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VViiddeeoo lleeccttuurreess ffoorr MMCCAA 
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55.. AANNAALLYYSSIISS OOFF IINNDDEETTEERRMMIINNAATTEE 
SSTTRRUUCCTTUURREESS BBYY FFOORRCCEE MMEETTHHOODD
5.1 ANALYSIS OOFF IINNDDEETTEERRMMIINNAATTEE SSTTRRUUCCTTUURREESS 
BBYY FFOORRCCEE MMEETTHHOODD -- AANN OOVVEERRVVIIEEWW 
 5.1 ANALYSIS OF INDETERMINATE STRUCTURES BY FORCE 
METHOD - AN OVERVIEW 
 5.2 INTRODUCTION 
 5.3 METHOD OF CONSISTENT DEFORMATION 
 5.4 INDETERMINATE BEAMS 
 5.5 INDETRMINATE BEAMS WITH MULTIPLE DEGREES OF 
INDETERMINACY 
 5.6 TRUSS STRUCTURES 
 5.7 TEMPERATURE CHANGES AND FABRICATION ERRORS
55..22 IINNTTRROODDUUCCTTIIOONN 
5.2 Introduction 
 While analyzing indeterminate structures, it is necessary to satisfy (force) 
equilibrium, (displacement) compatibility and force-displacement 
relationships 
 (a) Force equilibrium is satisfied when the reactive forces hold the structure 
in stable equilibrium, as the structure is subjected to external loads 
 (b) Displacement compatibility is satisfied when the various segments of the 
structure fit together without intentional breaks, or overlaps 
 (c) Force-displacement requirements depend on the manner the material of 
the structure responds to the applied loads, which can be 
linear/nonlinear/viscous and elastic/inelastic; for our study the behavior is 
assumed to be linear and elastic
55..22 IINNTTRROODDUUCCTTIIOONN ((CCoonntt’’dd)) 
 Two methods are available to analyze indeterminate structures, depending 
on whether we satisfy force equilibrium or displacement compatibility 
conditions - They are: Force method and Displacement Method 
 Force Method satisfies displacement compatibility and force-displacement 
relationships; it treats the forces as unknowns - Two methods which we will 
be studying are Method of Consistent Deformation and (Iterative 
Method of) Moment Distribution 
 Displacement Method satisfies force equilibrium and force-displacement 
relationships; it treats the displacements as unknowns - Two available 
methods are Slope Deflection Method and Stiffness (Matrix) method
5.3 METHOD OOFF CCOONNSSIISSTTEENNTT DDEEFFOORRMMAATTIIOONN 
 Solution Procedure: 
 (i) Make the structure determinate, by releasing the extra forces 
constraining the structure in space 
 (ii) Determine the displacements (or rotations) at the locations of 
released (constraining) forces 
 (iii) Apply the released (constraining) forces back on the structure 
(To standardize the procedure, only a unit load of the constraining force is 
applied in the +ve direction) to produce the same deformation(s) on 
the structure as in (ii) 
 (iv) Sum up the deformations and equate them to zero at the 
position(s) of the released (constraining) forces, and calculate the unknown 
restraining forces 
Types of Problems to be dealt: (a) Indeterminate beams; (b) 
Indeterminate trusses; and (c) Influence lines for indeterminate 
structures
5.4 IINNDDEETTEERRMMIINNAATTEE BBEEAAMMSS 
5.4.1 Propped Cantilever - Redundant vertical reaction released 
(i) Propped Cantilever: The structure is indeterminate to the first degree; 
hence has one unknown in the problem. 
(ii) In order to solve the problem, release the extra constraint and make 
the beam a determinate structure. This can be achieved in two 
different ways, viz., (a) By removing the vertical support at B, and 
making the beam a cantilever beam (which is a determinate beam); or (b) By 
releasing the moment constraint at A, and making the structure a simply 
supported beam (which is once again, a determinate beam).
