UNIT-IV SLOPE DEFLECTION METHOD - · PDF fileUNIT-IV SLOPE DEFLECTION METHOD ... B.M.D&S.F.D....
Transcript of UNIT-IV SLOPE DEFLECTION METHOD - · PDF fileUNIT-IV SLOPE DEFLECTION METHOD ... B.M.D&S.F.D....
UNIT-IV
SLOPE DEFLECTION METHOD
Continuous beams and rigid frames (with and without sway) – Symmetry and
antisymmetry – Simplification for hinged end – Support displacements
Introduction:
This method was first proposed by Prof. George A. Maney in 1915.
It is ideally suited to the analysis of continuous beams and rigid jointed frames.
Basic unknowns like slopes and deflections of joints are found out.
Moments at the ends of a member is first written down in terms of unknown slopes and
deflections of end joints.
Considering the joint equilibrium conditions, a set of equations are formed and solutions
of these simultaneous equations gives unknown slopes and deflections.
Then end moments of individual members are determined.
It involves solutions of simultaneous equations; a problem with more than three
unknowns is considered a difficult problem for hand calculations. Hence this method was
sidelined by moment distribution method with the help of computers; solutions for any
number of simultaneous equations can be obtained early.
The development of this method in the matrix form is “Stiffness Matrix Method” (it is
commonly used for the analysis of large structures with the help of computers.
Assumptions made in slope-deflection method
All joints are rigid.
The rotations of joints are treated as unknowns.
Between each pair of the supports the beam section is constant.
The joint in structure may rotate or deflect as a whole, but the angles between the
members meeting at that joint remain the same.
Distortions due to axial deformations are neglected.
Shear deformations are neglected.
Sign Conventions:
Moments:
Clockwise moments = (+)ive
Anti-clockwise moments = (-)ive
Rotations:
Clockwise rotations = (+)ive
Anti-clockwise rotations = (-)ive
Settlements:
Right side support is below left side support = (+)ive
Left side support is below right side support = (-)ive
Applications of Slope Deflection Equations:
Rigid jointed structures can be analyzed.
Continuous Beams
Frames without side sway (Non-Sway)
Frames with side sway (Sway)
The beam shown in Fig. is to be analyzed by slope-deflection method. What are the unknowns
and, to determine them, what are the conditions used?
Unknowns: ƟA, ƟB, ƟC
Equilibrium equations used: (i) MAB = 0 (ii) MBA + MBC = 0 (iii) MCB = 0
Write down the slope deflection equation for a fixed end support.
Write down the equilibrium equations for the frame shown in Fig.
Limitations of slope deflection method
It is not easy to account for varying member sections
It becomes very cumbersome when the unknown displacements are large in number.
Why slope-deflection method is called a ‘displacement method’?
In slope-deflection method, displacements (like slopes and displacements) are treated as
unknowns and hence the method is a „displacement method‟.
Degrees of freedom
In a structure, the numbers of independent joint displacements that the structure can
undergoes are known as degrees of freedom.
Write the fixed end moments for a beam carrying a central clockwise moment.
Problems:
1. Analyse the continuous beam given in figure by slope deflection method and draw the
B.M.D&S.F.D.
Step 1: Fixed end moments
MF
AB = -WL2/12 = -10×4
2/12 = -13.33 KNM
MF
BA = WL2/12 = 10×4
2/12 = -13.33 KNM
MF
BC = - Wab2/L
2 = -6×2×3
2/5
2 = -4.32 KNM
MF
CB = Wa2b/L
2 = 6×2
2×3/5
2 = 2.88 KNM
Step 2: Slope deflection equation
MAB = MF
AB+2EI/L (2θA+θB)
MAB = -13.33+EIθA + 0.5EIθB --------1
MBA = MF
BA+2EI/L (2θB+θA)
MBA = 13.33+0.5EIθA + EI θB --------2
MBC = MF
BC+2EI/L (2θB+θC)
MBC = -4.32+0.8EI θB --------3
MCB = 2.88+0.4EI θB --------4
Apply equilibrium conditions
MAB = 0
EI θA + 0.5EI θB = 13.33 --------5
MBA + MBC = 0
13.33 + 0.5EI θA +EI θB - 4.32 + 0.8EI θB = 0
0.5EI θA +1.8EI θB = -9.01 -------- 6
Solve eqn 5 & 6, we get
EIθA = 18.39
EIθB = -10.11
This values sub in eqn 1 to 4
MAB = 0 KNM
MBA = 12.67 KNM
MBC = -12.67 KNM
MCB = -1.16 KNM
Step 3: Find the Reactions
Span AB
RA = 16.83 KN
RB1 = 23.17 KN
RB2 = 6.312 KN
RC = -0.312 KN
𝑤 2. Analyze the frame given in figure by slope deflection method and draw the B.M.D & S.F.D.
