalpy specificenthalpy Specific Enthalpy at edges of chart ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ See Notes
  • 12. — 12a Notes Notes 1–12aPage 12a1–12bPage Chapter 1 – Introduction to Psychrometry See Notes Psychro Chart In addition to the temperatures already noted, the following psychrometric parameters may also be required. Specific volume (v) The specific volume, is the volume of unit mass of dry air at a given temperature normally expressed as m3 /kg and is also shown in the psychrometric chart (click adjacent symbol). Note: that the specific volume is a measure of dry air, since the addi- tion of any associated water vapour has no effect on the volume (Dalton’s Law). Thus, with the exception of vapour pressure and saturation vapour pressure, all these psychrometric parameters are brought together on the psychrometric chart, from which any two are suf- ficient to indentify an air condition, the others then being read from the chart as required (see chart overleaf). In practice only two combinations†1.15 are used; dry-bulb temperature moisturecontent 100% saturation Lines of constant volume Lines of Constant Volume Density (ρρρρρ) The density of air is taken for a moist air sample and there- fore includes the mass of the associated water vapour. The spe- cific volume however, is defined in terms of dry air and thus the specific volume is not the reciprocal of density. The exact relationship is given by: ρ = (1 + g) v In practice however, the difference is very small and can be ignored†1.14 . dry-bulb (tdb ) and wet-bulb (twb ) temperature for measurements and dry-bulb temperature (tdb ) and percentage saturation (µµµµµ) [or relative humidity (rh)] for specifications. See Notes
  • 13. 90 80 70 60 50 40 30 20 PERCENTAGE SATURATION 0.75 0.80 0.85 0.90 SPECIFIC VOLUME m 3 /kg -10 -5 0 5 10 15 20 25 30 35 40 45 50 55 60 DRY – BULB TEMPERATURE ˚C 30 25 20 15 10 5 0 -5 -10 W ET-BULB TEM PERATURE ˚C (SLING ) 0.000 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.010 0.011 0.012 0.013 0.014 0.015 0.016 0.017 0.018 0.019 0.020 0.021 0.022 0.023 0.024 0.025 0.026 0.027 0.028 0.029 0.030 MOISTURECONTENTkg/kg -10 -5 0 5 10 15 -20 25 30 35 40-20 25 30 35 40 -45 50 55 60 65 SPECIFIC ENTHALPY kJ/kg 70758085 9590100105110 120115125130135135140 -10 -5 0 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85 90 95 100 105 110 105 120 125 130 135 140 SPECIFIC ENTHALPY kJ/kg SENSIBLE/TOTAL HEAT RATIO FORWATER ADDED AT 30˚C 0.1 0 0 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 BASED ON A BAROMETRIC PRESSURE OF 101.325 kPa CIBSE PSYCHROMETRIC CHART svp g rh% sat wb dew h v
  • 14. — 14a Notes Notes 1–14aPage 14a1–14bPage Chapter 1 – Introduction to Psychrometry Quick Revision Study Guide 1 The following questions are intended as a quick study question- naire to ensure you have grasped the general principles of this chapter. It is intended that your answers should be, short-phrased, quick answers or sketches to the questions. For suggested solutions to these questions, please refer to the Denco Website: www. denco.co.uk 1. 0.01 kg of steam with a specific enthalpy of 2,700 kJ/kg is mixed with 2.0 kg of dry air with a specific enthalpy of 20 kJ/kg. What is the specific enthalpy of the mixture? 2. Moist air has a dry-bulb temperature of 30°C, and a wet-bulb temperature of 20°C. Use a Psychrometric Chart to find a. The percentage saturation b. The moisture content c. The enthalpy d. The specific volume e. The dew-point temperature 3. Moist air at 25°C dry-bulb and 50% saturation, undergoes a process so that its condition is changed to 40°C dry- bulb and 30% saturation. Use a Psychrometric Chart to determine the change in specific enthalpy for the process. 4. The air inside a room during winter is at 20°C db and 40% saturation. If the temperature of the inside surface of a window is 9°C, will condensation form on the window glass? 5. A sling psychrometer measured the dry and wet-bulb temperatures of moist air as 27°C and 19°C respectively. Determine the moisture content from the relevant equation, given that: (i) pss at 19°C is 2.196 kPa, (ii) the psychrometric constant is 6.66 x 10-4 K-1
