Bài báo cáo thực hành 2 môn lý thuyết mạch (Circuit Theory)

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Bài báo cáo thực hành 2 môn lý thuyết mạch (Circuit Theory)

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EE233 lab report 2

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The University of Danang

Danang University of Science and Technology

LAB REPORT

Instructor : Nguyen Tri Bang

Group members: Tran Viet Tu

Nguyen Cong Thien

Dinh Ngoc Tien

Le Dinh Hoai Nam

Danang 2017

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 Read IC component specifications and get data from them for circuit analysis and design

 Analyze and measure characteristics of circuits built with op-amps  Use the op-amp as a component in the design of simple circuits  Analyze the effect of open fault in manufacturing.

II Equipment used

The instruments needed for this experiment:

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 An arbitrary waveform generator,  A multimeter.

 An oscilloscope  Resistors and op-amp.

7 Experimental procedures

7.1 Instruments needed for this experiment

The instruments needed for this experiment are: a power supply, an arbitrary waveform generator, a multimeter, and an oscilloscope.

7.2 Op-amp voltage follower circuit

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1 Build the circuit in Figure 1 using R = 5 KΩ, power supply = ±12 V Set the function generator to provide a square wave input as follows (display on channel 1 of the

scope):

a Period T=100 µs, 50% duty cycle

b Amplitude: -10 V to +10 V

2 Use Channel 2 of the oscilloscope to display the output signal waveform Adjust the timebase to display 2 complete cycles of the signals

The yellow figure is channel 1: input The green figure is channel 2: output

3 From the oscilloscope, measure the time interval for the output to reach the steady state after an input transition.

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∆t =21.20μs

4 Calculate the slew rate using this data and compare with the typical slew rate in the specifications.

The slew rate is ∆V/∆t = |(V10% -V90%)| / ∆t = 10 V / 21.20μs = 0.47V /μs ≈ 0.5 V/μs It is approximate to the typical slew rate.

5 Are the slew rates the same for the high-to-low transition and the low-to-high

transition? If they are not, attempt to explain this difference in the data analysis section below.

For the high-to-low transition, ∆t1 = 32.80μs

Similarly the calculating slew rate in part 4, the slew rate for the high-to-low transition is 0.31 V/μs

For the low-to-high transition, ∆t2 = 21.20μs

And the slew rate for the low-to-high transition is 0.47 V/μs They are different

6 Save a screenshot

∆t = 32.80μs

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7 Clear all the measurements Change the input signal to a sine wave with amplitude 3 V (-3V to +3V peak-to-peak), frequency 1 KHz Check the output signal to make sure the voltage follower functions as expected Now increase the frequency of the input signal (keep the input amplitude the same) until the output signal starts to get distorted from a sine or cosine wave What is the frequency for the onset of this distortion?

The frequency is 1 KHz, Vpp input = 6.04V, Vpp output = 6.04V Therefore, the voltage gain is 1.So it is the voltage follower function.

From the experiment, the voltage output starts to distort when the frequency is

approximate to 30 KHz, but we choose the figure when the frequency is 35 KHz to see the

distortion easily 8 Save a screenshot.

The voltage output starts to distort when the frequency is 35 KHz.

7.3 Performance of the gain circuit in Figure 2

1 Build the circuit in Figure 2, with the initial setting of the resistor R2 = 0 (record this value) and power supply = ±12 V Apply a sine wave input signal with amplitude 100 mV (-100 mV to +100 mv), DC offset 0V, and frequency 10 Hz Display the input signal on channel 1 of the signal

The resistor R2 = 0.041 Ω

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2 Display Vout on Channel 2 and adjust the time base to display 2 complete cycles of the signals.

The same image in part 1

3 Record the overall gain at this setting of R2 (i.e record in a table the value of R2 and the corresponding value of the voltage gain).

Vpp input = Vmax(1) – Vmin(1) = 216 mV Vpp output = Vmax(2) – Vmin(2) = 2.16 V So the overall voltage gain is 10

4 Now vary R2 to take on these values: 1 KΩ, 2 KΩ, 3 KΩ … up to 10 KΩ at 1 KΩ step At each setting of R2, measure the gain and record it in the same table for subsequent

The vertical column is easy for plotting later.

