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CTFS time reversal, scaling, frequency shift

Short answer

Time reversal: x(-t) ↔ a_{-k}. Time scaling: x(αt) has same coefficients a_k but period T/α and fundamental frequency αω0. Frequency shifting: e^{jMω0 t}x(t) ↔ a_{k-M}, moving the spectrum M places to the right.

Describe the continuous-time Fourier series' time reversal, time scaling, and frequency shifting properties.

Let x(t)x(t) be periodic with period TT, ω0=2π/T\omega_0 = 2\pi/T, and x(t)↔FSakx(t) \xleftrightarrow{FS} a_k.

Time reversal

x(−t)↔FSa−kx(-t) \xleftrightarrow{FS} a_{-k}

Put k=−mk = -m in the synthesis equation:

x(−t)=∑kake−jkω0t=∑ma−mejmω0tx(-t) = \sum_k a_k e^{-jk\omega_0 t} = \sum_m a_{-m}e^{jm\omega_0 t}

Reversing the signal in time reverses its coefficient sequence. If x(t)x(t) is even, a−k=aka_{-k} = a_k. If it is odd, a−k=−aka_{-k} = -a_k.

Time scaling

x(αt), α>0:x(αt)=∑kakejk(αω0)tx(\alpha t),\ \alpha > 0: \quad x(\alpha t) = \sum_k a_k e^{jk(\alpha\omega_0)t}

x(αt)x(\alpha t) has period T/αT/\alpha and fundamental frequency αω0\alpha\omega_0. The coefficients aka_k stay the same, and only the harmonic spacing changes from ω0\omega_0 to αω0\alpha\omega_0. Compressing the signal (α>1\alpha > 1) spreads the spectral lines apart.

Frequency shifting

ejMω0tx(t)↔FSak−Me^{jM\omega_0 t}x(t) \xleftrightarrow{FS} a_{k-M}

The coefficients of the product are

1T∫TejMω0tx(t)e−jkω0tdt=1T∫Tx(t)e−j(k−M)ω0tdt=ak−M\frac{1}{T}\int_T e^{jM\omega_0 t}x(t)e^{-jk\omega_0 t}dt = \frac{1}{T}\int_T x(t)e^{-j(k-M)\omega_0 t}dt = a_{k-M}

Multiplying by a harmonic exponential moves the whole line spectrum MM places to the right. This is the dual of the time-shift property.

✓ Answer checked by Claude Opus 5.5 (high effort)

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