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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3554
BEHAVIOR OF REINFORCED CEMENT CONCRETE MULTISTOREY BUILDING UNDER
BLAST LOADING
Prasad R Gayake1, Swati S Ghuge2
1Assistant Professor, ME Structure, Department of Civil Engineering, DYPSOE, Lohegaon, Pune, Maharashtra, India
2Assistant Professor, Assistant Professor, Department of Civil Engineering, JCOE, Kuran, Pune, Maharashtra, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract - A critical study is presented in this report to
estimate the blast loading and its dynamic effects on various
component of MDOF structure. This study could be done
analytically by developing the MATLAB codes for MDOF
systems. However the analytical findings of MATLABprogram
results for some standard cases are going to verify over the
finite element software. Two models of MDOF fixed base
system with and without blast loading is being considered for
the study. The subsurface blast explosion is only being
considered for the study over MATLAB, However the surface
and subsurface blast explosion is being considered for the
study of 3D building over FE software package. The positive
impulsive triangular load is only being consideredforthetime
history analysis. For the present study the materialbehavioris
restricted to linear elastic only.
The mathematical formulation of MDOF systems aresolved by
using New mark Beta implicit step bystepintegrationmethod.
The entire study is focused on time domain form only. The
structural output results are measured in terms of structural
displacement, absolute acceleration, storey shear force and
base shear. The analytical investigation is being carried out
for the blast load parametric prediction. In the present study,
the effective blast resistant technique for the protection of
structural components could also been suggested.
Keyword’s: - MDOF, Blast Loading, Blast resistance
techniques, SAAP 2000 NL, MATLAB
1.INTRODUCTION
An explosion as a very fast chemical reaction during which a
rapid release of hot gases and energy takes place. During
explosion in air the hot gases that are produced expand in
order to occupy the available space, leading to wave type
propagation through space that is transmitted spherically
through an unbounded surrounding medium. This
phenomenon is termed as air burst. A schematic
representation of blast load that occurs very close to ground
surface and termed as surfaceburst.Inthepresentstudy, the
surface and subsurface blast phenomenon is studied. The
phenomenon lasts only for some milliseconds and it results
in the production of very high temperatures and pressures
capable to cause catastrophic damage to structures and
human life. Several factors govern the magnitude of blast
load on structure during an explosive detonation namely
charge weight, standoff distance, geometric configurationof
structure and orientationof structure.The powerofthe blast
primarily depends on the charge weight and standoff
distance with the former expressed as the equivalent weight
of Trinitrotoluene (TNT) that the building will encounter.
Range or stand-off is calculated with reference to the center
of gravity of the charge situated in the vehicle or the
structural member.
The common effects of blast load on structure includes
damage on the building's external and internal structural
frames, collapsing of walls, blowing out of large expanses of
windows, and shutting down of critical life-safety systems.
The major sources of blast load includes heinous terrorists’
activities and accidental explosions that results in large
dynamic loads.
Explosives and bombs are categorized as small medium and
high or large:
Small explosive devices up to 5 kg TNT, Medium explosive
devices up to 20 kg TNT
Large explosive devices and bombs up to 100 kg TNT, Very
large explosive devices and bombs up to 2500 kg TNT.
2. MATERIALS
2.1 Structure Details
In the present study a G+2 reinforced cement concrete
building considered under the blast load. thestoreyheight is
3.2 m. All beam sizes are 0.23*0.4 m & column sizes are
0.4*0.4 m. slab thickness are 0.12 m. the intensityofliveload
is . KN/m2. Used M25 grade of concrete.
For the present study the material behavior is restricted to
linear elastic only.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3555
Fig 1 : Line Plan
2.2 Methodology
2.2.1 Structure Modelling
Fig 2 Lumped Mass Model
Fig 3 3Dimensional Model
A Three dimensional has independent displacement at each
node and can simulate any tpye of behavior. Because of the
difficulties in modeling, verification. Verification and
numerical calculation, the three dimensional model has not
yet been used even in the most sophisticated design
practices. Figure 2.2.1(b) shows three dimensional frame
model which is especially useful to simulatetheresponses of
three dimensional effect such as,
1) Building with geometric configuration
2) Torsional response in the structure with eccentric
distribution of stiffness or mass, and
3) Earthquake motion in two directions or in skewed
direction etc.