Step 1: fixed end moments
MF
AB = -WL/8 = - 10×4/8 = -5 KNM
MF
BA = WL/8 = 10×4/8 = 5 KNM
MF
BC = -WL2/12 = - 10×2
2/12 = - 3.33 KNM
MF
CB = WL2/12 = 10×2
2/12 = 3.33 KNM
MF
CD = -WL/8 = - 10×4/8 = -5 KNM
MF
DC = WL/8 = 10×4/8 = 5 KNM
Step 2: Slope deflection equation
MAB=MFAB+2EI/L(2θA+θB)
MAB=-5 +0.5EIθB--------1
MBA = MF
BA+2EI/L (2θB+θA)
MBA = 5+EIθB --------2
MBC = MF
BC+2EI/L (2θB+θC)
MBC = -3.33+2EIθB + EIθC --------3
MCB = MF
CB+2EI/L (2θC+θB)
MCB = 3.33+2EIθC +EIθB --------4
MCD = MF
CD+2EI/L (2θC+θD)
MCD = -5+EIθC ---------5
MDC = MF
DC+2EI/L (2θD+θC)
MDC = 5+0.5EIθC ----------6
Apply equilibrium conditions
MBA+MBC = 0
5+EIθB-3.33+2EIθB +EIθC = 0 ----------7
MCB+MCD = 0
3.33+2EIθC +EIθB-5+EIθC = 0 ---------8
Solve eqn 7 & 8 we get
EIθB = -0.835
EIθC = 0.835
Sub this values eqn 1 to 6
MAB = -5.42 KNM
MBA = 4.17 KNM
MBC = -4.17 KNM
MCB = 4.17 KNM
MCD = -4.17 KNM
MDC = 5.42 KNM
Step 3: find reactions
Span AB:
RA = 5.31 KN
RB1 = 4.69 KN
Span BC:
RB2 = 10 KN
RC1 = 10 KN
Span CD:
RC2 = 4.69 KN
RD = 5.31 KN
3. Draw the SFD&BMD for th continuous beam shown in fig. Take E=2×105
N/mm2,I=3×10
6 mm
4 .The support B sinks by 30 mm. Using slope deflection method.
Step 1: fixed end moments
MF
AB = -WL2/12 = - 10×4
2/12 = -13.33 KNM
MF
BA = WL2/12 = 10×4
2/12 = -13.33 KNM
MF
BC = - Wab2/L
2 = -50×2×3
2/5
2 = -36 KNM
MF
CB = Wa2b/L
2 = 50×2
2×3/5
2 = 24 KNM
Step 2: Slope deflection equation
MAB = MF
AB + 2EI/L (2θA+θB) – 6EI∆/l2
MAB = EIθB - 20 -------1
MBA = MF
BA + 2EI/L (2θB+θA) – 6EI∆/l2
MBA = EIθB + 6.58 --------2
MBC = MF
BC + 2EI/L (2θB+θC) + 6EI∆/l2
MBC = 0.8EIθB -31.68 --------3
MCB = MF
CB + 2EI/L (2θC+θB) + 6EI∆/l2
MCB = 28.32 + 0.4EIθB --------4
Applying equilibrium conditions
MBA + MBC = 0
EIθB + 6.58 + 0.8EIθB - 31.68 = 0
EIθB = 13.94
This values sub in eqn 1 to 4
MAB = -13.03 KNM
MBA = 20.52 KNM
MBC = -20.52 KNM
MCB = 33.89KNM
Step 3: Find the reactions
Span AB
RA = 18.13 KN
RB1 = 21.87 KN
Span BC
RB2 = 27.33 KN
RC = 22.67 KN
4) Analyze continuous beam ABCD by slope deflection method and then draw bending
moment and SF diagram. Take EI constant.
