Question 1.4: A plane frame with an overhang is supported at points A and ...

A plane frame with an overhang is supported at points A and D (Fig.1-16). (This is the beam of Example 1-2 to which column BD has been added.) A linearly varying distributed load of peak intensity q0=160 N/mq_{0} = 160  N/m acts on span AB. Concentrated moment M0=380 NmM_{0} = 380  N·m is applied at A, and an inclined concentrated load P = 200 N acts at C. Force P also acts at mid-height of column BD. The lengths of segments AB and BD are L = 4 m, and the length of the overhang BC is 2 m.
Find support reactions at A and D and then calculate the axial force N, shear force V, and bending moment M at the top of column BD.

1.4
The blue check mark means that this solution has been answered and checked by an expert. This guarantees that the final answer is accurate.
Learn more on how we answer questions.

The four-step problem-solving approach for this plane frame follows the procedures presented for the beam in Example 1-2.

1. Conceptualize : Find the reaction forces Ay, DxA_{y} ,  D_{x} , and DyD_{y} using the FBD of the overall structure shown in Fig.1-17. Internal axial force N, shear force V, and bending moment M at the top of column BD (Fig.1-18) are obtained by cutting the column at that location. View column BD with joint D on your left and B on your right to establish the assumed positive directions of N, V, and M on either side of the cut section, as shown in Fig.1-18.

2. Categorize : First find reaction forces Ay,DxA_{y} , D_{x} , and DyD_{y}. Then use either the upper or lower free-body diagram in Fig.1-18 to find N, V, and M. The free-body diagrams in Fig.1-18 show internal axial force N, shear force V, and bending moment M in their assumed positive directions based on a deformation sign convention.

3. Analyze :
Solution for external reactions: Sum forces in the x direction to find reaction force component DxD_{x}. Next, sum moments about D to find reaction component AyA_{y}.

Finally, sum forces in the y direction to find reaction DyD_{y}. Use a statics sign convention in the solution as follows :

ΣFx=0Dx=35P+P=320\Sigma F_{x}=0 \quad D_{x}=\frac{3}{5} P+P=320 N

ΣMD=0Ay=1L[M0+12q0L[L3]+P1245P[L2]+35PL]=152\Sigma M_{D}=0 \quad A_{y}=\frac{1}{L}\left[-M_{0}+\frac{1}{2} q_{0} L\left[\frac{L}{3}\right]+P \frac{1}{2}-\frac{4}{5} P\left[\frac{L}{2}\right]+\frac{3}{5} P L\right]=152 N

ΣFy=0Dy=Ay+12q0L+45P=328\Sigma F_{y}=0 \quad D_{y}=-A_{y}+\frac{1}{2} q_{0} L+\frac{4}{5} P=328 N

All reaction force components are positive, so they act in the directions shown in Figs.1-17 and 1-18. The resultant reaction force at D is

Dres=Dx2+Dy2=458 ND_{ res }=\sqrt{D_{x}^{2}+D_{y}^{2}}=458  N.

Solution for internal axial force N, shear force V, and moment M at top of column BD: Using the lower free-body diagram in Fig.1-18,

ΣFy=0N=Dy=328 NΣFx=0V=Dx+P=120\Sigma F_{y}=0 \quad N=-D_{y}=-328  N \quad \Sigma F_{x}=0 \quad V=-D_{x}+P=-120 N

ΣM=0M=DxL+PL2=880 Nm\Sigma M=0 \quad M=-D_{x} L+P \frac{L}{2}=-880  N \cdot m

Alternatively, the upper free-body diagram can be used to compute N, V, and M (Fig.1-18):

ΣFy=0N=Ay12q0L45P=328 NΣFx=0V=35P=120\Sigma F_{y}=0 \quad N=A_{y}-\frac{1}{2} q_{0} L-\frac{4}{5} P=-328  N \quad \Sigma F_{x}=0 \quad V=-\frac{3}{5} P=-120 N

ΣM=0M=M0AyL45PL2+12q0L[L3]=880 Nm\Sigma M=0 \quad M=-M_{0}-A_{y} L-\frac{4}{5} P \frac{L}{2}+\frac{1}{2} q_{0} L\left[\frac{L}{3}\right]=-880  N \cdot m

The minus signs on internal axial force N, shear force V, and moment M indicate that all three quantities act opposite to directions assumed in Fig.1-18.

4. Finalize : Either the lower or upper free-body diagram can be used to find internal forces (N and V) and internal moment (M) at the top of column BD. Section forces and moments at any other location on the frame are found using the same approach. A properly drawn free-body diagram is an important first step in the solution.

1..4
1...4

Related Answered Questions