Strength of materials by s k mondal pdf

Page 204

Chapter-5 Deflection of Beam Again integrating both side we get

S K Mondal’s

EI³ dy = ³ M x +A dx Mx 2 Ax + B ...(ii) 2 Where A and B are integration constants.

or EI y

applying boundary conditions in equation (i) &(ii) at x = L,

dy dx

0 gives A = ML

ML2 2 2 Mx MLx ML2 Therefore deflection equation is y = 2EI EI 2EI Which is the equation of elastic curve.

at x = L, y = 0 gives B =

ML2 ML2 2

2

? Maximum deflection at free end

? Maximum slope at free end

T

ML G = 2EI

(It is downward)

ML EI

Let us take a funny example: A cantilever beam AB of length ‘L’ and uniform flexural rigidity EI has a bracket BA (attached to its free end. A vertical downward force P is applied to free end C of the bracket. Find the ratio a/L required in order that the deflection of point A is zero.

[ISRO – 2008]

We may consider this force ‘P’ and a moment (P.a) act on free end A of the cantilever beam.

Page 204 of 429


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Strength of materials by s k mondal pdf by S.Dharmaraj - Issuu