Solution:
FEM M KN 44.44 - 6
24100
L
Wab F
2
2
2
2
AB
KNM 88.88 6
24100
L
bWa F
2
2
2
2
BA
KNM 41.67- 12
520
12
wLF
22
BC
KNM 41.67 12
520
12
wLF
22
CB
M KN 30 - 5.120FCD
Slope deflection equations:
1--------- EI3
144.442
L
EI2FM BBAABAB
2--------- EI3
289.882
L
EI2FM BABBABA
3-------- EI5
2EI
5
467.412
L
EI2FM CBCBBCBC
4-------- EI5
2EI
5
467.412
L
EI2FM BCBCCBCB
KNM 30MCD
:
5-------- 0EI5
2EI
15
2222.47
EI5
2EI
5
467.41EI
3
289.88MM,Now
CB
CBBBCBA
6EI5
4EI
5
267.11
30EI5
2EI
5
467.41MM,And
CB
BCCDCB
clockwise B @ Rotation 75.1EI
iseanticlockw B @ Rotation 67.32EI
C
B
KNM 30M
KNM 00.3067.325
275.1
5
467.41M
KNM 11.6775.15
267.32
5
467.41M
KNM 11.6767.323
289.88M
KNM 00.6167.322
144.44M
CD
CB
BC
BA
AB
Reactions: Consider free body diagram of beam AB, BC and CD as shown
ABSpan
KN 31.32R100R
KN 69.67R
6111.6741006R
BA
B
B
BC Span
KN 42.57R520R
KN 58.42R
11.673052
5205R
BB
C
C
Maximum Bending Moments:
KNM 26.684
6
6111.676133.133Max
SpanBC: where SF=0, consider SF equation with C as reference
m 13.220
58.42x
0x2058.42SX
M KN 26.15302
13.22013.258.42M
2
max
5) Analyse the portal frame shown in figure and also drawn bending moment and shear force
diagram
Solution:
FEM
KNM 106.67 - 6
2480
6
4280
L
cdW
L
abWF
2
2
2
2
2
2
2
2
2
1BC
KNM 67.106L
dcW
L
bWaF
2
2
2
2
2
CB
Slope deflection equations:
1-------- EI2
10
4
EI202
L
EI2FM BBBAABAB
2------- EI024
EI202
L
EI2FM BBABBABA
3------ EI3
2EI
3
467.106)2(
6
I2E267.106
2L
EI2FM
CBCB
CBBCBC
4------ EI3
2EI
3
467.106)2(
6
I2E267.106
2L
EI2FM
BCBC
BCCBCB
5------- EI)02(4
EI20
2L
EI2FM
CC
DCCDCD
6------- EI2
1)0(
4
EI20
2L
EI2FM
CC
CDDCDC
Now (7)------- 0EI3
2EI
3
767.106MM CBBCBA
Clockwise 6445
3 03.960 EI
0EI3
45960.03-
subtracts
0EI3
14EI
3
434.213
0EI3
14EI
3
4969.746
B
B
CB
CB
Using equation (7)
ckwise Anticlo64643
767.106
2
3-
EI3
767.106
2
3EI BC
are moments Final
KNM -3264 2
1 M
KNM 64 M
KNM 64 643
2)64 (
3
467.106M
KNM 64 643
264
3
467.106M
KNM 64M
KNM 322
64M
DC
CD
CB
BC
BA
AB
Consider free body diagrams of beam and columns as shown
By symmetrical we can write
KNM 80R R
KNM 60R R
CD
BA
KN 24H
32644 H
0M
A
A
B
Apply
KN 24H
32644 H
0M
D
A
C
6 )Analyse the portal frame and then draw the bending moment diagram
Solution:
Assume sway to right.