5.4 IINNDDEETTEERRMMIINNAATTEE BBEEAAMMSS ((CCoonntt’’dd)) 
(a) Release the vertical support at B: 
x 
y 
P 
P 
C B 
B B 
DB = + 
DC 
L/2 L/2 L 
RB 
D¢BB=RB*fBB 
Applied in +ve 
direction 
The governing compatibility equation obtained at B is, 
DB 
+ D' 
BB = 0 
R f 
D+ ( ) ´ ( ) = 
0 
B B BB 
R / 
f 
From earlier analyses, 
 =-D 
B B BB 
3 2 
P L EI P L EI L B 
D=- +- ´ 
( / 2) /(3 ) [ ( / 2) /(2 )] ( / 2) 
3 3 
PL EI PL EI 
=- - 
/(24 ) /(16 ) 
3 
PL EI 
=- 
(5/ 48)( / ) 
f L3 /(3EI ) BB = 
R PL EI L EI P BB =-[-(5/ 48)( 3 / )]/[ 3 /(3 )]=(5/16) 
fBB = displacement per unit load (applied in +ve direction)
5.4 INDETERMINATE BEAM (Cont’d) 
5.4.2 Propped cantilever - Redundant support moment released 
L/2 P 
A B 
P 
Governing compatibility equation obtained at A is, 
+( )´( )= A A AA q M a , AA a= rotation per unit moment 
q 
A 
AA 
A M 
 =- 
a 
From known earlier analysis, (16 ) 
AA q =- [under a central concentrated 
2 
EI 
PL 
load] 
(1)[L /(3EI )] AA a =- 
This is due to the fact that +ve moment causes a –ve rotation 
M =-- [ PL2/(16EI)]/[ - 
L/(3EI)] 
A 
=- 
(3/16)PL 
L 
(b) Release the moment constraint at a: 
qA 
= 
A B 
Primary structure 
+ A B 
MA q¢A=MAaAA 
Redundant MA applied
5.4.3 OVERVIEW OF METHOD OF 
CONSISTENT DEFORMATION 
To recapitulate on what we have done earlier, 
I. Structure with single degree of indeterminacy: 
A B 
RB 
(a) Remove the redundant to make the structure determinate 
(primary structure) 
A B 
DBo 
(b) Apply unit force on the structure, in the direction of the 
redundant, and find the displacement 
fBB 
(c) Apply compatibility at the location of the removed redundant 
DB0 + fBB´RB = 0 
P 
P
5.5 INDETERMINATE BEAM WWIITTHH MMUULLTTIIPPLLEE DDEEGGRREEEESS 
OOFF IINNDDEETTEERRMMIINNAACCYY 
A 
w/u.l 
B C D E 
RB RC RD 
DB0 DC0 
DD0 
(a) Make the structure determinate (by releasing the supports at B, 
C and D) and determine the deflections at B, C and D in the 
direction of removed redundants, viz., DBO, DCO and DDO
(b) Apply unit loads at B, C and D, in a sequential manner and 
determine deformations at B, C and D, respectively. 
A 
B C D E 
fBB 
fCB fDB 1 
A 
B C D E 
fBC 
fCC fDC 
A 
1 
B C D E 
fBD 
fCD fDD 
1
(c ) Establish compatibility conditions at B, C and D 
DBO + fBBRB + fBCRC + fBDRD = 0 
DCO + fCBRB + fCCRC + fCDRD = 0 
DDO + fDBRB + fDCRC + fDDRD = 0
5.4.2 When support settlements occur: 
A 
B C D E 
DB DC DD Support settlements 
Compatibility conditions at B, C and D give the following equations: 
DBO + fBBRB + fBCRC + fBDRD = DB 
DCO + fCBRB + fCCRC + fCDRD = DC 
DDO + fDBRB + fDCRC + fDDRD = DD 
w / u. l.
