Mass = m
length = l
Current = i
Magnetic field = B = ?
$\text{iBl}=\mu\text{mg}$
$\Rightarrow\text{B}=\frac{\mu\text{gm}}{\text{il}}$
19 questions · timed · auto-graded
Mass = m
length = l
Current = i
Magnetic field = B = ?
$\text{iBl}=\mu\text{mg}$
$\Rightarrow\text{B}=\frac{\mu\text{gm}}{\text{il}}$
$\overrightarrow{\text{B}}=\text{B}_0\overrightarrow{\text{e}}_\text{r}$
$\overrightarrow{\text{e}}_\text{r}=$ Unit vector along radial direction
$\text{F}=\text{i}(\overrightarrow{\text{l}}\times\overrightarrow{\text{B}})=\text{ilB}\sin\theta$
$=\frac{\text{i}(2\pi\text{a})\text{B}_0\text{a}}{\sqrt{\text{a}^2}+\text{d}^2}=\frac{\text{i}2\pi\text{a}^2\text{B}_0}{\sqrt{\text{a}^2+\text{d}^2}}$

$\text{l}=2\pi\text{a}$
Magnetic field $=\overrightarrow{\text{B}}$ radially outwards
Current ⇒ 'i'
$\text{F}=\text{i l}\times\text{B}$
$=\text{i}\times(2\pi\text{a}\times\overrightarrow{\text{B}})$
$=2\pi\text{ai B}$ perpendicular to the plane of the figure going inside.

$\text{i}=5\text{A},\ \text{l}=50\text{cm}=0.5\text{m}$
$\text{B}=0.2\text{T},$
$\text{F}=\text{ilB}\sin\theta=\text{ilB}\sin90^\circ$
$=5\times0.5\times0.2$
$=0.05\text{N}$
For force on a current carrying wire in an uniform magnetic field
We need, l → length of wire
i → Current
B → Magnitude of magnetic field
Since $\overrightarrow{\text{F}}=\text{i}\ell\text{B}$
Now, since the length of the wire is fixed from A to B, so force is independent of the shape of the wire.

$\mu\text{R}=\text{F}$
$\Rightarrow\mu\times\text{m}\times\text{g}=\text{ilB}$
$\Rightarrow\mu\times10\times10^{-3}\times9.8$
$=\frac{6}{20}\times4.9\times10^{-2}\times0.8$
$\Rightarrow\mu=\frac{0.3\times0.8\times10^{-2}}{2\times10^{-2}}=0.12$
$\text{i}=\frac{\text{q}}{\text{t}}=\frac{\text{q}}{\text{t}}=\frac{\text{q}}{\Big(\frac{2\pi}{\omega}\Big)}=\frac{\text{q}\omega}{2\pi}$
$\mu=\text{n}\text{ ia}=\text{i A}[\because\text{n}=1]$
$=\frac{\text{q}\omega\pi\text{r}^2}{2\pi}$
$\text{L}=\text{I}\omega=\text{mr}^2\omega,\ \frac{\mu}{\text{L}}$
$=\frac{\text{q}\omega\text{r}^2}{2\text{mr}^2\omega}=\frac{\text{q}}{2\text{m}}$
$\Rightarrow\mu=\Big(\frac{\text{q}}{2\text{m}}\Big)\text{L}$

Edge = l
Current = i
Turns= n
mass = M
Magnetic filed = B
Min Torque produced must be able to balance the torque produced due to weight Now, $\tau\text{B}=\tau$ Weight.
$\mu\text{B}=\mu\text{g}\Big(\frac{1}{2}\Big)$
$\Rightarrow\text{n}\times\text{i}\times\text{l}^2\text{B}=\mu\text{g}\Big(\frac{1}{2}\Big)$
$\Rightarrow\text{B}=\frac{\mu}{2\text{nil}}$
Length = l, Current $=\text{l}\hat{\text{i}}$
$\overrightarrow{\text{B}}=\text{B}_0(\hat{\text{i}}+\hat{\text{j}}+\hat{\text{k}})\text{T}$
$\text{B}_0\hat{\text{i}}+\text{B}_0\hat{\text{j}}+\text{B}_0\hat{\text{k}}\text{T}$
$\text{F}=\text{Il}\times\overrightarrow{\text{B}}=\text{Il}\hat{\text{i}}\times\text{B}_0\hat{\text{i}}+\text{B}_0\hat{\text{j}}+\text{B}_0\hat{\text{k}}$
$=\text{Il}\text{B}_0\hat{\text{i}}\times\hat{\text{i}}+\text{lB}_0\hat{\text{i}}\times\hat{\text{j}}+\text{lB}0\hat{\text{i}}\times\hat{\text{k}}=\text{Il}\text{B}_0\hat{\text{k}}-\text{IlB}\hat{\text{j}}$
or, $|\overrightarrow{\text{F}}|=\sqrt{2\text{I}^2\text{l}^2\text{B}_0^2}=\sqrt{2}\text{Il}\text{B}_0$

Here, $2\text{T}\sin\theta=\text{i}\times\text{dl}\times\text{B}$
$\Rightarrow2\text{T}\theta=\text{i}\times\text{a}\times2\theta\times\text{B}$ $[\text{As}\theta\rightarrow0,\ \theta\approx0]$
$\Rightarrow\text{T}=\text{i}\times\text{a}\times\text{B}$
$\text{dl}=\text{a}\times2\theta$
Force of compression on the wire $=\text{i}\text{aB}$

Current anticlockwise
Since the horizontal Forces have no effect.
Let us check the forces for current along AD & BC [Since there is no $\overrightarrow{\text{B}}$ ]
In AD, F = 0
For BC
F = iaB upward
Current clockwise
Similarly, F = - iaB downwards
Hence change in force = change in tension
= iaB - (-iaB) = 2 iaB
F1 = Force on $\text{AD}=\text{i}\ell\text{B}$ inwards
F2 = Force on $\text{BC}=\text{i}\ell\text{B}$ inwards
They cancel each other
F3 = Force on $\text{CD}=\text{i}\ell\text{B}$ inwards
F4 = Force on $\text{AB}=\text{i}\ell\text{B}$ inwards
They also cancel each other.
So the net force on the body is 0.

$\text{F}=\text{ilB}\sin\theta$
$=\text{ilB}\sin90^\circ$
$=\text{i}\ 2\text{RB}$
$=2\times(8\times10^{-2})\times1$
$=16\times10^{-2}$
$=0.16\text{N}.$