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04-BS-9 · May 2014

Question 8 of 8: Velocity-Selector Capacitor Voltage for a Moving Electron

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Exams — May 2014 — 04-BS-9 Basic Electromagnetics. Three-hour, closed-book exam (approved Casio/Sharp calculator only). Aids given: $\varepsilon_0=8.85\times10^{-12}$ F/m, $\mu_0=4\pi\times10^{-7}$ H/m, $e=1.6\times10^{-19}$ C. Format: eight questions offered; any five constitute a complete paper and only the first five appearing in the answer book are marked. All eight are solved below for completeness.

Reference texts: Sadiku, Elements of Electromagnetics / Hayt & Buck, Engineering Electromagnetics — electrostatics, Gauss's law, capacitance, magnetostatics, Faraday's law; Young & Freedman, University Physics with Modern Physics — induced EMF and AC quantities.

Question 8: Velocity-Selector Capacitor Voltage for a Moving Electron (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given.

QuantityValue
Electron speed $v$ (West)$1\times10^5$ m/s
Magnetic field $B$ (vertical, Down)$0.5$ T
Plate separation $d$$1$ mm $=1\times10^{-3}$ m

Find. The capacitor voltage, plate polarity, and plate orientation needed so the electric force exactly cancels the magnetic force on the electron.

S plate (+) N plate (−) e⁻ v (West) B (Down, into loop symbol) E (North) Plates vertical, facing North–South; V = 50 V
Electron moving West in a downward B field. The required E points North, so the South-facing plate is positive.

Approach. Compute the magnetic force on the electron with $\vec F=q\vec v\times\vec B$ (careful with the electron's negative charge), then find the electric field that produces an equal and opposite force, and finally the plate voltage and polarity that produce that field.

  1. Magnetic force direction and magnitude. Take East$=\hat x$, North$=\hat y$, Up$=\hat z$, so $\vec v=-v\hat x$ (West) and $\vec B=-B\hat z$ (Down). For the electron ($q=-e$): $$\vec F_B=q(\vec v\times\vec B)=(-e)\big[(-v\hat x)\times(-B\hat z)\big]=(-e)(vB)(\hat x\times\hat z)=(-e)(vB)(-\hat y)=evB\,\hat y$$ so $\vec F_B$ points North, magnitude $$F_B=evB=(1.6\times10^{-19})(10^5)(0.5)$$ $$F_B=\boxed{8.0\times10^{-15}\ \text{N, North}}$$
  2. Required electric field. Cancellation needs $\vec F_E=-\vec F_B$ (South) on the electron. Since $\vec F_E=q\vec E=-e\vec E$, a electron force to the South requires $\vec E$ pointing North: $$E=\frac{F_B}{e}=vB=(10^5)(0.5)$$ $$E=\boxed{5.0\times10^{4}\ \text{V/m, North}}$$
  3. Plate voltage, polarity and orientation. A uniform field points from the $+$ plate to the $-$ plate, so a North-pointing $E$ needs the South plate positive and the North plate negative, with both plates vertical and facing North–South (perpendicular to the required field): $$V=Ed=(5.0\times10^4)(1\times10^{-3})$$ $$V=\boxed{50\ \text{V, South plate positive, North plate negative}}$$
QuantityResult
Magnetic force on electron$8.0\times10^{-15}$ N, North
Required $E$$5.0\times10^4$ V/m, North
Capacitor voltage $V$$50$ V; South plate $+$, North plate $-$; plates vertical, facing N–S
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