A particle of unit mass undergoes one-dimensional motion such that its velocity varies according to v(x)=βx−2n, where β and n are constants and x is the position of the particle. The acceleration of the particle as a function of x, is given by
A
−2β2x−2n+1
B
−2nβ2e−4n+1
C
−2nβ2x−2n−1
D
−2nβ2x−4n−1
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Solution
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v(x)=βx−2n
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