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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 setProblem set 2MIT problem set
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 setProblem set 2MIT problem set
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 setProblem set 2MIT problem set
01Charge Density and the Field on a Rod's Axis02The Field on a Charged Rod's Perpendicular Bisector03The Fields of a Charged Ring and a Charged Disk04How Field Lines Carry Force, Energy and Momentum05Electric Pressure and Tension: The Stress ε₀E²/2Problem setProblem set 2MIT problem set
01The Six-Step Recipe for Continuous Charge Fields02Coulomb's Law in Numbers: Hydrogen and Millikan's Oil Drop03Deflecting an Electron Between Charged Plates04The Dipole Far Field and the Field of a Charged Arc05The Field Beside a Finite Rod: Two Components, Two End AnglesProblem setProblem set 2

The Dipole Far Field and the Field of a Charged Arc

How does a first-order Taylor expansion turn two point charges into the 1/r³ dipole field, and why is a ring's centre field zero?


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Questions

Work each one out before you check it. Every question has a scratch pad and a calculator.

  1. Question 1

    A charge +q+q+q sits at (0,A)(0, A)(0,A) and −q-q−q at (0,−A)(0, -A)(0,−A), with A=0.040 nmA = 0.040\ \text{nm}A=0.040 nm. A point P is r=2.0 nmr = 2.0\ \text{nm}r=2.0 nm from the origin at θ=60°\theta = 60\degreeθ=60° from the +y+y+y axis, and r−r_-r−​ is its distance from −q-q−q. Using the first-order binomial approximation, find (r/r−)3(r/r_-)^3(r/r−​)3 to three decimal places.

    (r/r−)3≈(r/r_-)^3 \approx(r/r−​)3≈
  2. Question 2

    Use ke=8.99×109 N m2/C2k_e = 8.99\times10^{9}\ \text{N}\,\text{m}^2/\text{C}^2ke​=8.99×109 Nm2/C2. A dipole of moment p=2.0×10−29 C mp = 2.0\times10^{-29}\ \text{C}\,\text{m}p=2.0×10−29 Cm is at the origin. At r=4.0 nmr = 4.0\ \text{nm}r=4.0 nm, θ=60°\theta = 60\degreeθ=60° from p⃗\vec{\mathbf{p}}p​, find ErE_rEr​ and EθE_\thetaEθ​ from the far-field formulas, in units of 106 N/C10^{6}\ \text{N/C}106 N/C to three significant figures.

    Er=E_r =Er​=×10⁶ N/C
    Eθ=E_\theta =Eθ​=×10⁶ N/C
  3. Question 3

    Use ke=8.99×109 N m2/C2k_e = 8.99\times10^{9}\ \text{N}\,\text{m}^2/\text{C}^2ke​=8.99×109 Nm2/C2. A dipole of moment p=6.0×10−30 C mp = 6.0\times10^{-30}\ \text{C}\,\text{m}p=6.0×10−30 Cm is at the origin. Find the far-field magnitude at r=3.0 nmr = 3.0\ \text{nm}r=3.0 nm, θ=30°\theta = 30\degreeθ=30° from p⃗\vec{\mathbf{p}}p​, in units of 106 N/C10^{6}\ \text{N/C}106 N/C to three significant figures.

    ∣E⃗∣=|\vec{\mathbf{E}}| =∣E∣=×10⁶ N/C
  4. Question 4

    At a point θ=50°\theta = 50\degreeθ=50° from a dipole's axis, far from the dipole, find the angle between E⃗\vec{\mathbf{E}}E and r^\hat{\mathbf{r}}r^, in degrees to one decimal place.

    °
  5. Question 5

    Use ke=8.99×109 N m2/C2k_e = 8.99\times10^{9}\ \text{N}\,\text{m}^2/\text{C}^2ke​=8.99×109 Nm2/C2. An arc of radius R=0.15 mR = 0.15\ \text{m}R=0.15 m with λ=4.0 nC/m\lambda = 4.0\ \text{nC/m}λ=4.0 nC/m runs from −30°-30\degree−30° to +30°+30\degree+30° about the xxx-axis. Find the field magnitude at its centre, in N/C to three significant figures.

    E=E =E=N/C
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