A lumped mass model is simple and most frequently used in
early times for practical design of multi storey building. It
reduced the substantial amount of calculationandstoragein
comparison to two dimensional frame models. The soil
structure interactionmodel takesintoaccountthepossibility
of having different horizontal andvertical motionofsupport,
modifications of the natural period of structure due to
interaction with the soil, changing of the base motion in
comparison to the motion in free field, increasing the
effective damping due to difference between the tenancy of
regular structure motions.
2.2.2 Elastic Time History Analysis
A linear time history analysis overcomes all the
disadvantages of modal response spectrum analysis. One
interesting advantage of such procedure is that the relative
sign of response quantities are preserved in the response
histories.
2.2.3 Time History Method
A step by step procedure for analysis of frame by time
history method is as follows:-
The equation for MDOF system in matrix form can be
expressed as,
[m] {Ẍ}+ [c] {Ẋ} + [k] {X} = - Ẍg (t) [m] {I}
Where,
[M] = Mass Matrix
[K] = Stiffness Matrix
[C] = Damping Matrix
{I} = Unit Vector
Ẍg (T) = Ground Acceleration.
The solution of equation of motion for any specifiedforces is
difficult to obtain mainly to coupling of the variables {X} in
the physical coordinates In a modal analysis a set of normal
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3556
coordinates i.e. principal coordinates is defined, such that,
when expressed in those coordinates, the equations of
motion become uncoupled The physical coordinates{X} may
be related with normal or principal coordinates (q)fromthe
transformation expression as,
{X}= [Φ] { q }
[Φ] is the modal matrix,
Time derivatives of {X} are,
{Ẋ} = [Φ] { } {Ẍ} = [Φ] { }
Substituting the time derivatives in the equation of motion,
and pre-multiplying by [Φ]T result in,
[Φ]T[m][Φ] { } + [Φ]T[c] [Φ] { } + [Φ]T[k] [Φ] { q }= (- Ẍg (t)
[Φ]T[ m] {I})
More clearly it can be represented as follows,
[M]{ }+ [C] { } + [K] { q }= {Peff (t)}
Where,
[M] = [Φ]T[m][Φ]
[C] = [Φ]T[c] [Φ]
[K ] = [Φ]T[k] [Φ]
{Peff (t)}= (- Ẍg (t) [Φ]T[ m] {I}
[M ],[C] and [K] are the diagonal modal mass matrix modal
damping matrix, and stiffness matrix, respectively, and {peff
(t)}is the effective modal force vector.
3. RESULTS
3.1 Surface Blast Loading
3.1.1 3-Dimensional Model
a) Axial Column Time History Analysis
b) Uniaxial column time history analysis
c) Biaxial column time history analysis
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3557
d) Top storey Displacement time history
e) Top storey Acceleration time history
f) Base shear force
Table 1- Base Reactions
OutputCase CaseType StepType GlobalFX
Text Text Text KN
P LinModHist Max 254.705
P LinModHist Min -436.819
3.1.2 Lumped mass model
a) Top storey Displacement time history
b) Top storey Acceleration time history
c) Base Shear Force
Table 2 – Base Reactions
OutputCase CaseType StepType GlobalFX
Text Text Text KN
P LinModHist Max 639
P LinModHist Min -478
3.1.3 Comparison between 3-D model and Lumped
mass model
a) Top storey Acceleration time history
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3558
b) Top storey Acceleration time history
3.2: Subsurface blast loading:
3.2.1: 3- Dimensional model:
a) Axial column time history analysis
b) Uniaxial column time history analysis
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3559
c) Biaxial column time history analysis d) Top storey Displacement time history
e) Top storey Acceleration time history
f) Base shear force
Table 3 Base Reactons
OutputCase CaseType StepType GlobalFX
Text Text Text KN
P LinModHist Max 3702
P LinModHist Min -2895
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3560
3.2.2: Lumped mass model
a) Top storey Displacement time history
b) Top storey Acceleration time history
c) Base shear force
Table 4 Base Reactions
OutputCase CaseType StepType GlobalFX
Text Text Text KN
P LinModHist Max 5604
P LinModHist Min -5002
3.2.3: MATLAB Programming
a) Top storey Displacement time history
b) Top storey Acceleration time history
