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Question: A proton moving with a constant velocity passes through a region of space without any change in its ...

A proton moving with a constant velocity passes through a region of space without any change in its velocity. If E and B represent the electric and magnetic fields respectively identify which of the following options can be true for the space.
A) E=0,B=0E = 0,B = 0
B) E=0,B0E = 0,B \ne 0
C) E0,B=0E \ne 0,B = 0
D) E0,B0E \ne 0,B \ne 0

Explanation

Solution

When a charge particle moving in magnetic field then a magnetic forceFm{F_m} acts on the charge particle the direction of magnetic force can be find by the Fleming's left hand rule
And we also know that when a charge particle placed in an electric field then an electric forceFe{F_e}stats act on it in the direction of the field on positive charge.

Step by step solution:
Let’s talk about option A
When E=0,B=0E = 0,B = 0
In this condition when electric field is zero then electric force on proton will be zero
i.e. Fe=0{F_e} = 0
B=0B = 0 So the magnetic force on moving charge also will be zero
i.e. Fm=0{F_m} = 0
Means when both forces are zero so proton can pass space without changing their velocity
Now option B
When E=0E = 0 then the electric force on the proton will be zero
i.e. Fe=0{F_e} = 0
But when B0B \ne 0 then magnetic force may not be zeroFm0{F_m} \ne 0
Due to magnetic force the direction of proton will be change means velocity of proton may be change
Now option C
When E0E \ne 0 then electric force Fe0{F_e} \ne 0
When B=0B = 0 then Fm=0{F_m} = 0
Due to electric force the velocity of proton may be change
Now option D
When E0E \ne 0 then there is an electric force Fe=qE{F_e} = qE
And when B0B \ne 0 then there is a magnetic force Fm=qvBsinθ{F_m} = qvB\sin \theta
It may be possible these force are equal and opposite to each other in a particular situation so when the net force on proton will zero then velocity of proton will not change

Hence option A and option D will be correct here

Note: When a proton moving in magnetic field then magnetic force can be defined as Fm=qvBsinθ{F_m} = qvB\sin \theta
Where qq \Rightarrow charge of moving particle for proton +e + e
vv \Rightarrow Velocity of charge
BB \Rightarrow Magnetic field
θ\theta \Rightarrow Is the angle between velocity and magnetic field
When a charge particle placed in electric field then electric force can be defined as Fe=qE{F_e} = qE
Where qq \Rightarrow charge of particle
EE \Rightarrow Electric field intensity