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Electricity and Magnetism
Mathematical Tools and Fields
01Series Approximations: Keeping One or Two Terms02Integrals as Sums: Along a Line and a Curved Path03Line Integrals: Work as the Integral of F · ds04Closed Line Integrals: Work Around a Loop05Double Integrals: Area, Charge and Volume06Closed Surface Integrals: The Sphere and Its Charge07Electric Flux Through Surfaces and Volume IntegralsProblem set0/10Problem set 20/10MIT problem set0/4
01Field Theory Versus Action at a Distance02Scalar Fields: Contour, Color and Relief Maps03Vector Fields, Sources, Sinks and Divergence04Curl: Measuring the Circulation of a Field05Gravitational, Electric and Magnetic Fields06Drawing Vector Fields: Arrows, Lines and Grass SeedsProblem set0/10Problem set 20/10MIT problem set0/1
Electrostatics
01Coulomb's Law: Force Between Two Point Charges02Superposition: Adding Coulomb Forces as Vectors03Field Lines, Null Points and Uniform Fields04The Electric Dipole and Its 1/r³ Field05Torque, Energy and Force on a Dipole in a FieldProblem set0/10Problem set 20/10MIT problem set0/1

Torque, Energy and Force on a Dipole in a Field

Why does a dipole in a uniform field feel a torque but no net force, and what changes when the field is non-uniform?


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Your summary note

    1. 1

      Torque τ⃗=p⃗×E⃗\vec{\tau} = \vec{p} \times \vec{E}τ=p​×E in a uniform field

      Show the net force vanishes, compute r⃗+×F⃗++r⃗−×F⃗−\vec{r}_+ \times \vec{F}_+ + \vec{r}_- \times \vec{F}_-r+​×F+​+r−​×F−​ about the midpoint to get τ=pEsin⁡θ\tau = pE\sin\thetaτ=pEsinθ along −k^-\hat{k}−k^, and record the rotation of p⃗\vec{p}p​ toward E⃗\vec{E}E.

    2. 2

      Potential energy U=−p⃗⋅E⃗U = -\vec{p} \cdot \vec{E}U=−p​⋅E

      Integrate dW=−pEsin⁡θ dθdW = -pE\sin\theta\,d\thetadW=−pEsinθdθ from θ0\theta_0θ0​ to θ\thetaθ, take ΔU=−W\Delta U = -WΔU=−W, choose U(π/2)=0U(\pi/2) = 0U(π/2)=0, and reach U(θ)=−pEcos⁡θU(\theta) = -pE\cos\thetaU(θ)=−pEcosθ.

    3. 3

      Stable and unstable orientations

      Identify the stable minimum Umin⁡=−pEU_{\min} = -pEUmin​=−pE with p⃗\vec{p}p​ parallel to E⃗\vec{E}E and the unstable maximum Umax⁡=+pEU_{\max} = +pEUmax​=+pE with p⃗\vec{p}p​ anti-parallel.

    4. 4

      Net force p dEdxp\,\frac{dE}{dx}pdxdE​ in a non-uniform field

      Expand the field to first order about the dipole's center to derive F⃗e=p (dE/dx) i^\vec{F}_e = p\,(dE/dx)\,\hat{i}Fe​=p(dE/dx)i^, and record the charged comb picking up bits of paper through induced dipoles as the example.

    Attempt 1 of 2