c) Base shear force
Table 5 Base Reactions
OutputCase CaseType StepType GlobalFX
Text Text Text KN
P LinModHist Max 5604
P LinModHist Min -5002
3.2.3: Comparison between3-DmodelandLumped
mass model
a) Top storey Displacement time history
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3561
b) Top storey Acceleration time history
4. CONCLUSIONS:
Blast load for close explosion under subsurface and surface
was determined and simulated on a model building using
SAP 2000NL. The surface blast loading time history is
generated using W.E. Baker (1973) and apply to three
dimensional buildingmodel aswell aslumpedmassmodel in
SAP 2000NL, However the subsurface blast ground
acceleration is calculated as per the formulation adopted by
C. H. Dowdling (1985) and then it is apply to 3D building
model in SAP 2000NL. The MATLAB program is also
prepared for lumped mass model subjected underground
acceleration due to subsurface blast. Theresultsarenotedin
the form of displacement time history, acceleration time
history, and base reaction time history for lumped mass
model. On the other hand for 3D building, the results were
obtained in the form of joint displacement time history,joint
acceleration time history, joint base reaction time history,
element shear force/axial force time history and element
bending moment time history. Blast is an impulsive load but
its effect is remaining over the structure for up to 5 second,
thereafter it is diminishes very rapidly. Blast produces large
amount of base shear force and moment in building which
cannot be ignored while designing the structural members.
The structure is vibrating much severely during the initial
phase of blast. Here in the present study only linear elastic
structure is considered, the plastic deformation is not being
considered, otherwise there may have possibility that
structure undergoes in plastic stage and failed. In surface
blast, the acceleration and displacement of lumped mass
model is getting 12% less than the 3D building model. In
subsurface blast loading, the acceleration and displacement
of lumped mass model is getting 33% less than the 3D
building model. The base shear force of three dimensional
building is 33% less than the lumped mass building model.
The distributed Rayleigh mass is normallyconsideredby the
Finite element software during analysis, so therefore the
results of 3D model and lumped mass model could not
match. Here in the present study only multi storey building
system is considered in which blast has induced 2g to 4g
accelerations in buildings depending upon the blast charge
weight and exposed distance of structure from the blastsite,
however in high rise building this effect could be much
severe.
REFERENCES:
1) Ashalekshmi K G, Dr. Subha K,( 05 Apr-2018) A
Review On The Study Of The Response Of Ground Blast
Loads On Rcc Structures International Research Journal
Of Engineering And Technology (Irjet), E-Issn: 2395-
0056, P-Issn: 2395-0072.
2)Ashish Kumar Tiwary, Aditya Kumar Tiwary, Anil
Kumar, (2015) Blast Loading Effects on Steel Columns,
IOSR Journal of Mechanical and Civil Engineering(IOSR-
JMCE) e-ISSN: 2278-1684,p-ISSN:2320-334X.PP17-22.
Baker, W.E. (1973) Explosions inAir,UniversityofTexas
Press, Austin and London.
3)Boyina Sita Rama Krishna,Jinka Chandra Sekhar,( 6
June 2018) Blast Load Analysis And Effect On High Rise
Structure, International journal on civil engineeringand
technology,Volume 9.
4)Dowding, C.H. (1985) Blast Vibration Monitoring and
Control, vol. 297.Prentice-Hall, Englewood Cliffs.
5)Hrvoje Draganic, Vladimir Sigmund,(August 2012)
Blast Loading On Structures, Issn 1330-3651udc/Udk
624.01.04:662.15 , Article In Tehnicki Vjesnik.
6)Mir M. Ali, (2002) Protective design of concrete
buildings under blast loading,WITPress,AshurstLodge,
Southampton, SO40 7AA, UK.
7)Mohammed Asra Jabeen, Dr Manohar.G,Prashanth.P.
(2017) Optimum Design of Multi-Storied Building
Against Blast Loads, National Conference Proceeding
Ntsetfeb 2018 | Issn:2320-2882National Conference On
Trends In Science, Engineering & Technology By
Matrusri Engineering College & Ijcrt.
