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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

Series Approximations: Keeping One or Two Terms

Why do the first one or two terms of a series expansion carry nearly all the physics when x is small?


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    1. 1

      Truncating f(x)=a0+a1x+a2x2+…f(x) = a_0 + a_1 x + a_2 x^2 + \ldotsf(x)=a0​+a1​x+a2​x2+… when ∣x∣≪1|x| \ll 1∣x∣≪1

      Write the series expansion, state that for ∣x∣≪1|x| \ll 1∣x∣≪1 only the first one or two terms are kept, and record that the aim is a simple form to compare with another formula or experiment.

    2. 2

      Casting an expression into the form (1+x)m(1+x)^m(1+x)m

      Factor bbb out of (b−y)−1/3(b - y)^{-1/3}(b−y)−1/3, identify m=−1/3m = -1/3m=−1/3 and x=−y/bx = -y/bx=−y/b, and carry the signs through to b−1/3(1+y3b)b^{-1/3}\left(1 + \frac{y}{3b}\right)b−1/3(1+3by​) for y/b≪1y/b \ll 1y/b≪1.

    3. 3

      The standard small-xxx expansions

      List (1+x)m≈1+mx(1+x)^m \approx 1 + mx(1+x)m≈1+mx, sin⁡x≈x\sin x \approx xsinx≈x, cos⁡x≈1−x22\cos x \approx 1 - \frac{x^2}{2}cosx≈1−2x2​, tan⁡x≈x\tan x \approx xtanx≈x, ln⁡(1+x)≈x\ln(1+x) \approx xln(1+x)≈x and ex≈1+xe^x \approx 1 + xex≈1+x, and record that trigonometric angles are in radians.

    4. 4

      The general expansion and the tangent line f(0)+f′(0) xf(0) + f'(0)\,xf(0)+f′(0)x

      Write f(x)≈f(0)+f′(0) x+f′′(0)2!x2f(x) \approx f(0) + f'(0)\,x + \frac{f''(0)}{2!}x^2f(x)≈f(0)+f′(0)x+2!f′′(0)​x2 with the derivatives evaluated at x=0x = 0x=0, and state that the first two terms are the tangent line to the graph at x=0x = 0x=0.

    Attempt 1 of 2