The Fourier transform arises when the period of a Fourier series tends to infinity.
Circle one: True False
A Fourier series on an interval of length L has discrete frequencies spaced 1 over L apart. What happens as L grows without bound?
- The frequencies spread further apart
- The frequencies stay exactly fixed
- The frequencies pack closer and the sum approaches an integral
The Fourier transform of a Gaussian bell curve is:
- A pure sine wave
- Another Gaussian
- Zero at every frequency
Zoe says the Fourier transform arises when the period of a Fourier series tends to infinity. Is Zoe right?
Circle one: True False
The Fourier transform of a Gaussian bell curve is:
- Another Gaussian
- An indicator function of an interval
- A pure sine wave
- Zero at every frequency
A Fourier series on an interval of length L has discrete frequencies spaced 1/L apart. What happens as L grows without bound?
- The frequencies pack closer together and the sum approaches an integral over all frequencies
- The frequencies spread further apart
- The frequencies stay exactly fixed
- Only whole number frequencies survive
Why do differential equations love the Fourier transform?
- Differentiation becomes multiplication by frequency, turning calculus into algebra
- It removes all constants from the equation
- It makes every function smooth
What does the Fourier inversion theorem say, roughly?
- Applying the transform twice, with matching normalisation, recovers the original function
- Every function equals its own Fourier transform
- The transform of any signal is zero
- Fourier series of smooth functions never converge
Fourier inversion holds for every function with no hypotheses at all.
Circle one: True False
The Fourier transform of the indicator function of an interval is a multiple of:
- sin(x)/x, a sinc function
- e to the x
- A step function
- A polynomial in x