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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

Gravitational, Electric and Magnetic Fields

How does dividing force by a test mass or test charge turn gravity and Coulomb's law into fields?


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    1. 1

      Gravitational field g⃗=−GMr2r^\vec{g}=-\frac{GM}{r^2}\hat{r}g​=−r2GM​r^

      Derive g⃗\vec{g}g​ as the limit of F⃗g/m\vec{F}_g/mFg​/m from Newton's law, state its inward radial direction, and compute g=GM/RE2≈9.8 m/s2g=GM/R_E^2\approx 9.8\ \text{m/s}^2g=GM/RE2​≈9.8 m/s2 for the uniform field near the surface.

    2. 2

      Electric field E⃗=keQr2r^\vec{E}=k_e\frac{Q}{r^2}\hat{r}E=ke​r2Q​r^ of a point charge

      Define E⃗\vec{E}E as the limit of F⃗e/q\vec{F}_e/qFe​/q for a test charge, give its unit N/C, record outward for positive QQQ and inward for negative QQQ, and write F⃗e=qE⃗\vec{F}_e=q\vec{E}Fe​=qE.

    3. 3

      Sources of magnetic fields and their directions

      Record that like poles repel, compass needles align with B⃗\vec{B}B, moving charges create B⃗\vec{B}B, Earth's magnetic south pole lies in the north, and sketch a wire's circular field by the right-hand rule.

    Attempt 1 of 2