Skip to main content

FS coefficients; time scaling and conjugation

Short answer

Fourier coefficients a_k give amplitude, phase, and power of each harmonic; a_0 is the DC value. Time scaling: x(αt) has same a_k with scaled fundamental frequency αω0. Conjugation: x*(t) yields a*_{-k}.

What are the significance of Fourier series coefficients of a signal? State and prove time scaling and conjugation properties of continuous time Fourier series representation.

Significance of Fourier series coefficients

The coefficients ak=1T∫Tx(t)e−jkω0tdta_k = \frac{1}{T}\int_T x(t)e^{-jk\omega_0 t}dt describe the signal in the frequency domain:

  • ∣ak∣|a_k| gives the amplitude and ∠ak\angle a_k the phase of the kkth harmonic (frequency kω0k\omega_0); plotting them gives the magnitude and phase spectra.
  • a0a_0 is the dc (average) value of the signal.
  • ∣ak∣2|a_k|^2 is the power in the kkth harmonic, and by Parseval ∑∣ak∣2\sum|a_k|^2 is the total average power.
  • They show the bandwidth of the signal: how fast ∣ak∣|a_k| falls tells how many harmonics are needed (smooth signals need fewer).
  • An LTI system acts on each harmonic separately: the output coefficients are akH(jkω0)a_k H(jk\omega_0), which makes system analysis simple.

Time scaling property

Statement: if x(t)x(t) has period TT, ω0=2π/T\omega_0 = 2\pi/T, and x(t)⟷FSakx(t) \overset{FS}{\longleftrightarrow} a_k, then for α>0\alpha > 0, x(αt)x(\alpha t) has period T/αT/\alpha and

x(αt)=∑k=−∞∞akejk(αω0)tx(\alpha t) = \sum_{k=-\infty}^{\infty}a_k e^{jk(\alpha\omega_0)t}

i.e. the coefficients are unchanged but the fundamental frequency becomes αω0\alpha\omega_0.

Proof: let y(t)=x(αt)y(t) = x(\alpha t), period T′=T/αT' = T/\alpha; put τ=αt\tau = \alpha t:

bk=1T′∫0T′x(αt)e−jkαω0tdt=αT∫0Tx(τ)e−jkω0τdτα=ak\begin{aligned} b_k &= \frac{1}{T'}\int_0^{T'}x(\alpha t)e^{-jk\alpha\omega_0 t}dt \\ &= \frac{\alpha}{T}\int_0^{T}x(\tau)e^{-jk\omega_0\tau}\frac{d\tau}{\alpha} = a_k \end{aligned}

Conjugation property

Statement:

x∗(t)⟷FSa−k∗x^*(t) \overset{FS}{\longleftrightarrow} a_{-k}^*

Proof: take the conjugate of the synthesis equation:

x∗(t)=[∑k=−∞∞akejkω0t]∗=∑k=−∞∞ak∗e−jkω0t=∑m=−∞∞a−m∗ ejmω0t(m=−k)\begin{aligned} x^*(t) &= \left[\sum_{k=-\infty}^{\infty}a_k e^{jk\omega_0 t}\right]^* = \sum_{k=-\infty}^{\infty}a_k^* e^{-jk\omega_0 t} \\ &= \sum_{m=-\infty}^{\infty}a_{-m}^*\,e^{jm\omega_0 t} \qquad (m = -k) \end{aligned}

So the coefficient of ejmω0te^{jm\omega_0 t} in x∗(t)x^*(t) is a−m∗a_{-m}^*.

Consequence (conjugate symmetry): if x(t)x(t) is real, x(t)=x∗(t)x(t) = x^*(t), so ak=a−k∗a_k = a_{-k}^*. Hence ∣ak∣=∣a−k∣|a_k| = |a_{-k}| (even magnitude spectrum) and ∠a−k=−∠ak\angle a_{-k} = -\angle a_k (odd phase spectrum). If x(t)x(t) is also even, aka_k is real and even.

✓ Answer checked by Claude Opus 5.5 (high effort)

All Signals and Systems chapter 2 questions →