A straight rod of length l extends from x=α to x=ℓ+α. If the mass per unit length is (a+bx2). The gravitational force It exerts on a point mass m placed at x=0 given by
A
Gm(a(1α−1α+ℓ)+bl)
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B
Gm(a+bx2)l2
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C
Gm(a(1α+1α+l)+bl)
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D
Gm(a(1α+l−1α)+bl)
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