55..55 TTRRUUSSSS SSTTRRUUCCTTUURREESS 
80 kN 
C 
60 kN 
D 
A B 
80 kN 
C 
60 kN 
D 
A 1 2 
B 
Primary structure 
(a) (a) Remove the redundant member (say AB) and make the structure 
a primary determinate structure 
The condition for stability and indeterminacy is: 
r+m>=<2j, 
Since, m = 6, r = 3, j = 4, (r + m =) 3 + 6 > (2j =) 2*4 or 9 > 8  i = 1
5.5 Truss Structures (Cont’d) 
(b)Find deformation Dalong AB: 
ABO D=S (FuL)/AE 
ABO 0ABF= Force in member of the primary structure due to applied 
0 load 
u= Forces in members due to unit force applied along AB 
AB(c) Determine fAB uABL 
=å 
deformation 2 
along AB due to unit load applied along 
AB: 
, 
AB 
AE 
(d) Apply compatibility condition along AB: 
DABO+fAB,ABFAB=0
(e) Determine the individual member forces in a particular 
member CE by 
FCE = FCE0 + uCE FAB 
where FCE0 = force in CE due to applied loads on primary structure 
(=F0), and uCE = force in CE due to unit force applied along AB (= 
uAB)
5.6 TEMPERATURE CCHHAANNGGEESS AANNDD FFAABBRRIICCAATTIIOONN 
EERRRROORR 
 Temperature changes affect the internal forces in a structure 
 Similarly fabrication errors also affect the internal forces in a 
structure 
(i) Subject the primary structure to temperature changes and 
fabrication errors. - Find the deformations in the redundant 
direction 
(ii) Reintroduce the removed members back and make the 
deformation compatible

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Video lectures for mca

  • 1. VViiddeeoo lleeccttuurreess ffoorr MMCCAA By: video.edhole.com
  • 2. 55.. AANNAALLYYSSIISS OOFF IINNDDEETTEERRMMIINNAATTEE SSTTRRUUCCTTUURREESS BBYY FFOORRCCEE MMEETTHHOODD
  • 3. 5.1 ANALYSIS OOFF IINNDDEETTEERRMMIINNAATTEE SSTTRRUUCCTTUURREESS BBYY FFOORRCCEE MMEETTHHOODD -- AANN OOVVEERRVVIIEEWW  5.1 ANALYSIS OF INDETERMINATE STRUCTURES BY FORCE METHOD - AN OVERVIEW  5.2 INTRODUCTION  5.3 METHOD OF CONSISTENT DEFORMATION  5.4 INDETERMINATE BEAMS  5.5 INDETRMINATE BEAMS WITH MULTIPLE DEGREES OF INDETERMINACY  5.6 TRUSS STRUCTURES  5.7 TEMPERATURE CHANGES AND FABRICATION ERRORS
  • 4. 55..22 IINNTTRROODDUUCCTTIIOONN 5.2 Introduction  While analyzing indeterminate structures, it is necessary to satisfy (force) equilibrium, (displacement) compatibility and force-displacement relationships  (a) Force equilibrium is satisfied when the reactive forces hold the structure in stable equilibrium, as the structure is subjected to external loads  (b) Displacement compatibility is satisfied when the various segments of the structure fit together without intentional breaks, or overlaps  (c) Force-displacement requirements depend on the manner the material of the structure responds to the applied loads, which can be linear/nonlinear/viscous and elastic/inelastic; for our study the behavior is assumed to be linear and elastic
  • 5. 55..22 IINNTTRROODDUUCCTTIIOONN ((CCoonntt’’dd))  Two methods are available to analyze indeterminate structures, depending on whether we satisfy force equilibrium or displacement compatibility conditions - They are: Force method and Displacement Method  Force Method satisfies displacement compatibility and force-displacement relationships; it treats the forces as unknowns - Two methods which we will be studying are Method of Consistent Deformation and (Iterative Method of) Moment Distribution  Displacement Method satisfies force equilibrium and force-displacement relationships; it treats the displacements as unknowns - Two available methods are Slope Deflection Method and Stiffness (Matrix) method
  • 6. 5.3 METHOD OOFF CCOONNSSIISSTTEENNTT DDEEFFOORRMMAATTIIOONN  Solution Procedure:  (i) Make the structure determinate, by releasing the extra forces constraining the structure in space  (ii) Determine the displacements (or rotations) at the locations of released (constraining) forces  (iii) Apply the released (constraining) forces back on the structure (To standardize the procedure, only a unit load of the constraining force is applied in the +ve direction) to produce the same deformation(s) on the structure as in (ii)  (iv) Sum up the deformations and equate them to zero at the position(s) of the released (constraining) forces, and calculate the unknown restraining forces Types of Problems to be dealt: (a) Indeterminate beams; (b) Indeterminate trusses; and (c) Influence lines for indeterminate structures
  • 7. 5.4 IINNDDEETTEERRMMIINNAATTEE BBEEAAMMSS 5.4.1 Propped Cantilever - Redundant vertical reaction released (i) Propped Cantilever: The structure is indeterminate to the first degree; hence has one unknown in the problem. (ii) In order to solve the problem, release the extra constraint and make the beam a determinate structure. This can be achieved in two different ways, viz., (a) By removing the vertical support at B, and making the beam a cantilever beam (which is a determinate beam); or (b) By releasing the moment constraint at A, and making the structure a simply supported beam (which is once again, a determinate beam).
