36 CHAPTER 1. PROPERTIES OF MATTER
l
Load
Pin
Figure 1.32: Non-uniform bending - experimental set up
distance between the two knife edges and let a weightW = Mgis suspended at the
midpoint (i.e., at the distancel/ 2 from the knife edges). Then the reaction at each knife
edge isW/ 2 which acts vertically upwards. The part of the beam between the knife edges
is equivalent to a pair of inverted cantilevers, each of lengthl/ 2 with an upward force
W/ 2 at the inverted free end as shown in Figure1.33. The elevation at the loaded end
l
Load
l
2
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l
2
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W
2
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W
2
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y
W
Figure 1.33: Non-uniform bending - Equivalence to a pair of inverted cantilevers
of each inverted cantilever is equal to the depressionyat the midpoint of the bar. The
Young’s ModulusY is can be written from equation (1.33)as,
Y =
(^1) W
2
(^21) l
2
(^23)
3 yIg
(1.41)
For a beam of rectangular cross-section with breadthband thicknessd,
Y =
Mgl^3
48 y
(^1) bd 3
12
2
Therefore, the Young’s Modulus of a nonuniformly bent bar is given by,
Y=
Mgl^3
4 bd^3 y
(1.42)
Experimental Procedure
As shown in Figure1.32, support the given beam symmetrically on two knife edges with