To solve this problem, we need to understand the working principle of a moving coil galvanometer. The deflection in a moving coil galvanometer is directly proportional to the current flowing through it. This is based on the principle that the torque on a coil in a magnetic field is proportional to the current and the number of turns in the coil.
The deflection can be represented as:
\(\theta \propto I\)
Given:
First, convert \(60^{\circ}\) to radians:
\(60^{\circ} = \frac{60 \times \pi}{180} = \frac{\pi}{3} \text{ radians}\)
Using the proportionality, write the equation for both scenarios:
\(\frac{\pi}{3} \propto 200 \mu A\)
\(\frac{\pi}{10} \propto I_{\text{required}}\)
Equating the ratios as the proportionality constant is the same:
\(\frac{200}{I_{\text{required}}} = \frac{\frac{\pi}{3}}{\frac{\pi}{10}}\)
Simplify the right-hand side:
\(\frac{\pi}{3} \cdot \frac{10}{\pi} = \frac{10}{3}\)
Thus, the equation becomes:
\(\frac{200}{I_{\text{required}}} = \frac{10}{3}\)
Cross-multiply to solve for \(I_{\text{required}}\):
\(I_{\text{required}} = \frac{200 \times 3}{10} = 60 \mu A\)
Therefore, the current required to cause a deflection of \(\frac{\pi}{10}\) radians is 60 \(\mu A\).
Hence, the correct option is 60 \(\mu A\).
Given:
- \( i_2 = 200 \, \mu A \),
- \( \theta_2 = 60^\circ = \frac{\pi}{3} \, \text{radians} \).
The deflection \( \theta \) is proportional to the current \( i \). Therefore:
\(\frac{i_1}{i_2} = \frac{\theta_1}{\theta_2}.\)
For \( \theta_1 = \frac{\pi}{10} \, \text{radians} \):
\(\frac{i_1}{200} = \frac{\frac{\pi}{10}}{\frac{\pi}{3}}.\)
Simplify:
\(\frac{i_1}{200} = \frac{3}{10} \implies i_1 = 200 \times \frac{3}{10} = 60 \, \mu A.\)
The Correct answer is: 60 $\mu A$
Galvanometer:
A galvanometer is an instrument used to show the direction and strength of the current passing through it. In a galvanometer, a coil placed in a magnetic field experiences a torque and hence gets deflected when a current passes through it.
The name "galvanometer" is derived from the surname of Italian scientist Luigi Galvani, who in 1791 discovered that electric current makes a dead frog’s leg jerk.
A spring attached to the coil provides a counter torque. In equilibrium, the deflecting torque is balanced by the restoring torque of the spring, and we have the relation:
\[ NBAI = k\phi \]
Where:
As the current \( I_g \) that produces full-scale deflection in the galvanometer is very small, the galvanometer alone cannot be used to measure current in electric circuits.
To convert a galvanometer into an ammeter (to measure larger currents), a small resistance called a shunt is connected in parallel to the galvanometer.
To convert it into a voltmeter (to measure potential difference), a high resistance is connected in series with the galvanometer.
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = 4/3 \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \frac{n_2}{2n_1} \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is cm. 
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: