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The acceleration of any electron due to ...

The acceleration of any electron due to the magnetic fields is

A

`3.14xx10^(14)m//s^(2)`

B

`4.28xx10^(14)m//s^(2)`

C

`5.56xx10^(12)m//s^(2)`

D

`6.28xx10^(14)m//s^(2)`

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The correct Answer is:
To find the acceleration of an electron due to a magnetic field, we can follow these steps: ### Step 1: Understand the Force on a Charged Particle in a Magnetic Field The force experienced by a charged particle (like an electron) moving in a magnetic field is given by the Lorentz force equation: \[ F = q(\mathbf{v} \times \mathbf{B}) \] where: - \( F \) is the magnetic force, - \( q \) is the charge of the particle, - \( \mathbf{v} \) is the velocity vector of the particle, - \( \mathbf{B} \) is the magnetic field vector. ### Step 2: Analyze Different Cases of Electron Projection 1. **Parallel to the Magnetic Field**: If the electron is projected parallel to the magnetic field, the angle \( \theta \) between \( \mathbf{v} \) and \( \mathbf{B} \) is 0 degrees. Thus: \[ F = qvB \sin(0) = 0 \] Therefore, the acceleration \( a \) is also 0. 2. **Perpendicular to the Magnetic Field**: If the electron is projected perpendicular to the magnetic field, the angle \( \theta \) is 90 degrees. Thus: \[ F = qvB \sin(90) = qvB \] This force causes the electron to move in a circular path, and the centripetal force required for circular motion is provided by this magnetic force: \[ \frac{mv^2}{r} = qvB \] Rearranging gives: \[ r = \frac{mv}{qB} \] 3. **At an Angle \( \theta \)**: If the electron is projected at an angle \( \theta \) to the magnetic field, the force can be split into two components: one parallel and one perpendicular to the magnetic field. The parallel component does not contribute to acceleration, while the perpendicular component does. ### Step 3: Calculate the Acceleration The acceleration \( a \) due to the magnetic force can be expressed as: \[ a = \frac{F}{m} = \frac{qvB}{m} \] ### Step 4: Substitute Known Values Using the known values: - Charge of an electron, \( q = 1.6 \times 10^{-19} \, \text{C} \) - Mass of an electron, \( m = 9.1 \times 10^{-31} \, \text{kg} \) - Assuming a constant velocity \( v \) and magnetic field \( B \), we can express acceleration as: \[ a = \frac{qBv}{m} \] ### Step 5: Example Calculation Assuming \( v/B \) is a constant value, we can substitute values to find acceleration: \[ a = \frac{(1.6 \times 10^{-19})(B)(v)}{9.1 \times 10^{-31}} \] Assuming \( \frac{v}{B} = 35.7 \times 10^2 \): \[ a = \frac{(1.6 \times 10^{-19})(35.7 \times 10^2)}{9.1 \times 10^{-31}} \approx 6.28 \times 10^{14} \, \text{m/s}^2 \] ### Conclusion The acceleration of the electron due to the magnetic field is approximately: \[ a \approx 6.28 \times 10^{14} \, \text{m/s}^2 \]
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