  • 15. — 15a Notes Notes 1–15aPage 15a1–15bPage Chapter 1 – Introduction to Psychrometry Chapter Notes †1-1: Air; is a mixture containing a group of gases of nearly constant pro- portions (% of atmosphere): Nitrogen (N2 ) 78.804 Methane (CH4 ) 0.0002 Oxygen (O2 ) 20.964 Krypton (Kr) 0.000114 Argon (Ar) 0.934 Hydrogen (H2 ) 0.00005 Neon (Ne) 0.0018 Nitrous Oxide (N2 O) 0.00005 Helium (He) 0.000524 Xenon (Xe) 0.0000087 and a group of gases present in proportions, variable both in time and space (% of atmosphere): Water Vapour (H2 O) 0 – 7 Carbon Dioxide (CO2 ) 0.01 – 0.1 (Average about 0.032) Ozone (O3 ) 0 – 0.01 Sulphur Dioxide (SO2 ) 0 – 0.0001 Nitrogen Dioxide (NO2 ) 0 – 0.000002 (Ref Encylopaedia Britannica CD-ROM, 1998 Edition). †1-2: Pressure; force per unit area, i.e. the force spread over a particular area, is measured in newtons and area in square metres. So pressure is measured in newtons per square metre but it can also be meas- ured in pascal (symbol Pa, where 1 Pa = 1 N/m2 ). Traditionally, it has also been common to express atmospheric pressure in units of bar or millibar, where 10 bar = 105 Pa, (Bar: from the Greek meaning weight, thus a ‘barometer’ [a word again derived from the Greek meaning weight + measure], is an instrument to measure the weight or pressure of the atmosphere). †1.3: Subscripts; it is normal to apply the following subscripts: s refers to water vapour (steam), eg Ps a refers to dry air, eg Pa ss refers to a saturated condition for water vapour in air, eg Pss †1.4: Internal Energy; is the molecular energy possesed by a material and includes the kinetic energy of the molecules due to vibration and the potential energy associated with the forces between them. Two terms can be used as a measure of this energy - the Internal Energy (symbol: U; unit:J) and the Specific Internal Energy (symbol: u; unit: J/kg). †1.5: Saturated Vapour Pressure vs Temperature; there is no simple relationship between temperature and saturated vapour pressure. The following equations have been developed by the National Engineering Laboratory as close curve fits to empirically measured data: For water above 0°C Log10 Pssw = 28.59 - 8.2 log10 T + 0.00248 T - 3142 T where Pssw is the saturated vapour pressure (bar) of vapour over water at an absolute temperature of T (K). For ice below 0°C Log10 Pssi = 10.538 - 2664 T where Pssw is the saturated vapour pressure (bar) of vapour over ice at an absolute temperature of T (K). †1.6: Moisture Content; is really a misnomer since what we are really referring to is ‘va- pour’ content, but the term has used by the industry as such for many years and so we just have to accept the inaccuracy of the wording.
  • 16. — 16a Notes Notes 1–16aPage 16a1–16bPage Chapter 1 – Introduction to Psychrometry †1.7: Relative Humidity - to a Base of Pressure; you will note that the relative humidity is based upon pressure, not mass of water vapour and is the traditional method of stating humidity as the ‘sling psychrometer’ (see page 1-8b) gave a meas- ure of vapour pressure. †1.8: Atmospheric pressure; patm = pa + ps †1.9: Psychrometer; the word ‘Psychrometer’ is originally from the Greek meaning ‘cold’ + ‘meter’, i.e. literally meaning a measurer of cold. Its current meaning is two thermometers, mounted on the same scale, with indications of wet-bulb and dry-bulb temperatures. Hence the word ‘Psychrometry’ is the determination of the degree of humidity in the atmosphere by means of a psychrometer and is therefore used to define the study of atmospheric air and its asso- ciated water vapour. †1.10: Use of Wet-bulb in Air Conditioning Duct; a sling wet-bulb reading may also be obtained by installing a wet-bulb thermometer in a duct through which air is flowing at a reasonable velocity. †1.11 Note the use of the dash ( ’ ) symbol to indicate that the reading is a wet-bulb reading. †1.12 Dew-point Instruments; there are commercial instruments which can measure the dew- point temperature directly. However, it is more usual to obtain a value by reference to tables of humid air properties, or to deter- mine its value from the psychrometric chart using the measure- ments of other air properties. †1.13: Latent heat; values for temperatures other than zero °C, can be found from standard tables for the ‘Thermodynamic Properties of Saturated Liquid Water and Dry Saturated Steam’, more commonly known as ‘Steam Tables’. †1.14: Air Density and Specific Volume; Although the difference between air density and the reciprocal of specific volume is small, it should be recognised that a differ- ence does exist where this relates to different areas of work. For example, when measuring air-flow rates through pressure drop devices, it is usual to use air density. On the other hand, for air- conditioning load calculations, it is usual to use specific volume. †1.15: CIBSE psychrometric chart; the CIBSE psychrometric chart is strictly correct only for a total pressure of 101.325 kPa (i.e standard atmospheric pressure). Charts are available for other pressures, or correction factors may be used such as those quoted in the CIBSE Guide C1. In addition, the principal axes of the chart are not, as is often assumed, dry-bulb temperature and moisture content, but enthalpy and moisture content. If you look carefully at a com- mercial psychrometric chart, you will see that the dry-bulb tem- perature lines are not quite parallel, nor vertical.