The displacement: \[ x = 2R = \frac{2mv}{qB}. \] Substituting: \[ x = \frac{2\sqrt{2m(qV)}}{qB}. \] For \( \text{H}^+ \), \( x = 4 \, \text{cm} \). For \( A_M = 144 \): \[ x \propto \sqrt{m} \quad \Rightarrow \quad x = 48 \, \text{cm}. \]
The correct options are (A) and (B).
Step 1: The formula is given by:
\[ x = 2R = \frac{2mv}{qB} = 2 \sqrt{\frac{2m(e \Delta V)}{qB}} \]
For H+ ion, we have:
\[ x = 3.91 \, \text{cm} \quad \text{and} \quad x = 4 \, \text{cm}. \] Since (A) is correct, we move on to the next calculation.
Step 2: For m = 144 (mass of the proton), we get:
\[ x = 12 (x_{H^+}) = 48 \, \text{cm}. \] This shows that option (B) is correct.
Step 3: For the condition where 1 ≤ AM ≤ 196, we use the formula:
\[ (x_1 - x_0)_{\text{min}} = 2R_{196} - 2R_1 = (14 \times 4) - 4 = 52 \, \text{cm}. \] Thus, option (C) is incorrect.
Step 4: For AM = 196, the minimum width is given by:
\[ w_{\text{min}} = R_{196} = 28 \, \text{cm}. \] This shows that option (D) is incorrect.
Thus, the correct options are (A) and (B).
A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).
Due to presence of an em-wave whose electric component is given by \( E = 100 \sin(\omega t - kx) \, NC^{-1} \), a cylinder of length 200 cm holds certain amount of em-energy inside it. If another cylinder of same length but half diameter than previous one holds same amount of em-energy, the magnitude of the electric field of the corresponding em-wave should be modified as:
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: