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    6.

    When a wire of length 10  m10\,\,m is subjected to a force of 100  N100\,\,N along its length, the lateral strain produced is 0.01imes10βˆ’3m0.01 imes {10^{ - 3}}m. The Poisson’s ratio was found to be 0.40.4. If the area of cross-section of wire is 0.025  m20.025\,\,{{\rm{m}}^2}, its Young’s modulus is

    A

    1.6  imes108 Nmβˆ’21.6\,\, imes {10^8}\,{\rm{N}}{{\rm{m}}^{ - 2}}

    B

    2.5  imes1010 Nmβˆ’22.5\,\, imes {10^{10}}\,{\rm{N}}{{\rm{m}}^{ - 2}}

    C

    1.25  imes1011 Nmβˆ’21.25\,\, imes {10^{11}}\,{\rm{N}}{{\rm{m}}^{ - 2}}

    D

    16  imes109  Nmβˆ’216\,\, imes {10^9}\,\,{\rm{N}}{{\rm{m}}^{ - 2}}

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    9.

    When the tension in a metal wire is T1,its  length  isβ€Šβ€Šβ€‰β€‰l1{T_1},{\rm{its}}\,\,{\rm{length}}\,\,{\rm{is}}{\mkern 1mu} {\mkern 1mu} \,\,{l_1}. When the tension is T2{T_2} its length is l2{l_2}. The natural length of wire is

    A

    T2T1(l1+l2)\frac{{{T_2}}}{{{T_1}}}\left( {{l_1} + {l_2}} \right)

    B

    T1l1+T2l2{T_1}{l_1} + {T_2}{l_2}

    C

    l1T2βˆ’l2T1T2βˆ’T1\frac{{{l_1}{T_2} - {l_2}{T_1}}}{{{T_2} - {T_1}}}

    D

    l1T2+l2T1T2+T1\frac{{{l_1}{T_2} + {l_2}{T_1}}}{{{T_2} + {T_1}}}

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