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Example 19.3 
 
Analyse the continuous beam shown in Fig. 19.4a by moment-distribution 
method. The support 
ABC
B settles by  below mm 5 and C. Assume A EI to be 
constant for all members ; and . GPa E 200 =
4 6
10 8 mm I × =
 
 
 
Solution: 
 
Calculate fixed end beam moments due to externally applied loads assuming that 
support  and C are locked. B
 
 
m kN M m kN M
m kN M m kN M
F
CB
F
BC
F
BA
F
AB
. 67 . 2 ; . 67 . 2
. 2 ; . 2
- = + =
- = + =
     (1) 
 
 
 
In the next step calculate fixed end moments due to support settlements. In the 
span AB , the chord ' AB rotates in the clockwise direction and in span , the 
chord  rotates in the counterclockwise direction (Fig. 19.4b). 
BC
C B'
 
 
 
 
 
Page 2


Example 19.3 
 
Analyse the continuous beam shown in Fig. 19.4a by moment-distribution 
method. The support 
ABC
B settles by  below mm 5 and C. Assume A EI to be 
constant for all members ; and . GPa E 200 =
4 6
10 8 mm I × =
 
 
 
Solution: 
 
Calculate fixed end beam moments due to externally applied loads assuming that 
support  and C are locked. B
 
 
m kN M m kN M
m kN M m kN M
F
CB
F
BC
F
BA
F
AB
. 67 . 2 ; . 67 . 2
. 2 ; . 2
- = + =
- = + =
     (1) 
 
 
 
In the next step calculate fixed end moments due to support settlements. In the 
span AB , the chord ' AB rotates in the clockwise direction and in span , the 
chord  rotates in the counterclockwise direction (Fig. 19.4b). 
BC
C B'
 
 
 
 
 
 
radians
AB
3
3
10 25 . 1
4
10 5
-
-
× - =
×
- = ? 
 
radians
BC
3
3
10 25 . 1
4
10 5
-
-
× =
×
= ?       (2) 
 
?
?
?
?
?
?
?
? ×
-
× × × ×
- = - = =
- -
4
10 5
4
10 8 10 200 6 6
3 6 9
AB
AB
AB S
BA
S
AB
L
EI
M M ? 
 
.         (3)  3 3000 kNm Nm = =
 
m kN M M
S
CB
S
BC
. 0 . 3 - = = 
 
In the next step, calculate stiffness and distribution factors.  
 
EI EI K
EI K K
BC
BA AB
1875 . 0 25 . 0
4
3
25 . 0
= =
= =
          (4) 
 
At joint  :    429 . 0 ; 571 . 0 ; 4375 . 0 = = =
? BC BA
DF DF EI K B
 
At joint C :    0 . 1 ; 1875 . 0 = =
? CB
DF EI K
 
 
At fixed joint, the joint does not rotate and hence no distribution moments are 
developed and consequently distribution factor is equal to zero. The complete 
moment-distribution procedure is shown in Fig. 19.4c and Table 19.3. The 
diagram is self explanatory. In this particular case results are obtained in two 
cycles. In the first cycle joint is balanced and carry over moment is taken to 
joint 
C
. In the next cycle , joint B B is balanced and carry over moment is taken to 
joint . The bending moment diagram is shown in fig. 19.4d.       A
 
 
 
 
 
 
 
 
Page 3


Example 19.3 
 
Analyse the continuous beam shown in Fig. 19.4a by moment-distribution 
method. The support 
ABC
B settles by  below mm 5 and C. Assume A EI to be 
constant for all members ; and . GPa E 200 =
4 6
10 8 mm I × =
 
 
 
Solution: 
 
Calculate fixed end beam moments due to externally applied loads assuming that 
support  and C are locked. B
 
 
m kN M m kN M
m kN M m kN M
F
CB
F
BC
F
BA
F
AB
. 67 . 2 ; . 67 . 2
. 2 ; . 2
- = + =
- = + =
     (1) 
 
 
 
In the next step calculate fixed end moments due to support settlements. In the 
span AB , the chord ' AB rotates in the clockwise direction and in span , the 
chord  rotates in the counterclockwise direction (Fig. 19.4b). 
BC
C B'
 
 
 
 
 
 
radians
AB
3
3
10 25 . 1
4
10 5
-
-
× - =
×
- = ? 
 
radians
BC
3
3
10 25 . 1
4
10 5
-
-
× =
×
= ?       (2) 
 
?
?
?
?
?
?
?
? ×
-
× × × ×
- = - = =
- -
4
10 5
4
10 8 10 200 6 6
3 6 9
AB
AB
AB S
BA
S
AB
L
EI
M M ? 
 
