In this problem, we need to analyze the interactions of a proton moving through a region of space with electric and magnetic fields. We are given that the proton moves with constant velocity, indicating that the net force on it is zero.
The forces experienced by a charged particle (like a proton) moving in electric and magnetic fields are given by the Lorentz force law:
\(F = q(\vec{E} + \vec{v} \times \vec{B})\)
where:
For the proton to continue moving with constant velocity, the net force \(F\) must be zero:
\(\vec{E} + \vec{v} \times \vec{B} = 0\)
We will now analyze each given scenario:
Based on this analysis, the options where the proton can move with constant velocity are (A), (B), and (D).
For a proton to move with a constant velocity without any change, the net force on the particle must be zero. This implies:
\( q\vec{E} + q\vec{v} \times \vec{B} = 0 \)
Possible cases that satisfy this condition are:
Step 1. Case (A): \( \vec{E} = 0 \) and \( \vec{B} = 0 \) — No electric or magnetic fields are present, so no force acts on the proton.
Step 2. Case (B): \( \vec{E} = 0 \) and \( \vec{B} \neq 0 \) — The proton experiences no electric force, and if \( \vec{v} \) and \( \vec{B} \) are parallel, \( \vec{v} \times \vec{B} = 0 \).
Step 3. Case (D): \( \vec{E} \neq 0 \) and \( \vec{B} \neq 0 \) — Here, \( q\vec{E} \) and \( q\vec{v} \times \vec{B} \) can cancel each other out if they are equal in magnitude and opposite in direction.
Thus, the region of space may satisfy cases (A), (B), and (D), so the correct answer is (3).
Consider the following statements:
A. The junction area of a solar cell is made very narrow compared to a photodiode.
B. Solar cells are not connected with any external bias.
C. LED is made of lightly doped p-n junction.
D. Increase of forward current results in a continuous increase in LED light intensity.
E. LEDs have to be connected in forward bias for emission of light.
Match List - I with List - II:
List - I:
(A) Electric field inside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(B) Electric field at distance \( r > 0 \) from a uniformly charged infinite plane sheet with surface charge density \( \sigma \).
(C) Electric field outside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(D) Electric field between two oppositely charged infinite plane parallel sheets with uniform surface charge density \( \sigma \).
List - II:
(I) \( \frac{\sigma}{\epsilon_0} \)
(II) \( \frac{\sigma}{2\epsilon_0} \)
(III) 0
(IV) \( \frac{\sigma}{\epsilon_0 r^2} \) Choose the correct answer from the options given below: