1 / 20

ME 322: Instrumentation Lecture 22

ME 322: Instrumentation Lecture 22. March 12, 2014 Professor Miles Greiner. Announcements/Reminders. HW 8 Due Friday Josh will hold office hours in PE 215 (and 113) tomorrow after lab, until around 6 PM This week in lab: Lab 7 Boiling Water Temperature in Reno

daisy
Télécharger la présentation

ME 322: Instrumentation Lecture 22

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. ME 322: InstrumentationLecture 22 March 12, 2014 Professor Miles Greiner

  2. Announcements/Reminders • HW 8 Due Friday • Josh will hold office hours in PE 215 (and 113) tomorrow after lab, until around 6 PM • This week in lab: • Lab 7 Boiling Water Temperature in Reno • Midterm II, April 2, 2014 (three weeks) • Next week is Spring Break

  3. Fourier Transform V 0 t T1 • Any function V(t), over interval 0 < t < T1, may be decomposed into an infinite sum of sine and cosine waves • , • Discrete frequencies: , n = 0, 1, 2, … ∞ (integers) (not continuous) • Only admits modes for which an integer number of oscillations span the total sampling time T1. • The coefficient’s an and bnquantify the relative importance (energy content) and phase of each mode (wave). • The root-mean-square (RMS) coefficient for each mode quantifies its total energy content for a given frequency (from sine and cosine waves) n = 2 n = 1 n = 0 sine cosine

  4. Examples (ME 322r Labs) Frequency Domain Time Domain Function Generator 100 Hz sine wave • Wave amplitude does not need to remain constant • Signals may have a wide spectrum of energetic modes Damped Vibrating Cantilever Beam Unsteady Speed Air Downstream from a Cylinder in Cross Flow

  5. What is the lowest Frequency mode that can be observed during measurement time T1 • For example, if we measure outdoor temperature for one hour, can we observe variations that require a day to repeat? • The lowest (finite) observable frequency is f1 = 1/T1 • The only other frequencies that can be detected are • What is the frequency resolution? • Smallest change in frequency that can be detected • Increasing the total sampling time T1reduces the lowest detectable frequency and improves frequency resolution

  6. Upper and Lower Frequency Limits • If a signal is sampled at a rate of fS for a total time of T1 what are the highest and lowest frequencies that can be accurately detected? • (f1= 1/T1) < f < (fN = fS/2) • To reduce lowest frequency (and increase frequency resolution), increase total sampling time T1 • To observe higher frequencies, increase the sampling rate fS.

  7. Lab 8: Time Varying Voltage Signals Digital Scope • Produce sine and triangle waves with fm = 100 Hz, VPP = ±1-4 V, T1 = 0.04 sec • Sample both at fS = 48,000 Hz and numerically differentiate with two different differentiation time steps • Evaluate Spectral Content of sine wave at four different sampling frequencies fS= 5000, 300, 150 and 70 Hz; and T1 = 1 sec • note: some fS< 2fm • Sample singles between 10,000 Hz < fM < 100,000 Hz using fS = 48,000 Hz • Compare fa to folding chart Function Generator NI myDAQ fM = 100 Hz VPP = ±1 to ± 4 V Sine wave Triangle wave fS = 100 or 48,000 Hz Total Sampling time T1 = 0.04, 1 sec 4 cycles 192,000 samples

  8. Estimate Maximum Slope • Sine wave • Triangle Wave VPP VPP P P

  9. Fig. 3 Sine Wave and Derivative Based on Different Time Steps • dV/dt1 (Dt=0.000,0208 sec) is nosier than dV/dt10 (Dt=0.000,208 sec) • The maximum slope from the finite difference method is slightly larger than the ideal value. • This may be because the actual wave was not a pure sinusoidal.

  10. Fig. 4 Triangle Wave and Derivative Based on Different Time Steps • dV/dtm=1 is again nosier than dV/dtm=10 • dV/dtm=1 responds to the step change in slope more accurately than dV/dtm=10 • The maximum slope from the finite difference method is larger than the ideal value.

  11. Fig. 5 Measured Spectral Content of 100 Hz Sine Wave for Different Sampling Frequencies • The measured peak frequency fP equals the maximum signal frequency fM = 100 Hz when the sampling frequency fSis greater than 2fM • fs = 70 and 150 Hz do not give accurate indications of the peak frequency.

  12. Table 2 Peak Frequency versus Sampling Frequency • For fS > 2fM = 200 Hz the measured peak is close to fM. • For fS < 2fM the measured peak frequency is close to fM–fS. • The results are in agreement with sampling theory.

  13. Table 3 Signal and Indicated Frequency Data • This table shows the dimensional and dimensionless signal frequency fm (measured by scope) and frequency indicated by spectral analysis, fa. • For a sampling frequency of fS = 48,000 Hz, the folding frequency is fN = 24,000 Hz.

  14. Figure 6 Dimensionless Indicated Frequency versus Signal Frequency • The characteristics of this plot are similar to those of the textbook folding plot • For each indicated frequency fa, there are many possible signal frequencies, fm.

  15. Figure 2 VI Block Diagram

  16. Figure 1 VI Front Panel

  17. Construct VI • Starting Point VI • Spectral Measurement VI • Signal Processing; Waveform Measurement, • Result: linear • Convert to and from dynamic data • Signal Manipulation • Input data type: 1D array of scalars-single channel • “Time” of maximum • Mathematics; Probability and Statistics: Statistics

  18. Lab 8 Sample Data • http://wolfweb.unr.edu/homepage/greiner/teaching/MECH322Instrumentation/Labs/Lab%2008%20Unsteady%20Voltage/Lab8Index.htm • Calculate Derivatives • Plot using secondary axes • Design; Change Chart Type; Combo • Scatter with straight line • Frequency Domain Plot • The lowest finite frequency and the frequency resolution are both f1 = 1/T1

  19. Folding Diagram for given fS and fM? Maximum frequency that can be accurately measured using sampling frequency fS .

More Related