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 Page 1


 
 
                         ?     
?
= 0
B
M 0 = + +
BD BC BA
M M M   (3) 
 
                               
?
= 0
D
M ? 0 =
DB
M     (4)  
 
                         ?      
?
= 0
C
M 0 = +
CE CB
M M    (5) 
 
Substituting the values of and in the equations (3), 
(4), and (5) 
CB DB BD BC BA
M M M M M , , , ,
CE
M
                                         
3.333 0.667 0.5 4.833
BC D
EI EI EI ? ?? + +=- 
 
0.5 0
BD
EI EI ? ? += 
 
2.333 0.667 7.5
CB
EI EI ? ? + =    (6)  
 
Solving the above set of simultaneous equations, 
C B
? ? , and  
D
? are evaluated. 
 
2.4125
B
EI ? = - 
 
Page 2


 
 
                         ?     
?
= 0
B
M 0 = + +
BD BC BA
M M M   (3) 
 
                               
?
= 0
D
M ? 0 =
DB
M     (4)  
 
                         ?      
?
= 0
C
M 0 = +
CE CB
M M    (5) 
 
Substituting the values of and in the equations (3), 
(4), and (5) 
CB DB BD BC BA
M M M M M , , , ,
CE
M
                                         
3.333 0.667 0.5 4.833
BC D
EI EI EI ? ?? + +=- 
 
0.5 0
BD
EI EI ? ? += 
 
2.333 0.667 7.5
CB
EI EI ? ? + =    (6)  
 
Solving the above set of simultaneous equations, 
C B
? ? , and  
D
? are evaluated. 
 
2.4125
B
EI ? = - 
 
3.9057
C
EI ? = 
 
1.2063
D
EI ? =     (7) 
 
Substituting the values of 
C B
? ? , and 
D
? in (2), beam end moments are 
computed.  
 
2.794 kN.m
AB
M = 
 
5.080 kN.m
BA
M = - 
 
1.8094 kN.m
BD
M = - 
 
0
DB
M = 
 
6.859 kN.m
BC
M = 
 
3.9028 kN.m
CB
M = - 
 
3.9057 kN.m
CE
M = 
 
1.953 kN.m
EC
M =     (8) 
 
The reactions are computed in Fig 16.5(d), using equilibrium equations known 
beam-end moments and given loading. 
 
 
Page 3


 
 
                         ?     
?
= 0
B
M 0 = + +
BD BC BA
M M M   (3) 
 
                               
?
= 0
D
M ? 0 =
DB
M     (4)  
 
                         ?      
?
= 0
C
M 0 = +
CE CB
M M    (5) 
 
Substituting the values of and in the equations (3), 
(4), and (5) 
CB DB BD BC BA
M M M M M , , , ,
CE
M
                                         
3.333 0.667 0.5 4.833
BC D
EI EI EI ? ?? + +=- 
 
0.5 0
BD
EI EI ? ? += 
 
2.333 0.667 7.5
CB
EI EI ? ? + =    (6)  
 
Solving the above set of simultaneous equations, 
C B
? ? , and  
D
? are evaluated. 
 
2.4125
B
EI ? = - 
 
3.9057
C
EI ? = 
 
1.2063
D
EI ? =     (7) 
 
Substituting the values of 
C B
? ? , and 
D
? in (2), beam end moments are 
computed.  
 
2.794 kN.m
AB
M = 
 
5.080 kN.m
BA
M = - 
 
1.8094 kN.m
BD
M = - 
 
0
DB
M = 
 
6.859 kN.m
BC
M = 
 
3.9028 kN.m
CB
M = - 
 
3.9057 kN.m
CE
M = 
 
1.953 kN.m
EC
M =     (8) 
 
The reactions are computed in Fig 16.5(d), using equilibrium equations known 
beam-end moments and given loading. 
 
 
 
 
( )
6.095 kN
Ay
R = ? 
 
( )
9.403 kN
Dy
R = ? 
 
( )
4.502 kN
Ey
R = ? 
 
( ) 1.013 kN
Ax
R = ? 
 
( ) 0.542 kN
Dx
R = ? 
 
( ) 1.465 kN
Ex
R =- ?     (9) 
 
The bending moment diagram is shown in Fig 16.5.(e)  and the elastic curve is  
shown in Fig 16.5(f). 
 
