Exercise 1-3 Band-Limiting EXERCISE OBJECTIVE When you have completed this exercise, you will be familiar with band-limiting. You will be able to verify the effects of band-limiting on pulse signals as seen in both the frequency domain and the time domain. You will establish the relationship between pulse rise time and bandwidth. DISCUSSION OUTLINE The Discussion of this exercise covers the following points: DISCUSSION Spectral analysis All-pass filter Ideal low-pass filter Practical low-pass filter Cutoff frequency Filtering effects Spectral analysis Spectral analysis shows that a pulse waveform can be considered to consist of a large number of frequency components, each having its own frequency and power level. In order to transmit a pulse signal through a system without distortion, all of the frequency components must be transmitted equally well. They may all be amplified or attenuated uniformly, but the relative magnitude of each frequency component must not be altered. If all significant frequencies are not transmitted, the pulse waveform will suffer appreciable distortion. Figure 1-21 shows a signal being transmitted through a system. By comparing the signal at the input and the output of the system, one can determine how effectively the system transmits different frequencies, and obtain the frequency response characteristics of the system. In general, the frequency response of a system includes an amplitude response (amplitude versus frequency) as well as a phase response (phase versus frequency). We will limit ourselves to the amplitude response. Figure 1-21. Determining the frequency response characteristics of a system. © Festo Didactic 39862-00 29 Ex. 1-3 – Band-Limiting Discussion All-pass filter Figure 1-22 shows the frequency response curve of an all-pass system. This figure shows that the gain of an all-pass system is the same for all frequencies. This means that all frequencies are transmitted equally well. Figure 1-22. All-pass system frequency response. Completely unlimited all-pass transmission is not possible to obtain. In practical systems, there is always some limit to the frequencies that can be transmitted without attenuation. The limiting of the range of frequencies that are transmitted through a system is called bandwidth limitation or band-limiting. In order to understand the operation of band-limited systems, we will consider a system which transmits equally well, all frequencies within a certain range, but completely blocks frequencies outside of this range. This type of system is called an ideal, or brick-wall filter. Ideal low-pass filter Figure 1-23 shows the frequency response of an ideal low-pass filter. All frequencies from 0 Hz to the maximum frequency transmitted, called the cutoff frequency, are transmitted equally well, but frequencies greater than the cutoff frequency are not transmitted at all. The range of frequencies that are transmitted is called the bandwidth B of the system. For a low-pass filter, the bandwidth is equal to the cutoff frequency. Such an ideal low-pass filter will eliminate all frequency components greater than the cutoff frequency. A signal which contains no frequency components beyond a certain range is said to be strictly bandlimited. Figure 1-23.Ideal low-pass filter frequency response. 30 © Festo Didactic 39862-00 Ex. 1-3 – Band-Limiting Discussion Practical low-pass filter Ideal filters are impossible to construct. Practical filters have a fairly constant frequency response within a certain range, and gradually attenuate frequencies beyond this range. Figure 1-24 shows the frequency response of a practical lowpass filter. Frequencies well below the cutoff frequency are transmitted uniformly, whereas higher frequencies are attenuated. The amount of attenuation of the high frequencies varies with the frequency: the higher the frequency, the more the attenuation. This gradual increase in attenuation over a range of frequencies is called rolloff. The rate of attenuation is related to the order of the filter. In general, the order of a filter is a function of the number of reactive components (inductors and capacitors) in the filter circuit. The higher the filter order, the sharper the rolloff. Figure 1-24.Practical low-pass filter frequency response. Cutoff frequency The cutoff frequency of a practical filter is the frequency where the power of the transmitted signal is reduced by one-half, or 3 dB. This corresponds to an attenuation in amplitude to 1/ 2 times the original amplitude. The bandwidth (or bandpass) of a practical system is the range of frequencies over which the gain remains within 3 dB. This is often called the "half-power bandwidth" or " – 3 dB bandwidth" (see Figure 1-24). Depending on the design and order of the filter, the frequency response may increase slightly just before it begins to drop, or there may be slight ripples in the frequency response curve. Filtering