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Question: An electron accelerated through a potential difference V in a uniform tranverse magnetic field moves...

An electron accelerated through a potential difference V in a uniform tranverse magnetic field moves in a circle of radius R. If the accelerating potential is increased to 2V, the electron in the same magnetic field will follow a circle of radius:

A

R

B

√2 R

C

2R

D

4R

Answer

√2 R

Explanation

Solution

Explanation of the solution:

  1. Energy gain: When an electron is accelerated through a potential difference VV, its kinetic energy (KEKE) increases by an amount equal to the work done by the electric field, which is eVeV. KE=eVKE = eV

  2. Velocity of the electron: The kinetic energy is also given by 12mv2\frac{1}{2}mv^2, where mm is the mass of the electron and vv is its velocity. 12mv2=eV\frac{1}{2}mv^2 = eV Solving for vv: v=2eVmv = \sqrt{\frac{2eV}{m}}

  3. Motion in a magnetic field: When an electron moves with velocity vv perpendicular to a uniform magnetic field BB, the magnetic force FB=evBF_B = evB provides the necessary centripetal force Fc=mv2RF_c = \frac{mv^2}{R} for it to move in a circle of radius RR. evB=mv2RevB = \frac{mv^2}{R}

  4. Radius in terms of velocity: From the force balance, we can express the radius RR: R=mveBR = \frac{mv}{eB}

  5. Radius in terms of potential difference: Substitute the expression for vv from step 2 into the equation for RR from step 4: R=meB2eVmR = \frac{m}{eB} \sqrt{\frac{2eV}{m}} To simplify, bring mm and ee inside the square root: R=1Bm2e22eVmR = \frac{1}{B} \sqrt{\frac{m^2}{e^2} \frac{2eV}{m}} R=1B2mVeR = \frac{1}{B} \sqrt{\frac{2mV}{e}}

  6. Relationship between R and V: From the derived formula, we can see that the radius RR is directly proportional to the square root of the accelerating potential VV (assuming mm, ee, and BB are constant): RVR \propto \sqrt{V}

  7. Calculate the new radius: Let R1R_1 be the initial radius when the potential is V1=VV_1 = V. Let R2R_2 be the new radius when the potential is V2=2VV_2 = 2V. R2R1=V2V1\frac{R_2}{R_1} = \frac{\sqrt{V_2}}{\sqrt{V_1}} R2R1=2VV\frac{R_2}{R_1} = \sqrt{\frac{2V}{V}} R2R1=2\frac{R_2}{R_1} = \sqrt{2} R2=2R1R_2 = \sqrt{2}R_1

Therefore, if the accelerating potential is increased to 2V2V, the electron will follow a circle of radius 2R\sqrt{2}R.