8)Muhammed Zain Kangda and Sachin Bakre,(2016),
Positive Phase Blast Effects on Base Isolated Structures,
Manuscript No: AJSE-D-18-02611R1.

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IRJET- Behavior of Reinforced Cement Concrete Multistorey Building under Blast Loading

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3554 BEHAVIOR OF REINFORCED CEMENT CONCRETE MULTISTOREY BUILDING UNDER BLAST LOADING Prasad R Gayake1, Swati S Ghuge2 1Assistant Professor, ME Structure, Department of Civil Engineering, DYPSOE, Lohegaon, Pune, Maharashtra, India 2Assistant Professor, Assistant Professor, Department of Civil Engineering, JCOE, Kuran, Pune, Maharashtra, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract - A critical study is presented in this report to estimate the blast loading and its dynamic effects on various component of MDOF structure. This study could be done analytically by developing the MATLAB codes for MDOF systems. However the analytical findings of MATLABprogram results for some standard cases are going to verify over the finite element software. Two models of MDOF fixed base system with and without blast loading is being considered for the study. The subsurface blast explosion is only being considered for the study over MATLAB, However the surface and subsurface blast explosion is being considered for the study of 3D building over FE software package. The positive impulsive triangular load is only being consideredforthetime history analysis. For the present study the materialbehavioris restricted to linear elastic only. The mathematical formulation of MDOF systems aresolved by using New mark Beta implicit step bystepintegrationmethod. The entire study is focused on time domain form only. The structural output results are measured in terms of structural displacement, absolute acceleration, storey shear force and base shear. The analytical investigation is being carried out for the blast load parametric prediction. In the present study, the effective blast resistant technique for the protection of structural components could also been suggested. Keyword’s: - MDOF, Blast Loading, Blast resistance techniques, SAAP 2000 NL, MATLAB 1.INTRODUCTION An explosion as a very fast chemical reaction during which a rapid release of hot gases and energy takes place. During explosion in air the hot gases that are produced expand in order to occupy the available space, leading to wave type propagation through space that is transmitted spherically through an unbounded surrounding medium. This phenomenon is termed as air burst. A schematic representation of blast load that occurs very close to ground surface and termed as surfaceburst.Inthepresentstudy, the surface and subsurface blast phenomenon is studied. The phenomenon lasts only for some milliseconds and it results in the production of very high temperatures and pressures capable to cause catastrophic damage to structures and human life. Several factors govern the magnitude of blast load on structure during an explosive detonation namely charge weight, standoff distance, geometric configurationof structure and orientationof structure.The powerofthe blast primarily depends on the charge weight and standoff distance with the former expressed as the equivalent weight of Trinitrotoluene (TNT) that the building will encounter. Range or stand-off is calculated with reference to the center of gravity of the charge situated in the vehicle or the structural member. The common effects of blast load on structure includes damage on the building's external and internal structural frames, collapsing of walls, blowing out of large expanses of windows, and shutting down of critical life-safety systems. The major sources of blast load includes heinous terrorists’ activities and accidental explosions that results in large dynamic loads. Explosives and bombs are categorized as small medium and high or large: Small explosive devices up to 5 kg TNT, Medium explosive devices up to 20 kg TNT Large explosive devices and bombs up to 100 kg TNT, Very large explosive devices and bombs up to 2500 kg TNT. 2. MATERIALS 2.1 Structure Details In the present study a G+2 reinforced cement concrete building considered under the blast load. thestoreyheight is 3.2 m. All beam sizes are 0.23*0.4 m & column sizes are 0.4*0.4 m. slab thickness are 0.12 m. the intensityofliveload is . KN/m2. Used M25 grade of concrete. For the present study the material behavior is restricted to linear elastic only.