Fourier Transform Flashcards
the fourier transform and inverse fourier transform allow us to
move between conjugate spaces, such as time and frequency
the two most important integral transforms for physics
fourier transform and integral transform
fourier and laplace transforms both have the property that
the dimension of the original variable is the reciprocal of the target variable
considerations to get from fourier series to fourier transform
consider a function of time with period T
angular frequency of the rth component is wr=r2pi/T
delta w=2pi/T
make notation replacements to complex fourier series and complex fourier coefficients and combine
why is the 1/2pi split into two factors of 1/sqrt(2pi)
to make definitions of the fourier transform and inverse fourier transform as symmetrical as possible
The only requirement f(t) has to satisfy in order for its Fourier transform to exist is
integral from -infinity to infinity of |f(t)|dt is finite
The Fourier transform of a periodic function with frequency ω0 consists of
a series of narrow peaks
at the discrete frequencies nω0 (n = 1, 2, 3, . . .), which are exactly the frequencies represented
by the Fourier series expansion of f(t).
the fourier transform of spoke sound determines
what vowel we perceive it as
how is the fourier transform used to compress an image
the bits of the image that matter (the boundaries between different regions) have different frequency
components to the more homogenous parts, which can be removed without ruining our ability to identify shapes.
fourier transforming a function twice
gives almost the original function back
properties of the fourier transform
linearity
scaling
translation
differentiation
integration
linearity of fourier transforms
FT[af(t)+bg(t)] = aFT[f(t)] + bFT[g(t)]
scaling of fourier transforms
FT[f(at)]= 1/|a| FT(w/z)
translation of fourier transforms
FT[f(t+a)] = exp(iwa)FT(w)
fourier transform differentiation
FT[f’(t)]=iwFT(w)
FT[f^(n)(t)]=(iw)^n FT(w)