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Physics · Ch 10 — Electrostatics

Principle of Superposition

10.5

Principle of Superposition

The principle of superposition states that when a number of charges act simultaneously, the resultant (net) force on any one particular charge is found by taking the VECTOR SUM of the individual forces exerted on it by every other charge, considered ONE AT A TIME.

Consider a set of point charges q1,q2,q3,…q_1,q_2,q_3,\dots located at points A1,A2,A3,…A_1,A_2,A_3,\dots (Fig. 10.5). The force exerted on charge q1q_1 by q2q_2 alone, F⃗12\vec{F}_{12}, is calculated using ordinary Coulomb's law exactly as though every other charge simply were not there -- ignoring their presence entirely. In the same way, F⃗13\vec{F}_{13}, F⃗14\vec{F}_{14}, and so on, are computed one pairwise interaction at a time, each purely from Coulomb's law between just that pair. …

Figure 10.5Fig. 10.5: Principle of superposition

What this figure shows. A central charge q1q_1 at point A1A_1, surrounded by four other point charges q2,q3,q4,q5q_2,q_3,q_4,q_5 scattered at various positions and distances at points A2,A3,A4,A5A_2,A_3,A_4,A_5. Four separate force vectors, F⃗12,F⃗13,F⃗14,F⃗15\vec{F}_{12},\vec{F}_{13},\vec{F}_{14},\vec{F}_{15}, are drawn from q1q_1, each directed along the straight line joining q1q_1 to the respective other charge, representing the individual pairwise Coulomb force on q1q_1 due to each of the four surrounding charges considered one at a time. The figure establishes that the total/net force on q1q_1 is the VECTOR sum of these four individually-computed forces, never a simple scalar addi …

Misc Ex.4Example 10.4: Force on charge A due to charges B and C at the corners of a right triangle

Worked out. Charges of 2 μC2\,\mu C (A), 3 μC3\,\mu C (B) and 4 μC4\,\mu C (C) are placed with AB = 4.0 cm and BC = 3.0 cm at right angles, so AC=42+32=5.0AC=\sqrt{4^2+3^2}=5.0 cm. The force on A due to B alone is FAB=14πϵ0qAqBAB2=9×109×(2×10−6)(3×10−6)(0.04)2≈33.7F_{AB}=\frac{1}{4\pi\epsilon_0}\frac{q_Aq_B}{AB^2}=9\times10^9\times\frac{(2\times10^{-6})(3\times10^{-6})}{(0.04)^2}\approx33.7 N, directed along BA (away from B); the force on A due to C alone is FAC=9×109×(2×10−6)(4×10−6)(0.05)2≈28.8F_{AC}=9\times10^9\times\frac{(2\times10^{-6})(4\times10^{-6})}{(0.05)^2}\approx28.8 N, directed along CA (away from C). Using the triangle's geometry, the angle between F⃗AB\vec{F}_{AB} and F⃗AC\vec{F}_{AC} at A works out to ∠BAC≈36.9∘\angle BAC\approx36.9^\circ (from cos⁡(∠BAC)=AB2+AC2−BC22⋅AB⋅AC=0.8\cos(\angle BAC)=\frac{AB^2+AC^2-BC^2}{2\cdot AB\cdot AC}=0.8), so the resultant is F=FAB2+FAC2+2FABFACcos⁡(36.9∘)≈59.4F=\sqrt{F_{AB}^2+F_{AC}^2+2F_{AB}F_{AC}\cos(36.9^\circ)}\approx59.4 N, directed 16.9∘16.9^\circ north of west -- a full worked example of …