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3555 Fig 1 : Line Plan 2.2 Methodology 2.2.1 Structure Modelling Fig 2 Lumped Mass Model Fig 3 3Dimensional Model A Three dimensional has independent displacement at each node and can simulate any tpye of behavior. Because of the difficulties in modeling, verification. Verification and numerical calculation, the three dimensional model has not yet been used even in the most sophisticated design practices. Figure 2.2.1(b) shows three dimensional frame model which is especially useful to simulatetheresponses of three dimensional effect such as, 1) Building with geometric configuration 2) Torsional response in the structure with eccentric distribution of stiffness or mass, and 3) Earthquake motion in two directions or in skewed direction etc. A lumped mass model is simple and most frequently used in early times for practical design of multi storey building. It reduced the substantial amount of calculationandstoragein comparison to two dimensional frame models. The soil structure interactionmodel takesintoaccountthepossibility of having different horizontal andvertical motionofsupport, modifications of the natural period of structure due to interaction with the soil, changing of the base motion in comparison to the motion in free field, increasing the effective damping due to difference between the tenancy of regular structure motions. 2.2.2 Elastic Time History Analysis A linear time history analysis overcomes all the disadvantages of modal response spectrum analysis. One interesting advantage of such procedure is that the relative sign of response quantities are preserved in the response histories. 2.2.3 Time History Method A step by step procedure for analysis of frame by time history method is as follows:- The equation for MDOF system in matrix form can be expressed as, [m] {Ẍ}+ [c] {Ẋ} + [k] {X} = - Ẍg (t) [m] {I} Where, [M] = Mass Matrix [K] = Stiffness Matrix [C] = Damping Matrix {I} = Unit Vector Ẍg (T) = Ground Acceleration. The solution of equation of motion for any specifiedforces is difficult to obtain mainly to coupling of the variables {X} in the physical coordinates In a modal analysis a set of normal
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3556 coordinates i.e. principal coordinates is defined, such that, when expressed in those coordinates, the equations of motion become uncoupled The physical coordinates{X} may be related with normal or principal coordinates (q)fromthe transformation expression as, {X}= [Φ] { q } [Φ] is the modal matrix, Time derivatives of {X} are, {Ẋ} = [Φ] { } {Ẍ} = [Φ] { } Substituting the time derivatives in the equation of motion, and pre-multiplying by [Φ]T result in, [Φ]T[m][Φ] { } + [Φ]T[c] [Φ] { } + [Φ]T[k] [Φ] { q }= (- Ẍg (t) [Φ]T[ m] {I}) More clearly it can be represented as follows, [M]{ }+ [C] { } + [K] { q }= {Peff (t)} Where, [M] = [Φ]T[m][Φ] [C] = [Φ]T[c] [Φ] [K ] = [Φ]T[k] [Φ] {Peff (t)}= (- Ẍg (t) [Φ]T[ m] {I} [M ],[C] and [K] are the diagonal modal mass matrix modal damping matrix, and stiffness matrix, respectively, and {peff (t)}is the effective modal force vector. 3. RESULTS 3.1 Surface Blast Loading 3.1.1 3-Dimensional Model a) Axial Column Time History Analysis b) Uniaxial column time history analysis c) Biaxial column time history analysis
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3557 d) Top storey Displacement time history e) Top storey Acceleration time history f) Base shear force Table 1- Base Reactions OutputCase CaseType StepType GlobalFX Text Text Text KN P LinModHist Max 254.705 P LinModHist Min -436.819 3.1.2 Lumped mass model a) Top storey Displacement time history b) Top storey Acceleration time history c) Base Shear Force Table 2 – Base Reactions OutputCase CaseType StepType GlobalFX Text Text Text KN P LinModHist Max 639 P LinModHist Min -478 3.1.3 Comparison between 3-D model and Lumped mass model a) Top storey Acceleration time history
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3558 b) Top storey Acceleration time history 3.2: Subsurface blast loading: 3.2.1: 3- Dimensional model: a) Axial column time history analysis b) Uniaxial column time history analysis
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3559 c) Biaxial column time history analysis d) Top storey Displacement time history e) Top storey Acceleration time history f) Base shear force Table 3 Base Reactons OutputCase CaseType StepType GlobalFX Text Text Text KN P LinModHist Max 3702 P LinModHist Min -2895