  • 8. 5.4 IINNDDEETTEERRMMIINNAATTEE BBEEAAMMSS ((CCoonntt’’dd)) (a) Release the vertical support at B: x y P P C B B B DB = + DC L/2 L/2 L RB D¢BB=RB*fBB Applied in +ve direction The governing compatibility equation obtained at B is, DB + D' BB = 0 R f D+ ( ) ´ ( ) = 0 B B BB R / f From earlier analyses, =-D B B BB 3 2 P L EI P L EI L B D=- +- ´ ( / 2) /(3 ) [ ( / 2) /(2 )] ( / 2) 3 3 PL EI PL EI =- - /(24 ) /(16 ) 3 PL EI =- (5/ 48)( / ) f L3 /(3EI ) BB = R PL EI L EI P BB =-[-(5/ 48)( 3 / )]/[ 3 /(3 )]=(5/16) fBB = displacement per unit load (applied in +ve direction)
  • 9. 5.4 INDETERMINATE BEAM (Cont’d) 5.4.2 Propped cantilever - Redundant support moment released L/2 P A B P Governing compatibility equation obtained at A is, +( )´( )= A A AA q M a , AA a= rotation per unit moment q A AA A M =- a From known earlier analysis, (16 ) AA q =- [under a central concentrated 2 EI PL load] (1)[L /(3EI )] AA a =- This is due to the fact that +ve moment causes a –ve rotation M =-- [ PL2/(16EI)]/[ - L/(3EI)] A =- (3/16)PL L (b) Release the moment constraint at a: qA = A B Primary structure + A B MA q¢A=MAaAA Redundant MA applied
  • 10. 5.4.3 OVERVIEW OF METHOD OF CONSISTENT DEFORMATION To recapitulate on what we have done earlier, I. Structure with single degree of indeterminacy: A B RB (a) Remove the redundant to make the structure determinate (primary structure) A B DBo (b) Apply unit force on the structure, in the direction of the redundant, and find the displacement fBB (c) Apply compatibility at the location of the removed redundant DB0 + fBB´RB = 0 P P
  • 11. 5.5 INDETERMINATE BEAM WWIITTHH MMUULLTTIIPPLLEE DDEEGGRREEEESS OOFF IINNDDEETTEERRMMIINNAACCYY A w/u.l B C D E RB RC RD DB0 DC0 DD0 (a) Make the structure determinate (by releasing the supports at B, C and D) and determine the deflections at B, C and D in the direction of removed redundants, viz., DBO, DCO and DDO
  • 12. (b) Apply unit loads at B, C and D, in a sequential manner and determine deformations at B, C and D, respectively. A B C D E fBB fCB fDB 1 A B C D E fBC fCC fDC A 1 B C D E fBD fCD fDD 1
  • 13. (c ) Establish compatibility conditions at B, C and D DBO + fBBRB + fBCRC + fBDRD = 0 DCO + fCBRB + fCCRC + fCDRD = 0 DDO + fDBRB + fDCRC + fDDRD = 0
  • 14. 5.4.2 When support settlements occur: A B C D E DB DC DD Support settlements Compatibility conditions at B, C and D give the following equations: DBO + fBBRB + fBCRC + fBDRD = DB DCO + fCBRB + fCCRC + fCDRD = DC DDO + fDBRB + fDCRC + fDDRD = DD w / u. l.
  • 15. 55..55 TTRRUUSSSS SSTTRRUUCCTTUURREESS 80 kN C 60 kN D A B 80 kN C 60 kN D A 1 2 B Primary structure (a) (a) Remove the redundant member (say AB) and make the structure a primary determinate structure The condition for stability and indeterminacy is: r+m>=<2j, Since, m = 6, r = 3, j = 4, (r + m =) 3 + 6 > (2j =) 2*4 or 9 > 8 i = 1
  • 16. 5.5 Truss Structures (Cont’d) (b)Find deformation Dalong AB: ABO D=S (FuL)/AE ABO 0ABF= Force in member of the primary structure due to applied 0 load u= Forces in members due to unit force applied along AB AB(c) Determine fAB uABL =å deformation 2 along AB due to unit load applied along AB: , AB AE (d) Apply compatibility condition along AB: DABO+fAB,ABFAB=0
  • 17. (e) Determine the individual member forces in a particular member CE by FCE = FCE0 + uCE FAB where FCE0 = force in CE due to applied loads on primary structure (=F0), and uCE = force in CE due to unit force applied along AB (= uAB)
  • 18. 5.6 TEMPERATURE CCHHAANNGGEESS AANNDD FFAABBRRIICCAATTIIOONN EERRRROORR  Temperature changes affect the internal forces in a structure  Similarly fabrication errors also affect the internal forces in a structure (i) Subject the primary structure to temperature changes and fabrication errors. - Find the deformations in the redundant direction (ii) Reintroduce the removed members back and make the deformation compatible