Download presentation
Presentation is loading. Please wait.
Published byLoren Atkins Modified over 9 years ago
1
Measurements in Fluid Mechanics 058:180:001 (ME:5180:0001) Time & Location: 2:30P - 3:20P MWF 218 MLH Office Hours: 4:00P – 5:00P MWF 223B-5 HL Instructor: Lichuan Gui lichuan-gui@uiowa.edu http://lcgui.net
2
2 Lecture 5. Dynamic response of measuring systems
3
3 Models of dynamic response Dynamic measuring system - at least one of inputs is time dependent Description of dynamic response - differential equation that contains time derivatives. - Linear dynamic response: linear differential equation Simple dynamic response - Non-linear dynamic response: non-linear differential equation Zero-order systems K – static sensitivity - approximated by single, linear, ordinary differential equation with constant coefficients x – input y – output t – time constant coefficients: a i, i=1,2, ,n ; b j, j=1,2, ,m - example of zero-order systems: electric resistor - time independent
4
4 Models of dynamic response First-order systems Second-order systems K – static sensitivity – time constant - example of first-order systems: thermometer K – static sensitivity – damping ratio n – undamped natural frequency =0: undamped second-order system =1: critically damped second-order system 0< <1: underdamped second-order system >1: overdamped second-order system Damped natural frequency (for 0< <1): - example of second-order systems: liquid manometer
5
5 Type of input Unit-step (or Heaviside) function Unit-impulse (or Dirac’s delta) function - A relative fast change of the input from one constant level to another. - A sudden, impulsive application of different value of input, lasting only briefly before it returns to the original level for continuous function f(x):
6
6 Type of input Unit-slope ramp function Periodic function - A gradual change of the input, starting from a constant level persisting monotonically. - Function f(t) with period T so that f(t)=f(t+nT) T - Can be decomposed in Fourier series
7
7 Dynamic response of first-order system Step response t/ 1234 x/A 37%13.5%5%1.8%
8
8 Dynamic response of first-order system Impulse response t/ 1234 - x/A 37%13.5%5%1.8% Ramp response t/ 1234 - ( x/A- ) 37%13.5%5%1.8%
9
9 Dynamic response of first-order system Frequency response As , B/A 0, and - /2. Thus a first-order system acts like a low-pass filter.
10
10 Dynamic response of second-order system Step response - Damping ratio determines response - Critically damped & overdamped system output increases monotonically towards static level - output of underdamped system oscillates about the static level with diminishing amplitude. - Lightly damped system ( <<1) are subjected to large-amplitude oscillation that persist over a long time and obscure a measurement.
11
11 Dynamic response of second-order system Impulse response Ramp response - Critically damped & overdamped system output increases monotonically towards static level - underdamped system oscillates with diminishing amplitude. - undamped system with large-amplitude oscillation
12
12 Dynamic response of second-order system Frequency response - Critically damped & overdamped systems act like low-pass filters and have diminishing output amplitudes - Undamped systems have infinite output amplitude when = n - Underdamped systems with have no resonant peak - Underdamped systems with present a peak at resonant frequency.
13
13 Dynamic response of higher-order and non-linear system Dynamic analysis by use of Laplace transform - Laplace transform of time-dependent property f(t) : - Inverse Laplace transform: - Differentiation property of Laplace transform: Experimental determination of dynamic response - square-wave test: input switched periodically from one level to another - frequency test: sinusoidal input of constant amplitude and varying frequency Direct dynamic calibration suggested when measuring system exposed to time-dependent inputs
14
14 Distortion, loading and cross-talk Flow distortion - caused by instrument inserted in flow Loading of measuring system - measuring component extracts significant power from flow Instrument cross-talk - output of one measuring component acts as undesired input to the other
15
15 Homework - Questions and Problems: 10 on page 43 - Read textbook 2.3-2.4 on page 31-41 - Due on 09/02
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.