  • 7. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3560 3.2.2: Lumped mass model a) Top storey Displacement time history b) Top storey Acceleration time history c) Base shear force Table 4 Base Reactions OutputCase CaseType StepType GlobalFX Text Text Text KN P LinModHist Max 5604 P LinModHist Min -5002 3.2.3: MATLAB Programming a) Top storey Displacement time history b) Top storey Acceleration time history c) Base shear force Table 5 Base Reactions OutputCase CaseType StepType GlobalFX Text Text Text KN P LinModHist Max 5604 P LinModHist Min -5002 3.2.3: Comparison between3-DmodelandLumped mass model a) Top storey Displacement time history
  • 8. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 3561 b) Top storey Acceleration time history 4. CONCLUSIONS: Blast load for close explosion under subsurface and surface was determined and simulated on a model building using SAP 2000NL. The surface blast loading time history is generated using W.E. Baker (1973) and apply to three dimensional buildingmodel aswell aslumpedmassmodel in SAP 2000NL, However the subsurface blast ground acceleration is calculated as per the formulation adopted by C. H. Dowdling (1985) and then it is apply to 3D building model in SAP 2000NL. The MATLAB program is also prepared for lumped mass model subjected underground acceleration due to subsurface blast. Theresultsarenotedin the form of displacement time history, acceleration time history, and base reaction time history for lumped mass model. On the other hand for 3D building, the results were obtained in the form of joint displacement time history,joint acceleration time history, joint base reaction time history, element shear force/axial force time history and element bending moment time history. Blast is an impulsive load but its effect is remaining over the structure for up to 5 second, thereafter it is diminishes very rapidly. Blast produces large amount of base shear force and moment in building which cannot be ignored while designing the structural members. The structure is vibrating much severely during the initial phase of blast. Here in the present study only linear elastic structure is considered, the plastic deformation is not being considered, otherwise there may have possibility that structure undergoes in plastic stage and failed. In surface blast, the acceleration and displacement of lumped mass model is getting 12% less than the 3D building model. In subsurface blast loading, the acceleration and displacement of lumped mass model is getting 33% less than the 3D building model. The base shear force of three dimensional building is 33% less than the lumped mass building model. The distributed Rayleigh mass is normallyconsideredby the Finite element software during analysis, so therefore the results of 3D model and lumped mass model could not match. Here in the present study only multi storey building system is considered in which blast has induced 2g to 4g accelerations in buildings depending upon the blast charge weight and exposed distance of structure from the blastsite, however in high rise building this effect could be much severe. REFERENCES: 1) Ashalekshmi K G, Dr. Subha K,( 05 Apr-2018) A Review On The Study Of The Response Of Ground Blast Loads On Rcc Structures International Research Journal Of Engineering And Technology (Irjet), E-Issn: 2395- 0056, P-Issn: 2395-0072. 2)Ashish Kumar Tiwary, Aditya Kumar Tiwary, Anil Kumar, (2015) Blast Loading Effects on Steel Columns, IOSR Journal of Mechanical and Civil Engineering(IOSR- JMCE) e-ISSN: 2278-1684,p-ISSN:2320-334X.PP17-22. Baker, W.E. (1973) Explosions inAir,UniversityofTexas Press, Austin and London. 3)Boyina Sita Rama Krishna,Jinka Chandra Sekhar,( 6 June 2018) Blast Load Analysis And Effect On High Rise Structure, International journal on civil engineeringand technology,Volume 9. 4)Dowding, C.H. (1985) Blast Vibration Monitoring and Control, vol. 297.Prentice-Hall, Englewood Cliffs. 5)Hrvoje Draganic, Vladimir Sigmund,(August 2012) Blast Loading On Structures, Issn 1330-3651udc/Udk 624.01.04:662.15 , Article In Tehnicki Vjesnik. 6)Mir M. Ali, (2002) Protective design of concrete buildings under blast loading,WITPress,AshurstLodge, Southampton, SO40 7AA, UK. 7)Mohammed Asra Jabeen, Dr Manohar.G,Prashanth.P. (2017) Optimum Design of Multi-Storied Building Against Blast Loads, National Conference Proceeding Ntsetfeb 2018 | Issn:2320-2882National Conference On Trends In Science, Engineering & Technology By Matrusri Engineering College & Ijcrt. 8)Muhammed Zain Kangda and Sachin Bakre,(2016), Positive Phase Blast Effects on Base Isolated Structures, Manuscript No: AJSE-D-18-02611R1.