Here 0,0,0,0 DBDA
FEMS:
KNM 75.938
3580
L
bWaF
KNM 25.568
3580
L
WabF
2
2
2
2
CB
2
2
2
2
BC
Slope deflection equations
2-------- EI8
3EI
4
302
4
2EI0
L
32
L
EI2FM
1-------- EI8
3EI
2
1
4
30
4
2EI0
L
32
L
EI2FM
BB
ABBABA
BB
BAABAB
6--------- EI8
3EI
2
1
4
30
4
2EI0
L
32
L
EI2FM
5--------- EI8
3EI
4
302
4
2EI0
L
32
L
EI2FM
4--------- EI4
1EI
2
175.932
8
2EI75.93
2L
EI2FM
3--------- EI4
1EI
2
125.562
8
2EI25.56
2L
EI2FM
CC
CDDCDC
CC
DCCDCD
BCBC
BCCBCB
CBCB
CBBCBC
0MMMM
04
MM
4
MM,e.i
condition Shear - -- 0PHH
0MM
conditionsintJo0MM
DCCDBAAB
DCCDBAAB
HDA
CDCB
BCBA
70EI8
3EI
4
1EI
2
325.56
0EI4
1EI
2
125.56EI
8
3EIMM,Now
CB
CBBBCBA
80EI8
3EI
2
3EI
4
175.93
0EI8
3EIEI
4
1EI
2
175.93MM,And
CB
CBCCDCB
90EI2
3EI
2
3EI
2
3
EI`8
3EI
2
1
EI8
3EIEI
8
3EIEI
8
3EI
2
1MMMM,And
CB
C
CBBDCCDBAAB
(8) & (7) in Substitute
EIEIEI (9) From CB
(7) Eqn
10-------0EI8
1EI
8
925.56
0EIEI8
3EI
4
1EI
2
325.56
CB
CBCB
)8(Eqn
11----------0EI8
9EI
8
175.93
0EIEI8
3EI
2
3EI
4
175.93
CB
CBCB
Solving equations (10) & (11) we get 25.41EI B
By Equation (10)
5.3775.7825.41EIEIEI
75.7825.418
925.568
EI8
925.568EI
CB
BC
Hence
5.37EI,75.78EI,25.41EI CB
KNM31.255.378
375.78
2
1M
KNM69.645.378
375.78M
KNM69.6475.414
175.78
2
175.93M
KNM31.5575.784
125.41
2
125.56M
KNM31.555.378
325.41M
KNM69.345.378
325.41
2
1M
DC
CD
CB
BC
BA
AB
Reactions
SpanBC:
17.51R80R
KN83.288
38069.6431.55R
BC
B
Column CD:
5.224
31.2569.64HD
7) Frame ABCD is subjected to a horizontal force of 20 KN at joint C as shown in figure.
Analyse and draw bending moment diagram.
Solution:
Frame is Symmetrical and unsymmetrical loaded hence there is a sway. Assume sway
towards right
FEM
0FFFFFF DCCDCBBCBAAB
Slope deflection equations are
2EI3
2EI
3
4
3
32
3
EI2
L
32
L
EI2FM
1--------- EI3
2EI
3
2
3
3
3
EI2
L
32
L
EI2FM
B
B
ABBABA
B
B
BAABAB
5EI3
2EI
3
4
3
32
3
2EI
L
32
L
EI2FM
4-------- EI5.0EI
24
EI2
2L
EI2FM
3-------- EI5.0EI
24
EI2
2L
EI2FM
C
C
DCCDCD
BC
BC
BCCBCB
CB
CB
CBBCBC
6--------- EI3
2EI
3
2
3
3
3
EI2
L
32
L
EI2FM
C
c
CDDCDC
060MMMM
0203
MM
3
MM,e.i
020HH.III
0MM.II
0MM.I
DCCDBAAB
DCCDBAAB
DA
CDCB
BCBA
70EI3
2EI5.0EI
3
7
EI5.0EIEI3
2EI
3
4MMNow
CB
CBBBCBA
80EI3
2EI
3
7EI5.0
EI3
2EI
3
4EI5.0EIMMand
CB
CBCCDCB
9060EI3
8EI2EI2
60EI3
2EI
3
2EI
3
2
EI3
4EI
3
2EI
3
4EI
3
2EI
3
260MMMMand
CB
C
CBBDCCDBAAB
77.34EI
,18.8EI
,18.8EI
C
B
KNM73.1777.343
218.8
3
2M
KNM27.1277.343
218.8
3
4M
KNM27.1218.818.85.0M
KNM27.1218.85.018.80M
KNM27.1277.343
218.8
3
4M
KNM73.1777.343
218.8
3
2M
DC
CD
CB
BC
BA
AB
Reactions: Consider the free body diagram of the members
Member AB:
KN103
27.1273.17HA
MemberBC:
downwardsR of direction indicates sign ve-KN135.6RR
KN135.64
27.1227.12R
BCB
C
Member CD:
righttoleftisH of direction the indicates sign ve- KN103
27.1273.17H DD