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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

Integrals as Sums: Along a Line and a Curved Path

How does reading an integral sign as a sum of tiny pieces carry you from the x-axis to any curved path?


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    1. 1

      The integral as a limit of a sum: L=∫abdxL = \int_a^b dxL=∫ab​dx

      Write the length of a segment from x=ax=ax=a to x=bx=bx=b as ∑iΔxi\sum_i \Delta x_i∑i​Δxi​, pass to the limit Δx→dx\Delta x \rightarrow dxΔx→dx, and get L=b−aL = b - aL=b−a in meters.

    2. 2

      Total charge from a linear charge density λ\lambdaλ

      Define λ\lambdaλ in C/m, compute Q=λ(b−a)Q = \lambda(b-a)Q=λ(b−a) for uniform charge, then integrate λ(x)=kx2\lambda(x) = kx^2λ(x)=kx2 to get Q=k(b3−a3)3Q = \frac{k(b^3-a^3)}{3}Q=3k(b3−a3)​, and write the limit-of-sum definition ∑iλ(xi) Δxi\sum_i \lambda(x_i)\,\Delta x_i∑i​λ(xi​)Δxi​.

    3. 3

      The line integral along a curved path

      Sketch a curve from aaa to bbb with the displacement vector ds\mathbf{ds}ds tangent to it, state what its magnitude and direction are, and write LLL as the sum of the ∣ds∣|\mathbf{ds}|∣ds∣.

    Attempt 1 of 2