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7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
EXPERIMENT 2(B)
TITLE : Bending Moment Variation for Various Loading Conditions
OBJECTIVES : This experiment examines how bending moment varies at the cut position of the
beam for various loading conditions.
INTRODUCTION :
*Bending Moment
In a similar manner it can that if the Bending moments (BM) of the forces to the left of AA are
clockwise then the bending moment of the forces to the right of AA must be anticlockwise.
Bending Moment at AA is defined as the algebraic sum of the moments about the section of all
forces acting on either side of the section
Bending moments are considered positive when the moment on the left portion is clockwise and on
the right anticlockwise. This is referred to as aging bending moment as it tends to make the beam
concave upwards at AA. A negative bending moment is termed hogging.
http://www.codecogs.com/users/23287/SF-and-BM-0002.png7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
APPARATUS :
1) Digital Force Display
2) Load and Hanger
3) Rules
7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
THEORY :
We know that if a body or object of any sort is stationary, then the forces on it balance, as follows:
(1) Vertical equilibrium (total force up = total force down)
(2) Horizontal equilibrium (total force right = total force left)
(3) Moment equilibrium (total clockwise moment = total anticlockwise moment).
We will use the statement:
The Bending Moment at the cut is equal to the algebraic sum of the moments caused by the forces
acting to the left or right of the cut.
7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
PROCEDUR:
(i) Check the Digital Force Display meter reads zero with no load.
(ii)Measure the first position
.
7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
(iii) Carefully load the beam with the hangers in the positions shown in Figure 1, using the loads
indicated in table 2a.
cut
140mm 300mm
W1 RA RB
W1 = 3.92 N (400g)
Figure 1 : Force diagram
(iii) Record the Digital Force Display reading as in a figure 2 and figure 3.
(iv) Repeat the procedure with the beam loaded as in figure
(v) Convert the mass into a load (in Nrefer table 1a)
140mm cut
RA 260mm RB
W1 W2
W1 = 1.96 N (200g)
W2 = 3.92 N (400g)
Figure 2 : Force diagram
240mm cut
400mm
RA W1 W2 RB
W1 = 4.91 N (500g)
W2 = 3.92 N (400g)
Figure 3 : Force diagram
7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
Result :
Figure W1 (N) W2 (N) Experimental
bending moment
(Nm)
RA (N) RB (N) Theoretical
bending moment
(Nm)
1
2
3
CALCULATION :
Calculation for Theoretical bending moment (Nm)
W : Load (N), a : the distance to the load (not the cut) (m)-3
Load 3.92 ()( )
Load 5.88
Load 8.83
Calculation for RA and RB :
Figure 1 :
Figure 2 :
Figure 3 :
DISCUSSION :
7/28/2019 Bending_Moment_Variation_for_Various_Loading_Conditions[1].docx
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CC205~MECHANIC OF STRUCTURE
JKA, POLITEKNIK SULTAN ABDUL HALIM MUADZAM SHAH
1. Comment on how the result of the experiments compare with those calculated using the theory.
CONCLUSION :
REFERENCE :