5 Get a hardcopy output from the scope display with both waveforms at each of these settings of R2= 2 KΩ and R2=8 KΩ Turn these hardcopies in as part of your lab report

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R2 = 2 KΩ, the voltage gain is 6.02

R2 = 8 KΩ, the voltage gain is -5.83

7.4 Performance of your own gain circuit

1 Build the circuit you designed in the pre-lab,

section 6.4 above Use power supplies ±12 V Apply a sine wave input signal with

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amplitude 100 mV (-100 mV to + 100 mV peak-to-peak), frequency 10 Hz Display the input signal on channel 1 of the oscilloscope.

2 Use Channel 2 of the oscilloscope to display the output signal waveform Adjust the time base to display 2 complete cycles of the signals

3 Collect “sufficient” data to show convincingly that your circuit performs as designed Turn in the data you collect (scope display of waveforms, tables of data points, plots, etc.) With R2=0 Ω

Circuit in 7.3, the voltage gain = 10

Our performance: The voltage gain = - 9.58

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With R2=2 KΩ

Circuit in 7.3: The voltage gain = 6.02 Our performance : The voltage gain =

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8 Data analysis.

8.1 Op-amp voltage follower circuit.

1 From the pre-lab section 6.2 items 2 and the measured value in section 7.2 item 3, compare the calculated and measured values of the time for the output to reach the steady state.

The measured values:  Low to high: 21 μs  High to low: 32 μs The calculated value: 20us

The time for low-to-high transition is approximate to the calculated value but the time for high-to-low transition is greater than it.

2 If the slew rates are not the same for the high-to-low transition and the low-to-high transition as observed in the lab, attempt to explain why

From the section 7.2

The slew rate for the low-to-high transition is 0.47 V/μs The slew rate for the high-to-low transition is 0.31 V/μs They are different.

The slew rate is the slope of the signal (dΔV/dt), then when time from low-to-high and time from high-to-low is different which is explained in section 7.2 item 5 They lead to the different in slew rate

8.2 Performance of the circuit in Figure 2

1 Plot the data collected in section 7.3 item 4: voltage gain versus the setting of the resistor R2 Use linear scale on both axes

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Voltage gain versus R2 value

2 Compare this plot with the plot using calculated data in the pre-lab section 6.3 item Explain any difference

From the calculated data

Voltage gain versus R2 value

Comment: The measured values and the calculated values are nearly the same

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8.3 Performance of your own gain circuit

1 Justify the specific data you collected in section 7.4 (i.e if you collect voltage gain as function of frequency, explain why you think this data is important to support your conclusion that the circuit works as designed)

- This data base on R2, because it is the key to calculate Gain.

2 How much data is “sufficient” to demonstrate the performance of your circuit? This issue is critical in real-life testing If too much data is collected, the test cost is higher and the profit per product is lower If too little data is collected, your circuit might not really work as designed since it has not been well tested So what is “sufficient data” for this specific design? Justify your answer

- In our opinion, a set of three specific data is enough for the test Since we know that the gain is the first order function of R2, therefore it should be a “line” - And 2 points give us a line To make sure the result, three measured values are

enough for the test.

3 Analyze your data to demonstrate that the circuit works as designed Show plots, equations, differences between calculated and measured results, etc Discuss in detail if your circuit does not work as designed or if there are significant differences between the theoretical and the measured results.

Plot the gain as function of R2 from:

Measured gain value

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Voltage gain versus R2 value

Comment: The measure value is nearly same with the calculated values We realize that

they share some common point The shapes of these two pictures are quite similar

This report has discussed op-amps play an important role in the circuit, read component specifications and process data of circuit in analysis and design Analyze and measure characteristics of circuits building with op-amps, Use the op-amp as a component in the design of simple circuits and analyze the effect of open fault in manufacturing Remember that characteristics of the op-amps (slew rate, voltage gain, off-set voltage) were also mentioned Especially the Voffset of op-amp and solving Voffset This report show the difference between theoretical data and practical one The data collected correlated strongly to the hypotheses, percent errors reaching as so large but it are normal in the lab.

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