Instructor: Jongeun Choi

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Presentation transcript:

Instructor: Jongeun Choi Time Response*, ME451 Instructor: Jongeun Choi * This presentation is created by Jongeun Choi and Gabrial Gomes

Zeros and poles of a transfer function Let G(s)=N(s)/D(s), then Zeros of G(s) are the roots of N(s)=0 Poles of G(s) are the roots of D(s)=0 Im(s) Re(s)

Theorems Initial Value Theorem Final Value Theorem If all poles of sX(s) are in the left half plane (LHP), then

DC gain or static gain of a stable system 1.4 1.2 1 0.8 0.6 0.4 0.2 0.5 1 1.5 2 2.5 3

DC Gain of a stable transfer function DC gain (static gain) : the ratio of the steady state output of a system to its constant input, i.e., steady state of the unit step response Use final value theorem to compute the steady state of the unit step response

Pure integrator ODE : Impulse response : Step response : If the initial condition is not zero, then : Physical meaning of the impulse response

First order system ODE : Impulse response : Step response : DC gain: (Use the final value theorem)

First order system If the initial condition was not zero, then Physical meaning of the impulse response

Matlab Simulation G=tf([0 5],[1 2]); impulse(G) step(G) Time constant

First order system response System transfer function :

First order system response System transfer function : Impulse response :

First order system response System transfer function : Impulse response :

First order system response System transfer function : Impulse response : Step response :

First order system response Im(s) Re(s)

First order system response Im(s) Unstable Re(s)

First order system response Im(s) Unstable -1 Re(s)

First order system response Im(s) Unstable Re(s) -2

First order system response Im(s) Unstable faster response slower response Re(s) constant

First order system – Time specifications.

First order system – Time specifications. Time specs: Steady state value : Time constant : Rise time : Time to go from to Settling time :

First order system – Simple behavior. No overshoot No oscillations

Second order system (mass-spring-damper system) ODE : Transfer function :

Polar vs. Cartesian representations. … Imaginary part (frequency) … Real part (rate of decay)

Polar vs. Cartesian representations. … Imaginary part (frequency) … Real part (rate of decay) Polar representation : … natural frequency … damping ratio

Polar vs. Cartesian representations. … Imaginary part (frequency) … Real part (rate of decay) Polar representation : … natural frequency … damping ratio

Polar vs. Cartesian representations. … Imaginary part (frequency) … Real part (rate of decay) Polar representation : … natural frequency … damping ratio Unless overdamped

Polar vs. Cartesian representations. System transfer function : Significance of the damping ratio : … Overdamped … Critically damped … Underdamped … Undamped

Polar vs. Cartesian representations. System transfer function : Significance of the damping ratio : … Overdamped … Critically damped … Underdamped … Undamped

Polar vs. Cartesian representations. System transfer function : Significance of the damping ratio : … Overdamped … Critically damped … Underdamped … Undamped

Polar vs. Cartesian representations. System transfer function : All 4 cases Unless overdamped Significance of the damping ratio : … Overdamped … Critically damped … Underdamped … Undamped

Underdamped second order system Two complex poles:

Underdamped second order system

Impulse response of the second order system

Matlab Simulation zeta = 0.3; wn=1; G=tf([wn],[1 2*zeta*wn wn^2]); impulse(G)

Unit step response of undamped systems DC gain :

Unit step response of undamped system

Matlab Simulation zeta = 0.3; wn=1; G=tf([wn],[1 2*zeta*wn wn^2]); step(G)

Second order system response. Stable 2nd order system: 2 distinct real poles A pair of repeated real poles A pair of complex poles Im(s) Unstable Re(s)

Second order system response. Stable 2nd order system: 2 distinct real poles A pair of repeated real poles A pair of complex poles Im(s) Unstable Re(s)

Second order system response. Stable 2nd order system: 2 distinct real poles A pair of repeated real poles A pair of complex poles Im(s) Unstable Re(s)

Second order system response. Stable 2nd order system: 2 distinct real poles A pair of repeated real poles negative real part A pair of complex poles zero real part Im(s) Unstable Re(s)

Second order system response. Stable 2nd order system: 2 distinct real poles A pair of repeated real poles negative real part A pair of complex poles zero real part Im(s) Unstable Re(s)

Second order system response. Stable 2nd order system: 2 distinct real poles A pair of repeated real poles negative real part A pair of complex poles zero real part Im(s) Unstable Re(s)

Second order system response. Im(s) 2 distinct real poles = Overdamped Unstable Re(s)

Second order system response. Im(s) Repeated real poles = Critically damped Unstable Re(s)

Second order system response. Im(s) Complex poles negative real part = Underdamped Unstable Re(s)

Second order system response. Im(s) Complex poles zero real part = Undamped Unstable Re(s)

Second order system response. Im(s) Underdamped Unstable Undamped Overdamped or Critically damped Re(s) Underdamped

Overdamped system response System transfer function : Impulse response : Step response :

Overdamped and critically damped system response.

Overdamped and critically damped system response.

Overdamped and critically damped system response.

Overdamped and critically damped system response.

Polar vs. Cartesian representations.

Polar vs. Cartesian representations. System transfer function : All 4 cases Unless overdamped … Cartesian overdamped Significance of the damping ratio : … Overdamped … Critically damped … Underdamped … Undamped

Polar vs. Cartesian representations. System transfer function : All 4 cases Unless overdamped … Cartesian overdamped Significance of the damping ratio : … Overdamped … Critically damped … Underdamped … Undamped

Polar vs. Cartesian representations. System transfer function : All 4 cases Unless overdamped … Cartesian overdamped Significance of the damping ratio : … Overdamped Overdamped case: … Critically damped … Underdamped … Undamped

Second order impulse response – Underdamped and Undamped

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order impulse response – Underdamped and Undamped Increasing / Fixed

Second order step response – Underdamped and Undamped

Second order impulse response – Underdamped and Undamped Higher frequency oscillations Faster response Slower response Unstable Lower frequency oscillations

Second order impulse response – Underdamped and Undamped Less damping Unstable More damping

Second order step response – Time specifications. 1.4 1.2 1 0.8 0.6 0.4 0.2 0.5 1 1.5 2 2.5 3

Second order step response – Time specifications. … Steady state value. … Time to reach first peak (undamped or underdamped only). … % of in excess of . … Time to reach and stay within 2% of . 1.4 1.2 1 0.8 0.6 0.4 0.2 0.5 1 1.5 2 2.5 3

Second order step response – Time specifications. … Steady state value. More generally, if the numerator is not , but some :

Second order step response – Time specifications. … Peak time. Therefore, is the time of the occurrence of the first peak :

Second order step response – Time specifications. … Percent overshoot. Evaluating at , is defined as: Substituting our expressions for and :

Second order step response – Time specifications. … Settling time. Defining with , the previous expression for can be re-written as: As an approximation, we find the time it takes for the exponential envelope to reach 2% of . when

Typical specifications for second order systems. How many independent parameters can we specify? 3