Step 1: Known Information.
Initial orientation of the bar magnet: aligned with the magnetic field ($ \theta_0 = 0^\circ $).
Work done to rotate the magnet from $ 0^\circ $ to $ 45^\circ $ is $ W $.
We need to find the additional work required to rotate the magnet from $ 45^\circ $ to $ 60^\circ $ (an additional $ 15^\circ $).
Step 2: Formula for Work Done in Rotating a Bar Magnet.
The work done ($ W $) in rotating a bar magnet in a uniform magnetic field is given by: $$ W = M B (1 - \cos\theta) $$ where:
$ M $ is the magnetic moment of the magnet,
$ B $ is the magnetic field strength,
$ \theta $ is the angle between the magnetic moment and the magnetic field.
Step 3: Work Done to Rotate from $ 0^\circ $ to $ 45^\circ $. When the magnet is rotated from $ 0^\circ $ to $ 45^\circ $: $$ W_{0 \to 45} = M B (1 - \cos 45^\circ) $$ We know that: $$ \cos 45^\circ = \frac{1}{\sqrt{2}} $$ Thus: $$ W_{0 \to 45} = M B \left(1 - \frac{1}{\sqrt{2}}\right) = W $$ Step 4: Work Done to Rotate from $ 45^\circ $ to $ 60^\circ $.
When the magnet is rotated from $ 45^\circ $ to $ 60^\circ $, the total work done from $ 0^\circ $ to $ 60^\circ $ is: $$ W_{0 \to 60} = M B (1 - \cos 60^\circ) $$ We know that: $$ \cos 60^\circ = \frac{1}{2} $$ Thus: $$ W_{0 \to 60} = M B \left(1 - \frac{1}{2}\right) = M B \cdot \frac{1}{2} $$ The additional work done from $ 45^\circ $ to $ 60^\circ $ is: $$ W_{45 \to 60} = W_{0 \to 60} - W_{0 \to 45} $$ Substitute the expressions for $ W_{0 \to 60} $ and $ W_{0 \to 45} $: $$ W_{45 \to 60} = M B \cdot \frac{1}{2} - M B \left(1 - \frac{1}{\sqrt{2}}\right) $$ Simplify: $$ W_{45 \to 60} = M B \left(\frac{1}{2} - 1 + \frac{1}{\sqrt{2}}\right) $$ $$ W_{45 \to 60} = M B \left(-\frac{1}{2} + \frac{1}{\sqrt{2}}\right) $$ Step 5: Relate to Given Work $ W $.
From Step 3, we know: $$ W = M B \left(1 - \frac{1}{\sqrt{2}}\right) $$ Thus: $$ M B = \frac{W}{1 - \frac{1}{\sqrt{2}}} $$ Substitute $ M B $ into the expression for $ W_{45 \to 60} $: $$ W_{45 \to 60} = \frac{W}{1 - \frac{1}{\sqrt{2}}} \cdot \left(-\frac{1}{2} + \frac{1}{\sqrt{2}}\right) $$ Simplify the term $ -\frac{1}{2} + \frac{1}{\sqrt{2}} $: $$ -\frac{1}{2} + \frac{1}{\sqrt{2}} = \frac{-\sqrt{2} + 2}{2\sqrt{2}} = \frac{2 - \sqrt{2}}{2\sqrt{2}} $$ Thus: $$ W_{45 \to 60} = \frac{W}{1 - \frac{1}{\sqrt{2}}} \cdot \frac{2 - \sqrt{2}}{2\sqrt{2}} $$ Simplify $ 1 - \frac{1}{\sqrt{2}} $: $$ 1 - \frac{1}{\sqrt{2}} = \frac{\sqrt{2} - 1}{\sqrt{2}} $$ So: $$ W_{45 \to 60} = \frac{W}{\frac{\sqrt{2} - 1}{\sqrt{2}}} \cdot \frac{2 - \sqrt{2}}{2\sqrt{2}} $$ $$ W_{45 \to 60} = W \cdot \frac{\sqrt{2}}{\sqrt{2} - 1} \cdot \frac{2 - \sqrt{2}}{2\sqrt{2}} $$ Simplify: $$ W_{45 \to 60} = W \cdot \frac{2 - \sqrt{2}}{2(\sqrt{2} - 1)} $$ Rationalize the denominator: $$ \frac{2 - \sqrt{2}}{\sqrt{2} - 1} = \frac{(2 - \sqrt{2})(\sqrt{2} + 1)}{(\sqrt{2} - 1)(\sqrt{2} + 1)} = \frac{(2 - \sqrt{2})(\sqrt{2} + 1)}{2 - 1} = (2 - \sqrt{2})(\sqrt{2} + 1) $$ Expand: $$ (2 - \sqrt{2})(\sqrt{2} + 1) = 2\sqrt{2} + 2 - 2 - \sqrt{2} = \sqrt{2} $$ Thus: $$ W_{45 \to 60} = W \cdot \frac{\sqrt{2}}{2} $$ $$ W_{45 \to 60} = \frac{W}{\sqrt{2}} $$ Final Answer: $ \boxed{\frac{W}{\sqrt{2}}} $
Draw the pattern of the magnetic field lines for the two parallel straight conductors carrying current of same magnitude 'I' in opposite directions as shown. Show the direction of magnetic field at a point O which is equidistant from the two conductors. (Consider that the conductors are inserted normal to the plane of a rectangular cardboard.)
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Choke coil is simply a coil having a large inductance but a small resistance. Choke coils are used with fluorescent mercury-tube fittings. If household electric power is directly connected to a mercury tube, the tube will be damaged.
Reason (R): By using the choke coil, the voltage across the tube is reduced by a factor \( \frac{R}{\sqrt{R^2 + \omega^2 L^2}} \), where \( \omega \) is the frequency of the supply across resistor \( R \) and inductor \( L \). If the choke coil were not used, the voltage across the resistor would be the same as the applied voltage.
In light of the above statements, choose the most appropriate answer from the options given below:
Figure shows a current carrying square loop ABCD of edge length is $ a $ lying in a plane. If the resistance of the ABC part is $ r $ and that of the ADC part is $ 2r $, then the magnitude of the resultant magnetic field at the center of the square loop is: 