Related Questions

    1.

    The magnetic field due to a small magnetic dipole of magnetic moment MM, at distance rr from the centre on the equatorial line is given by (in M.K.S system)

    A

    μ04πimesMr2\frac{{{\mu _0}}}{{4\pi }} imes \frac{M}{{{r^2}}}

    B

    μ04πimesMr3\frac{{{\mu _0}}}{{4\pi }} imes \frac{M}{{{r^3}}}

    C

    μ04πimes2Mr2\frac{{{\mu _0}}}{{4\pi }} imes \frac{{2M}}{{{r^2}}}

    D

    μ04πimes2Mr3\frac{{{\mu _0}}}{{4\pi }} imes \frac{{2M}}{{{r^3}}}

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    6.

    The magnetic field due to short bar magnet of magnetic dipole moment MM and length 2l,2l, on the axis at a distance zz (where z  >>lz\; > > l) from the center of the magnet is given by formula

    A

    μ0  M4πz3M^\frac{{{\mu _0}\;M}}{{4\pi {z^3}}}{\rm{\hat M}}

    B

    2μ0  M4πz3M^\frac{{2{\mu _0}\;M}}{{4\pi {z^3}}}{\rm{\hat M}}

    C

    4πMμ0z2M^\frac{{4\pi M}}{{{\mu _0}{z^2}}}{\rm{\hat M}}

    D

    μ0  M2πz3M^\frac{{{\mu _0}\;M}}{{2\pi {z^3}}}{\rm{\hat M}}

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    8.

    The needle of a deflection galvanometer shows a deflection of 6060^\circ due to a short bar magnet at a certain distance in tan AA position. If the distance is double the deflection is

    A

    sin1[38]{\sin ^{ - 1}}\left[ {\frac{{\sqrt 3 }}{8}} \right]

    B

    cos1[38]{\cos ^{ - 1}}\left[ {\frac{{\sqrt 3 }}{8}} \right]

    C

    an1[38]{an ^{ - 1}}\left[ {\frac{{\sqrt 3 }}{8}} \right]

    D

    cot1[38]{\cot ^{ - 1}}\left[ {\frac{{\sqrt 3 }}{8}} \right]

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