.         (3)  3 3000 kNm Nm = =
 
m kN M M
S
CB
S
BC
. 0 . 3 - = = 
 
In the next step, calculate stiffness and distribution factors.  
 
EI EI K
EI K K
BC
BA AB
1875 . 0 25 . 0
4
3
25 . 0
= =
= =
          (4) 
 
At joint  :    429 . 0 ; 571 . 0 ; 4375 . 0 = = =
? BC BA
DF DF EI K B
 
At joint C :    0 . 1 ; 1875 . 0 = =
? CB
DF EI K
 
 
At fixed joint, the joint does not rotate and hence no distribution moments are 
developed and consequently distribution factor is equal to zero. The complete 
moment-distribution procedure is shown in Fig. 19.4c and Table 19.3. The 
diagram is self explanatory. In this particular case results are obtained in two 
cycles. In the first cycle joint is balanced and carry over moment is taken to 
joint 
C
. In the next cycle , joint B B is balanced and carry over moment is taken to 
joint . The bending moment diagram is shown in fig. 19.4d.       A
 
 
 
 
 
 
 
 
Table 19.3 Moment-distribution for continuous beam ABC 
 
Joints A B C 
 
Member AB BA BC CB 
Stiffness factor 0.25 EI 0.25 EI 0.1875 EI 0.1875 EI 
Distribution Factor  0.571 0.429 1.000 
      
Fixed End Moments 
due to applied loads 
(kN.m) 
2.000 -2.000 2.667 -2.667 
Fixed End Moments 
due to support 
settlements (kN.m) 
3.000 3.000 -3.000 -3.000 
Total 5.000 1.000 -0.333 -5.667 
      
Balance joint C and 
C.O. 
  2.835 5.667 
      
Total 5.000 1.000 2.502 0.000 
      
Balance joint B and 
C.O. to A 
-1.00 -2.000 -1.502  
      
Final Moments (kN.m) 4.000 -1.000 1.000 0.000 
 
 
 
 
Page 4


Example 19.3 
 
Analyse the continuous beam shown in Fig. 19.4a by moment-distribution 
method. The support 
ABC
B settles by  below mm 5 and C. Assume A EI to be 
constant for all members ; and . GPa E 200 =
4 6
10 8 mm I × =
 
 
 
Solution: 
 
Calculate fixed end beam moments due to externally applied loads assuming that 
support  and C are locked. B
 
 
m kN M m kN M
m kN M m kN M
F
CB
F
BC
F
BA
F
AB
. 67 . 2 ; . 67 . 2
. 2 ; . 2
- = + =
- = + =
     (1) 
 
 
 
In the next step calculate fixed end moments due to support settlements. In the 
span AB , the chord ' AB rotates in the clockwise direction and in span , the 
chord  rotates in the counterclockwise direction (Fig. 19.4b). 
BC
C B'
 
 
 
 
 
 
radians
AB
3
3
10 25 . 1
4
10 5
-
-
× - =
×
- = ? 
 
radians
BC
3
3
10 25 . 1
4
10 5
-
-
× =
×
= ?       (2) 
 
?
?
?
?
?
?
?
? ×
-
× × × ×
- = - = =
- -
4
10 5
4
10 8 10 200 6 6
3 6 9
AB
AB
AB S
BA
S
AB
L
EI
M M ? 
 
.         (3)  3 3000 kNm Nm = =
 
m kN M M
S
CB
S
BC
. 0 . 3 - = = 
 
In the next step, calculate stiffness and distribution factors.  
 
