Fourier Series · seed 1 · A4, ink-friendly. The answer key prints on its own page for grown-ups.
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Repeating waves built from pure tones

Mathematics · Differential Equations · ages 20-21
Name ______________________   Date ____________
  1. Multiplying a Fourier series by cos(2x) and integrating over one full period leaves only the a2 term, because every other sine and cosine in the series integrates to zero against cos(2x).

    Circle one:   True   False

  2. A periodic signal is 5 on (0, π) and 1 on (π, 2π), repeating every 2π. What is the constant term a0/2 of its Fourier series?

    Answer: ______________

  3. A square wave is -1 on (-pi, 0) and +1 on (0, pi), repeating every 2 pi. It is odd. What does that say about its cosine coefficients?

    • Every an is 0
    • Every bn is 0
    • a0 is infinite
  4. The sawtooth f(x) = x on (-pi, pi) has Fourier sine coefficients bn = 2(-1)^(n+1)/n. What is b4?

    Answer: ______________

  5. What is a partial sum of a Fourier series?

    • The series stopped after a few terms
    • The sum of all the jump sizes in the wave
    • The constant average term a0 over 2 alone
  6. Near a jump discontinuity in the original function, what do the Fourier partial sums do?

    • Converge smoothly to the jump once enough terms are kept
    • Overshoot by about 9% of the jump, however many terms
    • Land exactly on the function's value at the jump
    • Drop to zero right at the jump
  7. A square wave jumps from -1 to +1 at x = 0. What value does its Fourier series take at x = 0?

    • 1
    • 0
    • -1
    • It does not converge there
  8. If you multiply a periodic function's Fourier series by sin(3x) and integrate over one full period, which coefficient does that isolate?

    • a0
    • a3
    • b3
    • b1
  9. Near the square wave jump, the partial sums overshoot no matter how many terms you keep. What should you conclude?

    • The coefficients must have been computed wrongly
    • Overshoot near jumps is built into the method
    • Only even functions ever overshoot at jumps
  10. A circuit is driven by a square wave. How does the series help solve it?

    • It replaces the whole circuit with a single resistor
    • It splits the drive into tones solved one at a time
    • It removes the need for any differential equation
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Answer key

For grown-ups. Fold this page away before handing over the rest.

Repeating waves built from pure tones W1-mt_DJ3iwfj7NK-s1

  1. True · This is exactly why the coefficient formulas work: orthogonality wipes out every term except the one you multiplied by.
  2. 3 · The constant term is the average over one period: (5 + 1)/2 = 3.
  3. Every an is 0 · Odd functions are built from sines alone, so no cosine survives.
  4. -0.5 · b4 = 2(-1)^5 / 4 = -2/4 = -0.5.
  5. The series stopped after a few terms · Keeping the first tones already sketches the wave well away from jumps.
  6. Overshoot by about 9% of the jump, however many terms · This is the Gibbs phenomenon: the overshoot's height stays fixed near 9% of the jump size, it just gets squeezed into a narrower spike as you add terms.
  7. 0 · At a jump the series converges to the midpoint of the two sides: (-1 + 1)/2 = 0.
  8. b3 · Every cosine term and every other sine term vanishes against sin(3x), leaving only b3.
  9. Overshoot near jumps is built into the method · The series struggles at discontinuities, and extra terms never fully fix the jump.
  10. It splits the drive into tones solved one at a time · Each tone drives its own easy single frequency problem, and the answers add up.
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