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Electric Potential & Energy

The electric potential $V$ is a scalar field whose negative gradient gives $\vec E$. Working with $V$ is usually easier than with $\vec E$ directly: it's a scalar sum rather than a vector sum. The energy stored in an electric field is $u=\varepsilon_0 E^2/2$ per unit volume.

Key Concepts

Electric Potential
V(rβƒ—)=βˆ’βˆ«Orβƒ—Eβƒ—β‹…dlβƒ—V(\vec r)=-\int_{\mathcal{O}}^{\vec r}\vec E\cdot d\vec l (reference point O\mathcal{O} usually at infinity). For a point charge: V=kq/rV=kq/r. Eβƒ—=βˆ’βˆ‡V\vec E=-\nabla V.
Superposition
VV is a scalar, so the potential of multiple charges is the algebraic sum: V=βˆ‘ikqi/riV=\sum_i kq_i/r_i. Much simpler than the vector sum for Eβƒ—\vec E.
Energy of a Charge Distribution
The energy stored in assembling a continuous charge distribution: W=Ξ΅02∫E2 d3rW=\frac{\varepsilon_0}{2}\int E^2\,d^3r. Energy density: u=Ξ΅0E2/2u=\varepsilon_0 E^2/2.
Method of Images
A point charge +q+q at height dd above a grounded infinite conductor can be replaced by +q+q plus an image charge βˆ’q-q at depth dd below the surface. The boundary condition V=0V=0 at the surface is automatically satisfied.

Key Equations

Potential of point charge
V=14πΡ0qrV = \frac{1}{4\pi\varepsilon_0}\frac{q}{r}
Scalar; superpose for multiple charges.
Energy density
u=Ξ΅02E2=12ΞΌ0B2u = \frac{\varepsilon_0}{2}E^2 = \frac{1}{2\mu_0}B^2
Energy stored per unit volume in EM fields.
Energy of point charges
W=12βˆ‘iqiV(rβƒ—i)W = \frac{1}{2}\sum_i q_i V(\vec{r}_i)
Total electrostatic energy; factor Β½ avoids double-counting.
Worked Example

Potential of Two Charges

Problem

Charge q1=+3.0q_1=+3.0 nC is at the origin and q2=βˆ’1.0q_2=-1.0 nC is at x=0.40x=0.40 m. Find the potential at P=(0.40,0.30,0)P=(0.40,0.30,0) m.

Solution

Distance from q1q_1 to PP: r1=0.16+0.09=0.50r_1=\sqrt{0.16+0.09}=0.50 m.

Distance from q2q_2 to PP: r2=(0.40βˆ’0.40)2+0.09=0.30r_2=\sqrt{(0.40-0.40)^2+0.09}=0.30 m.

V=k(q1r1+q2r2)=8.99Γ—109(3Γ—10βˆ’90.50+βˆ’10βˆ’90.30)V = k\left(\frac{q_1}{r_1}+\frac{q_2}{r_2}\right) = 8.99\times10^9\left(\frac{3\times10^{-9}}{0.50}+\frac{-10^{-9}}{0.30}\right)
V=8.99Γ—109(6Γ—10βˆ’9βˆ’3.33Γ—10βˆ’9)=8.99Γ—109Γ—2.67Γ—10βˆ’9=24.0Β VV = 8.99\times10^9(6\times10^{-9}-3.33\times10^{-9}) = 8.99\times10^9\times2.67\times10^{-9} = 24.0\text{ V}
Answer V=24.0V=24.0 V.
Practice

Exercises

7 problems
1 of 7

Find the potential VV (in V) at r=0.30r=0.30 m from a point charge Q=5.0Γ—10βˆ’9Q=5.0\times10^{-9} C. (k=8.99Γ—109k=8.99\times10^9 NΒ·mΒ²/CΒ².)

V
2 of 7

Work done moving charge q=2.0Γ—10βˆ’9q=2.0\times10^{-9} C from r1=0.50r_1=0.50 m to r2=0.20r_2=0.20 m from a fixed charge Q=4.0Γ—10βˆ’9Q=4.0\times10^{-9} C. W=q(V2βˆ’V1)=qkQ(1/r2βˆ’1/r1)W=q(V_2-V_1)=qkQ(1/r_2-1/r_1) (in J).

J
3 of 7

Energy stored assembling two charges q1=q2=1.0Γ—10βˆ’9q_1=q_2=1.0\times10^{-9} C separated by d=0.10d=0.10 m (in J). W=kq1q2/dW=kq_1q_2/d.

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4 of 7

Energy density in a uniform E=1000E=1000 N/C field (in J/mΒ³). u=Ξ΅0E2/2u=\varepsilon_0 E^2/2.

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5 of 7

A charge q=+1.0Γ—10βˆ’9q=+1.0\times10^{-9} C is at distance d=0.10d=0.10 m above a grounded conductor. The image charge is βˆ’1.0Γ—10βˆ’9-1.0\times10^{-9} C. Find the attractive force (in N) between the charge and its image (2d2d apart).

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6 of 7

A capacitor has Q=3.0Γ—10βˆ’6Q=3.0\times10^{-6} C on plates with area A=0.010A=0.010 mΒ² and separation d=0.001d=0.001 m (Ξ΅0=8.85Γ—10βˆ’12\varepsilon_0=8.85\times10^{-12}). Find the electric field E=Οƒ/Ξ΅0E=\sigma/\varepsilon_0 (in N/C). Οƒ=Q/A\sigma=Q/A.

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7 of 7

For the same capacitor, find the energy stored (in J). U=Q2/(2C)=Ξ΅0E2Ad/2U=Q^2/(2C)=\varepsilon_0 E^2 Ad/2. C=Ξ΅0A/d=8.85Γ—10βˆ’12Γ—0.01/0.001=8.85Γ—10βˆ’11C=\varepsilon_0 A/d=8.85\times10^{-12}\times0.01/0.001=8.85\times10^{-11} F.

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Key Takeaways

  • VV is a scalar β€” superpose algebraically. Then Eβƒ—=βˆ’βˆ‡V\vec E=-\nabla V gives the field.
  • Work done moving charge qq through potential difference Ξ”V\Delta V: W=qΞ”VW=q\Delta V.
  • Energy density u=Ξ΅0E2/2u=\varepsilon_0E^2/2 tells you where the electromagnetic energy is stored.
  • Method of images solves boundary value problems by replacing the conductor with image charges that maintain the boundary condition.