EI EI K
EI K K
BC
BA AB
1875 . 0 25 . 0
4
3
25 . 0
= =
= =
          (4) 
 
At joint  :    429 . 0 ; 571 . 0 ; 4375 . 0 = = =
? BC BA
DF DF EI K B
 
At joint C :    0 . 1 ; 1875 . 0 = =
? CB
DF EI K
 
 
At fixed joint, the joint does not rotate and hence no distribution moments are 
developed and consequently distribution factor is equal to zero. The complete 
moment-distribution procedure is shown in Fig. 19.4c and Table 19.3. The 
diagram is self explanatory. In this particular case results are obtained in two 
cycles. In the first cycle joint is balanced and carry over moment is taken to 
joint 
C
. In the next cycle , joint B B is balanced and carry over moment is taken to 
joint . The bending moment diagram is shown in fig. 19.4d.       A
 
 
 
 
 
 
 
 
Table 19.3 Moment-distribution for continuous beam ABC 
 
Joints A B C 
 
Member AB BA BC CB 
Stiffness factor 0.25 EI 0.25 EI 0.1875 EI 0.1875 EI 
Distribution Factor  0.571 0.429 1.000 
      
Fixed End Moments 
due to applied loads 
(kN.m) 
2.000 -2.000 2.667 -2.667 
Fixed End Moments 
due to support 
settlements (kN.m) 
3.000 3.000 -3.000 -3.000 
Total 5.000 1.000 -0.333 -5.667 
      
Balance joint C and 
C.O. 
  2.835 5.667 
      
Total 5.000 1.000 2.502 0.000 
      
Balance joint B and 
C.O. to A 
-1.00 -2.000 -1.502  
      
Final Moments (kN.m) 4.000 -1.000 1.000 0.000 
 
 
 
 
 
 
 
 
Summary 
 
The moment-distribution method is applied to analyse continuous beam having 
support settlements. Each step in the numerical example is explained in detail. 
All calculations are shown at appropriate locations. The deflected shape of the 
continuous beam is sketched. Also, wherever required, the bending moment 
diagram is drawn. The numerical examples are explained with the help of free-
body diagrams.  
 
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FAQs on The Moment Distribution Method: Statically Indeterminate Beams With Support Settlements - 3 - Structural Analysis - Civil Engineering (CE)

1. What is the Moment Distribution Method for statically indeterminate beams with support settlements?
Ans. The Moment Distribution Method is a structural analysis technique used to determine the distribution of moments and reactions in statically indeterminate beams that have support settlements. It takes into account the stiffness of the members and the settlements at the supports to calculate the final moments and reactions.
2. How does the Moment Distribution Method handle support settlements in statically indeterminate beams?
Ans. The Moment Distribution Method handles support settlements in statically indeterminate beams by considering the additional rotations and displacements caused by the settlements. These settlements are incorporated into the analysis by modifying the stiffness of the affected members and redistributing the moments and reactions accordingly.
3. What are the advantages of using the Moment Distribution Method for beams with support settlements?
Ans. The Moment Distribution Method offers several advantages for analyzing beams with support settlements. Firstly, it provides a relatively simple and intuitive approach to determine the distribution of moments and reactions. Secondly, it allows for the consideration of support settlements, which are common in real-world structures and can significantly affect the beam's behavior. Finally, it can handle complex structural configurations and is suitable for both manual and computer-based calculations.
4. Are there any limitations to using the Moment Distribution Method for beams with support settlements?
Ans. Yes, there are some limitations to using the Moment Distribution Method for beams with support settlements. One limitation is that it assumes linear-elastic behavior of the members and neglects any nonlinear effects that may arise from large deformations or material nonlinearity. Additionally, it may not accurately capture the redistribution of moments and reactions if the support settlements are significantly different in magnitude or occur at different locations along the beam.
5. Can the Moment Distribution Method be applied to beams with multiple support settlements?
Ans. Yes, the Moment Distribution Method can be applied to beams with multiple support settlements. Each settlement is considered individually, and the analysis is performed iteratively by redistributing the moments and reactions after incorporating the effects of each settlement. However, it is important to note that the accuracy of the results may be affected if the settlements are significant and occur at different locations along the beam.
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