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    5.

    A particle of mass 'm' is subjected to a force F=βˆ’kx+F0x2F = -kx + \frac{F_0}{x^2}, where 'k' and 'F0F_0' are positive constants. If the particle starts from rest at x=ax=a, what is its speed when it reaches x=a2x=\frac{a}{2}?

    A

    ka24m\sqrt{\frac{ka^2}{4m}}

    B

    2F0am\sqrt{\frac{2F_0}{am}}

    C

    k(a2βˆ’a24)+2F0(2aβˆ’1a)m\sqrt{\frac{k(a^2-\frac{a^2}{4}) + 2F_0(\frac{2}{a}-\frac{1}{a})}{m}}

    D

    ka2+4F02am\sqrt{\frac{ka^2 + 4F_0}{2am}}

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    9.

    A particle of mass mm moves along the x-axis under the influence of a variable force F(x)=βˆ’kx+ax3F(x) = -kx + \frac{a}{x^3}, where kk and aa are positive constants. If the particle starts from rest at x=x0x = x_0, what is its speed when it reaches x=x02x = \frac{x_0}{2}?

    A

    v=3m(kx024βˆ’ax02)v = \sqrt{\frac{3}{m}(\frac{kx_0^2}{4} - \frac{a}{x_0^2})}

    B

    v=3m(kx022βˆ’a2x02)v = \sqrt{\frac{3}{m}(\frac{kx_0^2}{2} - \frac{a}{2x_0^2})}

    C

    v=km(x02βˆ’x024)v = \sqrt{\frac{k}{m}(x_0^2 - \frac{x_0^2}{4})}

    D

    v=2m(kx022βˆ’2ax02)v = \sqrt{\frac{2}{m}(\frac{kx_0^2}{2} - \frac{2a}{x_0^2})}

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