A straight rod of length L extends from x=a to x=L +a. The gravitational force is exerted on a point mass 'm' at x=0, if the mass per unit length of the rod is A+Bx2 is given by.
A
Gm[A(1a+L−1a)−BL]
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B
Gm[A(1a−1a+L)+BL]
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C
Gm[A(1a+L−1a)+BL]
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D
Gm[A(1a−1a+L)−BL]
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Solution
The correct option is BGm[A(1a−1a+L)+BL] dm=(A+Bx2)dx df=GMdmx2 =F=∫a+LaGMx2(A+Bx2)dx =GM[−Ax+Bx]a+La Gm[A(1a−1a+L)+BL