 
Page 4


 
 
                         ?     
?
= 0
B
M 0 = + +
BD BC BA
M M M   (3) 
 
                               
?
= 0
D
M ? 0 =
DB
M     (4)  
 
                         ?      
?
= 0
C
M 0 = +
CE CB
M M    (5) 
 
Substituting the values of and in the equations (3), 
(4), and (5) 
CB DB BD BC BA
M M M M M , , , ,
CE
M
                                         
3.333 0.667 0.5 4.833
BC D
EI EI EI ? ?? + +=- 
 
0.5 0
BD
EI EI ? ? += 
 
2.333 0.667 7.5
CB
EI EI ? ? + =    (6)  
 
Solving the above set of simultaneous equations, 
C B
? ? , and  
D
? are evaluated. 
 
2.4125
B
EI ? = - 
 
3.9057
C
EI ? = 
 
1.2063
D
EI ? =     (7) 
 
Substituting the values of 
C B
? ? , and 
D
? in (2), beam end moments are 
computed.  
 
2.794 kN.m
AB
M = 
 
5.080 kN.m
BA
M = - 
 
1.8094 kN.m
BD
M = - 
 
0
DB
M = 
 
6.859 kN.m
BC
M = 
 
3.9028 kN.m
CB
M = - 
 
3.9057 kN.m
CE
M = 
 
1.953 kN.m
EC
M =     (8) 
 
The reactions are computed in Fig 16.5(d), using equilibrium equations known 
beam-end moments and given loading. 
 
 
 
 
( )
6.095 kN
Ay
R = ? 
 
( )
9.403 kN
Dy
R = ? 
 
( )
4.502 kN
Ey
R = ? 
 
( ) 1.013 kN
Ax
R = ? 
 
( ) 0.542 kN
Dx
R = ? 
 
( ) 1.465 kN
Ex
R =- ?     (9) 
 
The bending moment diagram is shown in Fig 16.5.(e)  and the elastic curve is  
shown in Fig 16.5(f). 
 
 
 
 
 
 
 
Summary 
In this lesson plane frames restrained against sidesway are analysed using 
slope-deflection equations. Equilibrium equations are written at each rigid joint of 
the frame and also at the support. Few problems are solved to illustrate the 
procedure. The shear force and bending moment diagrams are drawn for the 
plane frames.  
 
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FAQs on The Slope Deflection Method: Frames Without Sidesway - 4 - Structural Analysis - Civil Engineering (CE)

1. What is the slope deflection method in structural analysis?
The slope deflection method is a structural analysis technique used to determine the deflected shape and internal forces of a structure, specifically frames without sidesway. It involves calculating the rotation and displacement at each joint of the frame by considering the bending and axial deformations of the members. By using the equilibrium conditions and compatibility equations, the method enables the determination of member forces and moments.
2. How does the slope deflection method handle frames without sidesway?
The slope deflection method is particularly suitable for analyzing frames without sidesway. In such frames, the lateral deflection or sidesway is prevented due to the presence of rigid connections or bracing elements. This simplifies the analysis as the deflections and rotations at the joints are only caused by bending and axial deformations. The method considers the stiffness of each member and the compatibility of rotations and displacements at the joints to determine the internal forces and deflected shape of the frame.
3. What are the advantages of using the slope deflection method for frames without sidesway?
The slope deflection method offers several advantages when analyzing frames without sidesway. Firstly, it provides accurate results by considering the actual stiffness and deformation behavior of the members. Secondly, it allows for the determination of member forces and moments, which are crucial for assessing the structural integrity and designing appropriate connections. Lastly, it can handle frames with various support conditions and member types, making it a versatile technique for structural analysis.
4. Are there any limitations or assumptions associated with the slope deflection method for frames without sidesway?
Yes, the slope deflection method has some limitations and assumptions. One key assumption is that the members of the frame behave elastically, meaning that they do not undergo plastic deformation. Additionally, the method assumes that the deflections and rotations are small, which may not be accurate for highly flexible or dynamic structures. Furthermore, it assumes that the frame is statically determinate and that the applied loads are known. These assumptions should be considered when applying the slope deflection method.
5. How can I apply the slope deflection method to analyze frames without sidesway?
To apply the slope deflection method, you need to follow a systematic procedure. First, determine the support conditions and member properties of the frame. Next, calculate the fixed-end moments for each member based on the applied loads and member properties. Then, establish the slope-deflection equations for each member, considering the rotations and displacements at the ends. Finally, solve the resulting system of equations to obtain the unknown rotations and displacements, which can be used to determine the member forces and moments.
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