effects Figure 1-25 shows the effect of band-limiting a narrow-pulse signal using a lowpass filter. Before band-limiting, the spectrum is fairly flat over a certain range, as shown by the dotted line. After band-limiting, the attenuation of each harmonic depends on its frequency – the higher the frequency, the more the attenuation. The degree of attenuation at the cutoff frequency of the filter is equal to 3 dB. © Festo Didactic 39862-00 31 Ex. 1-3 – Band-Limiting Procedure Outline Figure 1-25. Band-limiting using a low-pass filter. These frequency domain characteristics have their counterpart in the time domain. In pulses which have been distorted by band-limiting, the transition of the amplitude from zero to the final value is not instantaneous. Instead, this transition takes a certain time. The rise time is usually defined as the time required for the voltage to rise from 10% to 90% of its final value. The rise time of a pulse depends on the bandwidth of the system through which it has been transmitted. For this reason, bandwidth is a measure of how rapidly a signal in the system can change. As the bandwidth B is decreased, the voltage rises more slowly. The rise time is inversely proportional to the bandwidth. For practical low-pass filters of order greater than second order, the rise time is approximately equal to 1/(2B). Therefore, band-limiting limits the minimum rise time of transmitted pulses. PROCEDURE OUTLINE The Procedure is divided into the following sections: PROCEDURE Set-up and connections Observing a pulse signal Observing a pulse frequency spectrum Filtering in the frequency domain Rise time Set-up and connections 1. Turn on the RTM Power Supply and the RTM and make sure the RTM power LED is lit. File f Restore Default Settings returns all settings to their default values, but does not deactivate activated faults. 2. Start the LVCT software. In the Application Selection box, choose PAM and click OK. This begins a new session with all settings set to their default values and with all faults deactivated. Double-click to select SWapp If the software is already running, choose Exit in the File menu and restart LVCT to begin a new session with all faults deactivated. b 3. Make the external connections for Pulses shown on the System Diagram tab of the software. For details of connections to the Reconfigurable Training Module, refer to the RTM Connections tab of the software. b 32 Click the PULSES button to show the required external connections. © Festo Didactic 39862-00 Ex. 1-3 – Band-Limiting Procedure Observing a pulse signal 4. Make the following Generator Settings on Function Generator A: Function ......................................................... Pulse Frequency (Hz) .............................................. 1 000 Duty Cycle (%)............................................... 1 5. Click the PAM Generator tab in order to display the PAM Generator diagram. Show the Probes bar (click in the toolbar or choose View f Probes Bar). Connect the probes as follows: Oscilloscope Probe Connect to Signal 1 TP1 AUDIO INPUT E TP6 Buffered CLOCK INPUT 6. Show the Oscilloscope (click in the toolbar or choose Instruments f Oscilloscope). Figure 1-26 shows an example of settings and what you should observe. Oscilloscope Settings: Channel 1........................... 500 mV/div Persistence ............................ 4 Traces Time Base ........................... 0.5 ms/div Trigger Slope ............................. Rising Trigger Level ............................... 0.5 V Trigger Source ................................Ext Figure 1-26. Pulse signal with 1% duty cycle. a The pulses appear to fade in and out on the oscilloscope due to their short duration. Turning on the persistence allows the pulses to be observed more easily. Observing a pulse frequency spectrum 7. Show the Probes bar (click in the toolbar or choose View f Probes Bar). Connect the Spectrum Analyzer Probe to TP1. © Festo Didactic 39862-00 33 Ex. 1-3 – Band-Limiting Procedure Show the Spectrum Analyzer (click in the toolbar or choose Instruments f Spectrum Analyzer). Figure 1-27 shows an example of settings and what you should observe. Spectrum Analyzer Settings: Maximum Input ....................... -30 dBV Scale Type ........................ Logarithmic Scale .................................... 5 dBV/div Averaging ........................................... 4 Time Window ....................... Hamming Frequency Span ................... 2 kHz/div Reference Frequency .................0 kHz Figure 1-27. Pulse signal spectrum with 1% duty cycle. 8. Is the spectrum fairly flat? Explain. Filtering in the frequency domain 9. Store the current spectrum in Memory location M1. Move the Spectrum Analyzer probe to TP2 and set the Low-pass filter to the Max value of 8 kHz. Compare the filtered and unfiltered signal spectrum. b Click M1 or M2 in the instrument toolbar to store the current display in Memory 1 or Memory 2. Use the Memories setting to show the contents of Memory 1, Memory 2, or both. Have all of the harmonics been attenuated to the same degree? Explain. 