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Chebyshev poles lie on an ellipse

Short answer

Poles are σ_k = –sinh a sinθ_k, ω_k = cosh a cosθ_k, θ_k=(2k–1)π/(2n), a=(1/n)sinh⁻¹(1/ε). Eliminating θ_k gives σ²/sinh²a + ω²/cosh²a = 1, an ellipse; semi-minor axis = sinh a (σ-axis), semi-major = cosh a (jω-axis), foci at ±j1.

Show that the poles of chebyshev filter lie on an ellipse. Also show the major and minor axes.

The poles of a Chebyshev low-pass filter lie on an ellipse whose semi-minor axis is sinh⁡a\sinh a (along the real axis) and whose semi-major axis is cosh⁡a\cosh a (along the imaginary axis), where a=1nsinh⁡−1(1/ε)a = \frac{1}{n}\sinh^{-1}(1/\varepsilon).

Finding the poles

The normalized Chebyshev response is ∣T(jω)∣2=11+ε2Cn2(ω)|T(j\omega)|^2 = \dfrac{1}{1+\varepsilon^2 C_n^2(\omega)} with Cn(ω)=cos⁡(ncos⁡−1ω)C_n(\omega) = \cos(n\cos^{-1}\omega). Replacing ω\omega by s/js/j, the poles satisfy

1+ε2Cn2(s/j)=0  ⇒  cos⁡[ncos⁡−1(s/j)]=±jε1 + \varepsilon^2 C_n^2(s/j) = 0 \;\Rightarrow\; \cos\left[n\cos^{-1}(s/j)\right] = \pm\frac{j}{\varepsilon}

Let cos⁡−1(s/j)=u+jv\cos^{-1}(s/j) = u + jv. Then

cos⁡(nu)cosh⁡(nv)−jsin⁡(nu)sinh⁡(nv)=±jε\cos(nu)\cosh(nv) - j\sin(nu)\sinh(nv) = \pm\frac{j}{\varepsilon}
  • Real part: cos⁡(nu)cosh⁡(nv)=0\cos(nu)\cosh(nv) = 0. Since cosh⁡(nv)≥1\cosh(nv) \ge 1, cos⁡(nu)=0\cos(nu) = 0, so uk=(2k−1)π2nu_k = \dfrac{(2k-1)\pi}{2n}, k=1,…,2nk = 1,\dots,2n.
  • Imaginary part: with sin⁡(nuk)=±1\sin(nu_k) = \pm1, sinh⁡(nv)=1/ε\sinh(nv) = 1/\varepsilon, so v=a=1nsinh⁡−11εv = a = \dfrac{1}{n}\sinh^{-1}\dfrac{1}{\varepsilon}.

Now s=jcos⁡(uk+ja)=j[cos⁡ukcosh⁡a−jsin⁡uksinh⁡a]s = j\cos(u_k + ja) = j[\cos u_k\cosh a - j\sin u_k\sinh a]:

sk=σk+jωk=sin⁡uksinh⁡a+jcos⁡ukcosh⁡as_k = \sigma_k + j\omega_k = \sin u_k \sinh a + j\cos u_k \cosh a

The left-half-plane poles (for a stable filter) are

σk=−sinh⁡a sin⁡uk,ωk=cosh⁡a cos⁡uk,k=1,…,n\sigma_k = -\sinh a\,\sin u_k, \qquad \omega_k = \cosh a\,\cos u_k, \qquad k = 1,\dots,n

Showing the locus is an ellipse

(σksinh⁡a)2+(ωkcosh⁡a)2=sin⁡2uk+cos⁡2uk=1\left(\frac{\sigma_k}{\sinh a}\right)^2 + \left(\frac{\omega_k}{\cosh a}\right)^2 = \sin^2u_k + \cos^2u_k = 1

This is an ellipse centred at the origin.

Major and minor axes

AxisDirectionHalf-lengthFull length
Majorjωj\omega axiscosh⁡a\cosh a2cosh⁡a2\cosh a
Minorσ\sigma axissinh⁡a\sinh a2sinh⁡a2\sinh a

Since cosh⁡2a−sinh⁡2a=1\cosh^2 a - \sinh^2 a = 1, the foci are at s=±j1s = \pm j1.

              jw
              |  cosh a
        x . . + . . o
      .       |       .
 ----x--------+--------o---- sigma
   -sinh a    |      sinh a
      .       |       .
        x . . + . . o
              |
   x = LHP poles used, o = RHP mirror

Geometric construction: draw two circles of radius sinh⁡a\sinh a and cosh⁡a\cosh a; draw radial lines at angles uku_k from the jωj\omega axis. Each pole takes its real part from the small circle and its imaginary part from the large circle (compare: Butterworth poles lie on the unit circle).

✓ Answer checked by Claude Sonnet 5.5

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