written 6.3 years ago by | • modified 6.3 years ago |
Subject: Structural Analysis II
Topic: Flexibility Method
Difficulty: Medium / High
written 6.3 years ago by | • modified 6.3 years ago |
Subject: Structural Analysis II
Topic: Flexibility Method
Difficulty: Medium / High
written 6.3 years ago by |
As a support is fixed support. Therefore we have to use an imaginary span near the fixed end as shown in fig
1) Free bending moment
For Span AB BM at C=$\frac{wL^{2}}{8}=\frac{5\times(4)^{2}}{8}=10kN.m$
2) Free Bending Moment diagram
3) Applying theorem of three moments or elapeyron's theorem
For Span $A^{1}-A-B$
$MA^{1}l_{1}+2M_{A}(l_{1}+l_{2})+M_{B}l_{2}+\frac{6A_{1}x_{1}}{l_{1}}+\frac{6A_{2}x_{2}}{l_{2}}=0$
As $A^{1}$ is an imaginary Span
${M_{A}}^{1}=0 \ \ \ \ l_{1}=0$
$0+2M_{A}(0+4)+0+0+\frac{6\times26.67\times2}{4}=0$
$8M_{A}=80.01$
$M_{A}=\frac{80.01}{8}=-10kN.m$
$M_{A}=-10kN.m$
4) Find Reaction at Support
$\sum m_{B}=0$
$-R_{B}\times4+5\times4\times\frac{4}{2}-10=0$
$R_{B}=7.5kN \ \ \ \sum F_{y}=0(+ve)$
$-(5\times4)+7.5+R_{B}=0$
$\underline{R_{A}=12.5kN}$
5)B.M.D 6) S.F.D