Slope deflection method:
Slope deflection method is a displacement method used for the analysis of beams and frames. This method was introduced by George A Maney and was significantly used for more than a decade until the development of the Moment distribution method.
Steps involved in solving a problem by slope deflection method:
Slope deflection method is a displacement method used for the analysis of beams and frames. This method was introduced by George A Maney and was significantly used for more than a decade until the development of the Moment distribution method.
Steps involved in solving a problem by slope deflection method:
1.Determine the fixed end moments by considering each span as a fixed beam
2. Write the slope deflection equations for each span
3. Write the equilibrium equations for each joint
4. Solve the equilibrium equations and slope deflection equations for finding rotations(θ) and settlements (Δ)
5. Substitute the values of Δ and θ and find the final end moments (M)
6. Draw BMD and SFD
Slope deflection equations for any member AB of span L.
2. Write the slope deflection equations for each span
3. Write the equilibrium equations for each joint
4. Solve the equilibrium equations and slope deflection equations for finding rotations(θ) and settlements (Δ)
5. Substitute the values of Δ and θ and find the final end moments (M)
6. Draw BMD and SFD
Slope deflection equations for any member AB of span L.
MAB = MFAB+2EI/L[2θΑ+θΒ-3δ/L]
MBA= MFBA+2EI/L[θA+2θB-3δ/L]
where,
MAB & MBA= Final end moments at ends A & B respectively in any member AB.
MFAB & MFBA = Fixed end moments at ends A and B respectively in any member AB.
θA & θB=Rotations at ends A & B respectively in any member AB.
L = Span of member AB
δ = settlement
MBA= MFBA+2EI/L[θA+2θB-3δ/L]
where,
MAB & MBA= Final end moments at ends A & B respectively in any member AB.
MFAB & MFBA = Fixed end moments at ends A and B respectively in any member AB.
θA & θB=Rotations at ends A & B respectively in any member AB.
L = Span of member AB
δ = settlement
Solved example for illustration:
Q: Analyse the continuous beam ABCD shown in figure by slope deflection method.
Solution:
Step 1: Fixed end moments
MFAB = -wL²/12
= -(30×4²)/12 = -40KNm
MFBA = wL²/12
= (30×4²)/12 = 40KNm
MFBC = -wab²/L²
= -(60×2×2²)/4² = -30KNm
MFCB = wba²/L²
= (60×2×2²)/4² = 30KNm
MFCD = -wab²/L²
= -(60×2×4²)/6² = -53.33KNm
MFDC = wba²/L²
= (60×4×2²)/6² = 26.667KNm
Step 2: Slope deflection equations
(since θA=0 & δ=0)
MAB = -40+2EI/4[2(0)+θB-0]
= -40+0.5EIθB
MBA= MFBA+2EI/L[θA+2θB-3δ/L]
(since θA=0)
MBA=40+2EI/4[0+2θB-0]
=40+EIθB
MBC= -30+2EI/4[2θB+θC-0]
=-30+EIθB+0.5EIθC
MCB= 30+2EI/4[θΒ+2θC-0]
=30+0.5EIθΒ+EIθC
MCD= -55.33+2EI/6[2θC+θD-0]
= -55.33+0.667EIθC+0.33EIθD
MDC= 26.667+2EI/6[θC+2θD-0]
=26.667+0.33EIθC+0.667EIθD
Step 3: Equilibrium equations
ΣMB=0
MBA+MBC=0
or 40+EIθB-30+EIθB+0.5EIθC =0
or 2EIθB+0.5EIθC= -10 _____(1)
ΣMC=0
MCB+MCD=0
or 30+0.5EIθΒ+EIθC-55.33+0.667EIθC+0.33EIθD
or 1.5EIθB+5EIθC+EIθD+70 ___(2)
ΣMD=0
MDC=26.667+0.33EIθC+0.667EIθD=0
or EIθC+2EIθD= -80 _______(3)
on solving equations 1,2 & 3 we get,
EIθC= 28.485
EIθB= -12.121
EIθD -54.243
Step 4: Final end moments
Final end moments are calculated by substituting the values of EIθC, EIθB & EIθD in the slope deflection equations.
Hence,
MAB=-40+0.5(-12.121)
=-46.061KNm
MBA = 40-12.121=27.879KNm
MBC = -27.879KNm
MCB=30+0.5(-12.121)+28.485
=52.425KNm
MCD= -52.425KNm
MDC=0
Bending moment diagram:
Comments
Post a Comment