NivaarExam PrepOfficial exam papers ↗

04-BS-9 · May 2018

Question 2 of 8: Total Electrostatic Energy of a Charge Triangle with Protons at the Centroid

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

Notes on this paper

National Exams — May 2018 — 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 — Coulomb's law and Gauss's law for spherical and piecewise charge distributions, the Biot–Savart/Ampère law for finite, semi-infinite and arc-shaped conductors, Faraday's law for a loop crossing a spatially bounded field, the differential (point) form of Ampère's law, and series-layered parallel-plate capacitance; Young & Freedman, University Physics with Modern Physics — Snell's law and the geometry of apparent vs. real position across a refracting interface.

Question 2: Total Electrostatic Energy of a Charge Triangle with Protons at the Centroid (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
Triangle side $a$ (equilateral)$1\times10^{-10}$ m
Charge at each vertexone electron, $-e$ (three vertices)
Charge at the centroidthree protons together, $+3e$

Find. The total electrostatic potential energy of the four-charge assembly, relative to all four charges infinitely far apart.

−e −e −e +3e (centroid) R = a/√3 a
Equilateral triangle of electrons (side a) with three protons together at the centroid, at circumradius R=a/√3 from every vertex. Total energy sums all six unique pairwise Coulomb interactions.

Approach. Potential energy is a pairwise sum, $U=\sum_{i<j}\dfrac{q_iq_j}{4\pi\varepsilon_0r_{ij}}$, over every unique pair of the four charges: three vertex–vertex pairs at separation $a$, and three vertex–centroid pairs at separation $R=a/\sqrt3$ (the equilateral triangle's circumradius).

  1. Vertex–vertex contribution (3 pairs). Each pair is $(-e)(-e)=+e^2$ at separation $a$: $$U_{vv}=3\times\frac{e^2}{4\pi\varepsilon_0a}=\frac{3e^2}{4\pi\varepsilon_0a}$$
  2. Vertex–centroid contribution (3 pairs). Each pair is $(-e)(+3e)=-3e^2$ at separation $R=a/\sqrt3$: $$U_{vc}=3\times\frac{-3e^2}{4\pi\varepsilon_0(a/\sqrt3)}=\frac{-9\sqrt3\,e^2}{4\pi\varepsilon_0a}$$
  3. Total energy. Adding the two contributions, with $1/4\pi\varepsilon_0=8.99\times10^9$ N·m$^2$/C$^2$: $$U=U_{vv}+U_{vc}=\frac{e^2}{4\pi\varepsilon_0a}\left(3-9\sqrt3\right)$$ $$U=\frac{(8.99\times10^{9})(1.6\times10^{-19})^2}{1\times10^{-10}}(3-15.5885)$$ $$\boxed{U=-2.897\times10^{-17}\ \text{J}}$$
QuantityResult
Vertex–vertex energy $U_{vv}$ (3 pairs)$6.904\times10^{-18}$ J
Vertex–centroid energy $U_{vc}$ (3 pairs)$-3.588\times10^{-17}$ J
Total electrostatic energy $U$$-2.897\times10^{-17}$ J