Lecture 9 Notes: Mapping the s-plane to the z-plane

Lecture 9: Mapping the s-plane to the z-plane

Overview

  • This lecture focuses on mapping the s-plane to the z-plane.
  • The aim is to establish how domains in the s-plane change under the z-operator.

Objectives

  1. Revise the influence of s-plane poles on input responses.
  2. Map the s-plane into the z-plane.
  3. Review several examples.

Characteristic Roots and Stability

  • The general form of a second-order system is given by: <br/>y¨+2ζω<em>0y˙+ω</em>02y=u<br/><br /> ÿ + 2ζω<em>0ẏ + ω</em>0^2y = u<br />
  • The characteristic roots (λ) are determined by: <br/>λ<em>1,2=ω</em>0(ζ±ζ21)<br/><br /> λ<em>{1,2} = −ω</em>0(ζ ± \sqrt{ζ^2 − 1})<br />

Stability Regions

  • Relationship between s-plane and z-plane:
    <br/>s=σ+jω    z=esT=eσTejωT<br/><br /> s = σ + jω \implies z = e^{sT} = e^{σT} ⋅ e^{jωT}<br />

Mapping the s-plane to the z-plane

  • The mapping esTe^{sT} is periodic with a period of jωs=j2πTjω_s = j\frac{2π}{T} because:
    <br/>e(s+2πjT)T=esTe2πj=esT<br/><br /> e^{(s+ \frac{2πj}{T})T} = e^{sT}e^{2πj} = e^{sT}<br />

Example 1: Pole at z = 1 - Critically Stable, No Oscillations

  • Transfer function:
    <br/>Y(z)U(z)=zz1=11z1<br/><br /> \frac{Y(z)}{U(z)} = \frac{z}{z-1} = \frac{1}{1-z^{-1}}<br />
  • Difference equation:
    <br/>y<em>n=y</em>n1+un<br/><br /> y<em>n = y</em>{n-1} + u_n<br />
  • Impulse response (where un=1u_n = 1 for n=0n = 0 and 00 for n1n ≥ 1):
    • y<em>0=y</em>1+u0=0+1=1y<em>0 = y</em>{-1} + u_0 = 0 + 1 = 1
    • y<em>1=y</em>0+u1=1+0=1y<em>1 = y</em>0 + u_1 = 1 + 0 = 1
    • y<em>2=y</em>1+u2=1+0=1y<em>2 = y</em>1 + u_2 = 1 + 0 = 1
    • y<em>3=y</em>2+u3=1+0=1y<em>3 = y</em>2 + u_3 = 1 + 0 = 1

Example 2: Pole at z = 0.6 - Stable, No Oscillations

  • Transfer function:
    <br/>Y(z)U(z)=zz0.6=110.6z1<br/><br /> \frac{Y(z)}{U(z)} = \frac{z}{z-0.6} = \frac{1}{1-0.6z^{-1}}<br />
  • Difference equation:
    <br/>y<em>n=0.6y</em>n1+un<br/><br /> y<em>n = 0.6y</em>{n-1} + u_n<br />
  • Impulse response (where un=1u_n = 1 for n=0n = 0 and 00 for n1n ≥ 1):
    • y<em>0=0.6y</em>1+u0=0+1=1y<em>0 = 0.6y</em>{-1} + u_0 = 0 + 1 = 1
    • y<em>1=0.6y</em>0+u1=0.6×1+0=0.6y<em>1 = 0.6y</em>0 + u_1 = 0.6 × 1 + 0 = 0.6
    • y<em>2=0.6y</em>1+u2=0.6×0.6+0=0.36y<em>2 = 0.6y</em>1 + u_2 = 0.6 × 0.6 + 0 = 0.36
    • y<em>3=0.6y</em>2+u3=0.6×0.36+0=0.216y<em>3 = 0.6y</em>2 + u_3 = 0.6 × 0.36 + 0 = 0.216

Example 3: Pole at z = -1 - Critically Stable, With Oscillations

  • Transfer function:
    <br/>Y(z)U(z)=zz+1=11+z1<br/><br /> \frac{Y(z)}{U(z)} = \frac{z}{z+1} = \frac{1}{1+z^{-1}}<br />
  • Difference equation:
    <br/>y<em>n=y</em>n1+un<br/><br /> y<em>n = -y</em>{n-1} + u_n<br />
  • Impulse response (where un=1u_n = 1 for n=0n = 0 and 00 for n1n ≥ 1):
    • y<em>0=y</em>1+u0=0+1=+1y<em>0 = -y</em>{-1} + u_0 = 0 + 1 = +1
    • y<em>1=y</em>0+u1=1+0=1y<em>1 = -y</em>0 + u_1 = -1 + 0 = -1
    • y<em>2=y</em>1+u2=(1)+0=+1y<em>2 = -y</em>1 + u_2 = -(-1) + 0 = +1
    • y<em>3=y</em>2+u3=1+0=1y<em>3 = -y</em>2 + u_3 = -1 + 0 = -1

Example 4: Pole at z = -0.6 - Stable, With Oscillations

  • Transfer function:
    <br/>Y(z)U(z)=zz+0.6=11+0.6z1<br/><br /> \frac{Y(z)}{U(z)} = \frac{z}{z+0.6} = \frac{1}{1+0.6z^{-1}}<br />
  • Difference equation:
    <br/>y<em>n=0.6y</em>n1+un<br/><br /> y<em>n = -0.6y</em>{n-1} + u_n<br />
  • Impulse response (where u(nT)=1u(nT) = 1 for n=0n = 0 and 00 for n1n ≥ 1):
    • y<em>0=0.6y</em>1+u0=0+1=1y<em>0 = -0.6y</em>{-1} + u_0 = 0 + 1 = 1
    • y<em>1=0.6y</em>0+u1=0.6×1+0=0.6y<em>1 = -0.6y</em>0 + u_1 = -0.6 × 1 + 0 = -0.6
    • y<em>2=0.6y</em>1+u2=0.6×0.6+0=+0.36y<em>2 = -0.6y</em>1 + u_2 = 0.6 × 0.6 + 0 = +0.36
    • y<em>3=0.6y</em>2+u3=0.6×0.36+0=0.216y<em>3 = -0.6y</em>2 + u_3 = -0.6 × 0.36 + 0 = -0.216

Summary: Mapping the s-plane to the z-plane

  • The influence of s-plane poles on input responses.
  • Mapped the s-plane into the z-plane.
  • Reviewed several examples.

Reading

  • Ogata’95, Sections 4.1 and 4.2.

Next Lecture

  • Lecture 10: Digital control design in the w-domain.