We are given two moving-coil galvanometers \(M_1\) and \(M_2\) with data:
\(M_1:\; R_1=5\,\Omega,\; N_1=15,\; A_1=3.6\times10^{-3}\,\text{m}^2,\; B_1=0.25\,\text{T}\)
\(M_2:\; R_2=7\,\Omega,\; N_2=21,\; A_2=1.8\times10^{-3}\,\text{m}^2,\; B_2=0.50\,\text{T}\)
Torsional constant \(k\) (spring) is the same for both.
For a moving-coil galvanometer, current sensitivity is \(S_I=\dfrac{\theta}{I}=\dfrac{NAB}{k}\). Voltage sensitivity is deflection per volt:
\[ S_V=\frac{\theta}{V}=\frac{\theta}{I}\cdot\frac{I}{V}=\frac{NAB}{k}\cdot\frac{1}{R}=\frac{NAB}{kR}. \]
Hence, for equal \(k\), the ratio of voltage sensitivities is
\[ \frac{S_{V1}}{S_{V2}}=\frac{N_1A_1B_1/R_1}{N_2A_2B_2/R_2} =\frac{N_1A_1B_1R_2}{N_2A_2B_2R_1}. \]
Step 1: Substitute the given values:
\[ \frac{S_{V1}}{S_{V2}} =\frac{15\,(3.6\times10^{-3})\,(0.25)\,(7)} {21\,(1.8\times10^{-3})\,(0.50)\,(5)}. \]
Step 2: Simplify (the \(10^{-3}\) cancels):
\[ \text{Numerator}=15\times3.6\times0.25\times7=94.5,\qquad \text{Denominator}=21\times1.8\times0.50\times5=94.5. \] \[ \therefore\ \frac{S_{V1}}{S_{V2}}= \frac{94.5}{94.5}=1. \]
The ratio of voltage sensitivities is \(S_{V1}:S_{V2}=1:1\).
Assertion (A): The deflection in a galvanometer is directly proportional to the current passing through it.
Reason (R): The coil of a galvanometer is suspended in a uniform radial magnetic field.
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.
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Two blocks of masses \( m \) and \( M \), \( (M > m) \), are placed on a frictionless table as shown in figure. A massless spring with spring constant \( k \) is attached with the lower block. If the system is slightly displaced and released then \( \mu = \) coefficient of friction between the two blocks.
(A) The time period of small oscillation of the two blocks is \( T = 2\pi \sqrt{\dfrac{(m + M)}{k}} \)
(B) The acceleration of the blocks is \( a = \dfrac{kx}{M + m} \)
(\( x = \) displacement of the blocks from the mean position)
(C) The magnitude of the frictional force on the upper block is \( \dfrac{m\mu |x|}{M + m} \)
(D) The maximum amplitude of the upper block, if it does not slip, is \( \dfrac{\mu (M + m) g}{k} \)
(E) Maximum frictional force can be \( \mu (M + m) g \)
Choose the correct answer from the options given below:
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: