$\text{B}=\frac{\mu_0}{4\pi}\frac{2\text{M}}{\text{d}^3}=\frac{10^{-7}\times2\times8\times10^{22}}{(6400\times10^{3})^{3}}\approx60\times10^{-6}\text{t}=60\mu\text{T}$

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$\text{B}=\frac{\mu_0}{4\pi}\frac{2\text{M}}{\text{d}^3}=\frac{10^{-7}\times2\times8\times10^{22}}{(6400\times10^{3})^{3}}\approx60\times10^{-6}\text{t}=60\mu\text{T}$


$\text{dx}=10\sin30^\circ\text{cm}=5\text{cm}$
$\frac{\text{dV}}{\text{dx}}=\text{B}=\frac{0.1\times10^{-4}\text{T-m}}{5\times10^{-2}\text{m}}$
Since B is perpendicular to equipotential surface.
Here it is at angle 120° with (+ve) x-axis and B = 2 × 10-4 T
$\text{B}_\text{H}=\text{B}\cos60^\circ$
$\Rightarrow\text{B}=52\times10^{-6}=52\mu\text{T}$
$\text{B}_\text{v}=\text{B}\sin\delta=52\times10^{-6}\frac{\sqrt{3}}{2}$
$=44.98\mu\text{T} \approx45\mu\text{T}$
For like poles tied together
M = M1 - M2
For unlike poles M' = M1 + M2
$\frac{\text{v}_1}{\text{v}_2}=\sqrt{\frac{\text{M}_1-\text{M}_2}{\text{M} _1-\text{M}_2}}\Rightarrow\Big(\frac{10}{2}\Big)^2$
$=\frac{\text{M}_1-\text{M}_2}{\text{M}_1+\text{M}_2}\Rightarrow25=\frac{\text{M}_1-\text{M}_2}{\text{M}_1+\text{M}_2}$
$\Rightarrow\frac{26}{24}=\frac{2\text{M}_1}{2\text{M}_2}\Rightarrow\frac{\text{M}_1}{\text{M}_2}=\frac{13}{12}$

$\theta=\tan^{-1}\sqrt{2}\Rightarrow\tan\theta=\sqrt{2}\Rightarrow2=\tan^2\theta$
$\Rightarrow\tan\theta=2\cot\theta\Rightarrow\frac{\tan\theta}{2}=\cot\theta$
We know
$\frac{\tan\theta}{2}=\tan\propto$Comparing we get,
$\tan\propto=\cot\theta$$\tan\propto=(90-\theta)$
$\propto=90-\theta$
$\theta +\propto=90$
Hence magnetic field due to the dipole is
$\perp\text{r}$ to the magnetic axis.
$\text{T}_1=0.1$
$\text{B}=\text{B}_\text{H}-\text{B}_{\text{Wire}}=2.4\times10^{-6}-\frac{\mu_0}{2\pi}\frac{\text{i}}{\text{r}}$
$=24\times10^{-6}-\frac{2\times10^{-7}\times18}{0.2}$
$=(24-10)\times10^{-6}=14\times10^{-6}$
$\text{T}=2\pi\sqrt{\frac{\text{I}}{\text{MB}_\text{H}}}$
$\frac{\text{T}_1}{\text{T}_2}=\sqrt{\frac{\text{B}}{\text{B}_\text{H}}}$
$\Rightarrow\frac{0.1}{\text{T}_2}=\sqrt{\frac{14\times10^{-6}}{24\times10^{-6}}}\Rightarrow\Big(\frac{0.1}{\text{T}_{2}}\Big)=\frac{14}{24}$
$\Rightarrow\text{T}_{1}^2=\frac{0.01\times14}{24}\Rightarrow\text{T}_2=0.076$

$\text{B} =\frac{\mu_02\text{M}}{4\pi\text{ d}^3}\Rightarrow2\times10^{-4}=\frac{10^{-7}\times2\text{M}}{(10^ {-1})^3}$
$\Rightarrow\frac{2\times10^{-4}\times10^{-3}}{10^{-7}\times2}=\text{M}\Rightarrow\text{M}=1\text{Am}^2$
$\frac{\mu_0\text{ M }}{4\pi\text{ d}^3}\Rightarrow2\times10^{-4}=\frac{10^{-7}\times\text{M}}{(10^{-1})^3}\Rightarrow\text{m}=2\text{Am}^2$
$\gamma=\frac{1}{2\pi}\sqrt{\frac{\text{MB}_\text{H}}{\text{I}}}$
$\gamma=\frac{1}{2\pi}\sqrt{\frac{\text{M}(\text{B}_\text{H}-\text{B})}{\text{I}}}$
$\text{B}=\frac{\mu_0}{4\pi}\frac{\text{m}}{\text{d}^3}=\frac{10^{-7}\times1.6}{8\times10^{-3}}=20\mu\text{T}$
$\frac{\gamma_1}{\gamma_2}=\sqrt{\frac{\text{B}}{\text{B}_\text{H}-\text{B}}}\Rightarrow\frac{40}{\gamma _2}=\sqrt{\frac{25}{5}}$
$\Rightarrow\gamma_2=\frac{40}{\sqrt{5}}=17.88\approx \text{osci/min}$
$\gamma_1 =\frac{1}{2\pi}\sqrt{\frac{\text{MB}_\text{H}}{\text{I}}}$
$\gamma_2=\frac{1}{2\pi}\sqrt{\frac{\text{M} (\text{B} _\text{H}-\text{B}}{\text{I}}}$
$\frac{\gamma_1}{\gamma_2}=\sqrt{\frac{\text{B}}{\text{B}_\text{H}-\text{B}}}\Rightarrow\frac{40}{\gamma_2}=\sqrt{\frac{25}{45}}$
$\Rightarrow\gamma_2=\frac{40}{\sqrt{\big(\frac{25}{45}\big)}}=53.66\approx54\text{ osci/min}$
$\text{d}=10\text{cm}=0.1\text{m}$
We know
$\frac{\text{M}}{\text{B}}=\frac{4\pi}{\mu_0}\frac{(\text{d-}^2\ell^2)^2}{2\text{d}}\tan\theta$
$=\frac{4\pi}{\mu_0}\times\frac{\text{d}^4}{2\text{d}}\tan\theta$
[As the magnet is short]$=\frac{4\pi}{4\pi\times10^{-7}}\times\frac{(0.1)^3}{2}\times\tan37^\circ$
$=0.5\times0.75\times1\times10^{-3}\times10^7$
$=3.75\times10^3\text{A-m}^2\text{T}^{-1}$
$=-0.2\times10^{-3}\times0.5=-0.1\times10^{-3}\text{T-m}$
Since the sigh is-ve therefore potential decreases.$\frac{\mu_0}{4\pi}\frac{2\text{M}}{\text{d}^3}=18\times10^{-6}$
$\Rightarrow\frac{10^{-7}\times2\times0.72}{\text{d}^3}=18\times10^{-6}$
$\Rightarrow\text{d}^3=\frac{2\times0.7\times10^{-7}}{18\times10^{-6}}$
$\Rightarrow\text{d}=\Big(\frac{8\times10^{-9}}{10{-6}}\Big)^\frac{1}{3}$
$=2\times10^{-1}\text{m}=20\text{cm}$



Here I' = 2I
$\text{T}_1=\frac{1}{40}\text{min}$
$\text{T}_2=?$
$\frac{\text{T}_1}{\text{T}_2}=\sqrt{\frac{\text{I}}{\text{I'}}}$
$\Rightarrow\frac{1}{40\text{T}_2}=\sqrt{\frac{1}{2}}\Rightarrow\frac{1}{1600\text{T}_2^2}\frac{1}{2}$
$\Rightarrow\text{T}_2^2=\frac{1}{800}\Rightarrow\text{T}_2=0.03536\text{min}$
For 1 oscillation Time taken = 0.03536 min
For 40 Oscillation Time
$=4\times0.03536=1.414=\sqrt{2}\text{ min}$