34 © Festo Didactic 39862-00 Ex. 1-3 – Band-Limiting Procedure 10. The degree of attenuation at the cutoff frequency of a filter is 3 dB. Use the horizontal cursors to determine which harmonic has been attenuated by approximately 3 dB. Is the result consistent with the frequency setting of the Low-pass Filter? 11. Connect the probes as follows in order to observe the filtered signal in both the time and frequency domains: Probe Connect to Signal Oscilloscope 1 TP1 AUDIO INPUT Oscilloscope 2 TP2 Low-pass Filter output Spectrum Analyzer TP2 Low-pass Filter output 12. Make the following Generator Settings on Function Generator A: Function ......................................................... Pulse Frequency (Hz) .............................................. 1 000 Duty Cycle (%)............................................... 50 Set the Low-pass Filter order to 4th and capture the oscilloscope and spectrum analyzer output for each of the following Cutoff Frequency values: 1. 8 kHz 2. 6 kHz 3. 4 kHz 4. 2 kHz 5. 1 kHz 6. 300 Hz How does reducing the bandwidth affect the spectrum? © Festo Didactic 39862-00 35 Ex. 1-3 – Band-Limiting Procedure Rise time 13. Return the settings on Function Generator A to the following if they have been modified: Function ......................................................... Pulse Frequency (Hz) .............................................. 1 000 Duty Cycle (%) ............................................... 50 Set the Low-pass Filter frequency to the maximum value of 8 kHz. Turn off channel 1 on the oscilloscope so that only the filtered signal is displayed. Adjust the settings on the oscilloscope so that the display is similar to Figure 1-28. Use the single refresh option on the oscilloscope to freeze the display for measuring purposes. a a The horizontal trigger at the bottom of the oscilloscope screen should be dragged to the center of the screen. To refresh and freeze the display, click the button in the instrument toolbar. This refreshes the display once and freezes it. You can also press F5 or , press F6 or choose View f choose View f Single Refresh. Click Continuous Refresh to resume normal operation. Oscilloscope Settings: Channel 2........................... 200 mV/div Time Base ............................. 50 Ps/div Trigger Slope ............................. Rising Trigger Level ............................... 0.5 V Trigger Source ............................. Ch 2 Figure 1-28. Oscilloscope display for measuring rise time. 14. For the bandwidth values (Low-pass filter frequencies) shown in Table 1-2, capture the output and use the oscilloscope cursors to determine the rise time tr (from 10% to 90%) of the pulse voltage as shown in Figure 1-29. Record the values of tr in Table 1-2. Calculate the values of 1/B and record them in the table as well. a Use the horizontal cursors to mark the 90% and 10% levels and then use the vertical cursors to determine the time between the two levels. The position of the horizontal cursors should not require adjusting as the filter bandwidth is modified. The oscilloscope window can be maximized for easier viewing. 36 © Festo Didactic 39862-00 Ex. 1-3 – Band-Limiting Procedure 90% Crossing 100% 90% 10% Crossing Rise Time 10% 0% Figure 1-29. Measuring rise time. Table 1-2. Rise time measurements. Bandwidth B (kHz) 1/B (Ps) Rise Time tr (Ps) 8 6 4 2 © Festo Didactic 39862-00 37 Ex. 1-3 – Band-Limiting Conclusion 15. Using the values in Table 1-2, plot the rise time tr versus 1/B in Figure 1-30. Figure 1-30. Relationship between rise time and bandwidth. Describe the relationship between the rise time tr and the bandwidth B. 16. When you have finished using the system, exit the LVCT software and turn off the equipment. CONCLUSION 38 In this exercise, you observed that a practical band-limited system transmits frequencies within its bandwidth uniformly (within 3 dB) but attenuates frequencies outside this range. You observed that attenuating the high frequency components of a pulse signal increases the distortion of the pulses, and that the pulse rise time is inversely proportional to the bandwidth. © Festo Didactic 39862-00 Ex. 1-3 – Band-Limiting Review Questions REVIEW QUESTIONS 1. What is the half-power bandwidth of a practical low-pass filter? 2. How does band-limiting a pulse signal with a low-pass filter affect the spectrum of the signal? 3. Does a practical low-pass filter completely eliminate frequency components outside its bandwidth? Explain. 4. How does band-limiting a pulse signal with a low-pass filter affect the waveform (shape) of the pulses? 5. What is the relation between rise time and bandwidth? © Festo Didactic 39862-00 39
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