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ME- 495 Mechanical and Thermal Systems Lab Fall 2011 Chapter 5: MEASURING SYSTEM RESPONSE Professor: Sam Kassegne, PhD, PE.

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Presentation on theme: "ME- 495 Mechanical and Thermal Systems Lab Fall 2011 Chapter 5: MEASURING SYSTEM RESPONSE Professor: Sam Kassegne, PhD, PE."— Presentation transcript:

1 ME- 495 Mechanical and Thermal Systems Lab Fall 2011 Chapter 5: MEASURING SYSTEM RESPONSE Professor: Sam Kassegne, PhD, PE

2 Signal Response of Measurand?

3 RESPONSE System Response: an evaluation of the systems ability to faithfully sense, transmit and present all pertinent information included in the measurand and exclude all else: Key response characteristics/components are: –Amplitude response –Frequency response –Phase response –Slew Rate

4 COMPONENTS OF SYSTEM RESPONSE 1) Amplitude response: ability to treat all input amplitudes uniformly –Overdriving – exceeding an amplifiers ability to maintain consistent proportional output –Gain = Amplification = S o /S i –S min <S i <S max Overloaded in this range.

5 2) Frequency Response ability to measure all frequency components proportionally Attenuation: loss of signal frequencies over a specific range Attenuated in this range. COMPONENTS OF SYSTEM RESPONSE

6 3) Phase Response amplifiers ability to maintain the phase relationships in a complex wave. This is usually important for complex waves unlike amplitude and frequency responses which are important for all types of input wave forms. Why? COMPONENTS OF SYSTEM RESPONSE

7 4) Delay/Rise time: time delay between start of step but before proper output magnitude is reached. Slew rate: maximum rate of change that the system can handle (de/dt) (i.e. for example 25 volts/microsecond) COMPONENTS OF SYSTEM RESPONSE

8 Dynamic Characteristics of Simplified Mechanical Systems F(t) = general excitation force  = fundamental circular forcing frequency Generalized Equation of Motion for a Spring Mass Damper System(1-axis)

9 (I)FIRST ORDER SYSTEM (I.A) Step Forced If mass = 0, we get a first-order system. E.g. Temperature sensing systems F(t)=0 for t<0 F(t) = F0 for t >= 0 –t=time, k=deflection constant –s=displacement,  =damping coefficient –F o =amplitude of input force This can be reduced to the general form: (after integration over time and simplification) –P=magnitude of any first order system at time t –P  =limiting magnitude of the process as t   –P A =initial magnitude of process at t=0 –  = time constant =  /k The above equation could be used to define processes such as a heated/cooled bulk or mass, such as temperature sensor subjected to a step-temperature change, simple capacitive-resistive or inductive-resistive circuits, and the decay of a radioactive source.

10 Figure (a) depicts progressive process Figure (b) depicts decaying process

11 F(t) = Fo cos  t (I)FIRST ORDER SYSTEM (I.B) Harmonically Excited

12 PHASE LAG

13 First Order System – Harmonically Excited – Example T emperature Probe Example

14 TEMPERATURE PROBE EXAMPLE - Continued

15

16 Step input –F=0 when t<0 –F=F o when t>0 Underdamped Eq: (II) SECOND ORDER SYSTEM (II.A) Step Input

17 OVERDAMPED SECOND ORDER SYSTEM  =  /  C >1 This represents both damped and under-damped cases.

18 (II) SECOND ORDER SYSTEM (II.B) Harmonically Excited F(t) = Fo cos  t

19

20 MICROPHONE EXAMPLE Second Order System – Harmonically Excited Example Microphone Example

21 MICROPHONE EXAMPLE


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