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 :
-2nβ2x-4n-1
v(x)=βx−2na=dvdt=dvdx.dxdt=dvdx.vdvdx=−2nβx−2n−1∴a=−2nβx−2n−1.βx−2n =2nβ2x−4n−1