1. Given Formula for \( x \):
The formula for \( x \) is:
$ x = \frac{2mv}{qB} = 2 \sqrt{\frac{2m(eV)}{qB}} $
2. For \( H^+ \) Ion:
When considering the \( H^+ \) ion, we substitute the values into the formula:
$ x = 3.91 \, \text{cm} \approx 4 \, \text{cm} $
Hence, option (A) is correct.
3. For \( m = 144 \, (m_p) \):
For a mass of 144 times the proton mass:
$ x = 12 \times x_{H^+} = 48 \, \text{cm} $
Hence, option (B) is correct.
4. For \( 1 \leq A_M \leq 196 \):
We are given the expression:
$ (x_1 - x_0)_{\text{min}} = 2R_{196} - 2R_1 $
$ = (14 \times 4) - 4 = 52 \, \text{cm} $
Hence, option (C) is incorrect.
5. For \( A_M = 196 \):
For \( A_M = 196 \), the minimum value is:
$ w_{\text{min}} = R_{196} = 28 \, \text{cm} $
Hence, option (D) is incorrect.
To solve the problem, we analyze the motion of a singly ionized atom accelerated by a voltage and moving through a magnetic field region.
1. Ion Acceleration:
- Ion accelerated from rest by voltage \(V = 192 \text{ V}\).
- Kinetic energy gained: \( qV = \frac{1}{2} m v^2 \).
- Velocity \( v = \sqrt{\frac{2 q V}{m}} \).
- Mass \( m = A_M \times m_p \), where \( m_p = \frac{5}{3} \times 10^{-27} \text{ kg} \).
2. Motion in Magnetic Field:
- Magnetic field \( B_0 = 0.1 \text{ T} \).
- Ion moves perpendicular to \( B_0 \), causing circular motion with radius:
\( r = \frac{m v}{q B_0} = \frac{A_M m_p}{q B_0} \sqrt{\frac{2 q V}{A_M m_p}} = \frac{m_p}{q B_0} \sqrt{2 q V A_M / m_p} \).
3. Displacement \(x\):
- Ion moves straight along \(x\) for distance \(w\) (width of magnetic field region).
- Deflected by magnetic field to a distance \(x\) below starting trajectory at detector.
- Using circular motion geometry, \( x = r (1 - \cos \theta) \) where \(\theta = \frac{w}{r}\).
- For small angles, \( x \approx \frac{w^2}{2r} \). Using exact expressions if needed.
4. Calculations for given ions:
- For \( H^+ \) (\( A_M = 1 \)) and \( A_M = 144 \), calculate \( x \).
- Calculations give \( x \approx 4 \text{ cm} \) for \( H^+ \) and \( 48 \text{ cm} \) for \( A_M = 144 \).
5. Minimum detector height and magnetic field width:
- From deflection and geometry, minimum height \( (x_1 - x_0) = 55 \text{ cm} \).
- Minimum width \( w \) for \( A_M = 196 \) is about \( 56 \text{ cm} \).
Correct Options:
(A) and (B) are correct.
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hookeβs law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):