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    22.

    If the velocity v(isβ€…β€Šcmsβˆ’1)v\left( {{\rm{is\;cm}}{{\rm{s}}^{ - 1}}} \right) of a particle is given in terms of t (in second) by the relation β€…β€Šβ€…β€Šv=at+bt+c\;\;v = at + \frac{b}{{t + c}} then, the dimensions of a,b and c are

    A

    a =Β [L]β€…β€Š\left[ {\rm{L}} \right]{\rm{\;}}, b =Β β€…β€Š[LT]{\rm{\;}}\left[ {{\rm{LT}}} \right], c =Β [T2]\left[ {{{\rm{T}}^2}} \right]

    B

    a =Β [L2]\left[ {{{\rm{L}}^2}} \right], b =Β [T]β€…β€Š\left[ {\rm{T}} \right]{\rm{\;}}, c =Β [LTβˆ’2]\left[ {{\rm{L}}{{\rm{T}}^{ - 2}}} \right]Β 

    C

    a =Β [LT2]\left[ {{\rm{L}}{{\rm{T}}^2}} \right], b =Β [LT]\left[ {{\rm{LT}}} \right], c =Β [L]\left[ {\rm{L}} \right]

    D

    a =Β [LTβˆ’2]\left[ {{\rm{L}}{{\rm{T}}^{ - 2}}} \right], b =Β [L]β€…β€Š\left[ {\rm{L}} \right]{\rm{\;}}, c =Β [T]\left[ {\rm{T}} \right]

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    23.

    If the velocity v(isβ€…β€Šcmsβˆ’1)v\left( {{\rm{is\;cm}}{{\rm{s}}^{ - 1}}} \right) of a particle is given in terms of t (in second) by the relation β€…β€Šβ€…β€Šv=at+bt+c\;\;v = at + \frac{b}{{t + c}} then, the dimensions of a,b and c are

    A

    a =Β [L]β€…β€Š\left[ {\rm{L}} \right]{\rm{\;}}, b =Β β€…β€Š[LT]{\rm{\;}}\left[ {{\rm{LT}}} \right], c =Β [T2]\left[ {{{\rm{T}}^2}} \right]

    B

    a =Β [L2]\left[ {{{\rm{L}}^2}} \right], b =Β [T]β€…β€Š\left[ {\rm{T}} \right]{\rm{\;}}, c =Β [LTβˆ’2]\left[ {{\rm{L}}{{\rm{T}}^{ - 2}}} \right]Β 

    C

    a =Β [LT2]\left[ {{\rm{L}}{{\rm{T}}^2}} \right], b =Β [LT]\left[ {{\rm{LT}}} \right], c =Β [L]\left[ {\rm{L}} \right]

    D

    a =Β [LTβˆ’2]\left[ {{\rm{L}}{{\rm{T}}^{ - 2}}} \right], b =Β [L]β€…β€Š\left[ {\rm{L}} \right]{\rm{\;}}, c =Β [T]\left[ {\rm{T}} \right]

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