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    Copyright 2014 GWU SEAS ECE Department ECE 2110: Circuit Theory

    1

    SCHOOL OF ENGINEERING AND APPLIED SCIENCEDEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING

    ECE2110:CIRCUIT THEORY LABORATORY

    Experiment #11:Final Project Preparation Lab 1 Active Filter Design

    EQUIPMENT

    Lab Equipment Equipment Description

    (1) DC Power Supply Agilent E3631A Triple Output DC Power Supply

    (1) Function Generator Agilent 33522A Function/Arbitrary Waveform Generator

    (1) Digital Multimeter (DMM) Keithley Model 175 Digital Multimeter (DMM)

    (1) Digital Oscilloscope Agilent DSO1024A Digital Oscilloscope

    (1) Breadboard Prototype Breadboard

    (1) BNC T-Connector One input to two output BNC connector

    (1) Test Leads Banana to Alligator Lead Set(2) Test Leads BNC to Mini-Grabber Lead Set

    (1) BNC Cable BNC to BNC Cable

    Table 1 Equipment List

    COMPONENTS

    Type Value Symbol Name Multis im Part Descripti on

    Resistor --- R Basic/Resistor Various Values

    Capacitor --- F C Basic/Capacitor Various Values

    Op-Amp LM741 LM741 Basic/Analog/OpAmp/741 ---

    Power Amp LM386 LM386 --- Audio AmplifierSpeaker 6 --- --- 18W Speaker

    Table 2 Component List

    OBJECTIVES

    Understand the difference between active and passive filters

    Design and build a band-pass filter using active components

    Understand the limitations of the LM741

    Understand what an LM386 is and why it is necessary

    Build and measure a band-pass filter using LM741s and an LM386

    Note: At this point, the final project should be introduced by the GTA. Ideally, an introduction to theproject will be given at the end of the last lab to prepare students for this prelab and lab. Students, pleasefind the final project specifications document on the ECE 2110 lab website under the Projects section..

    http://www.seas.gwu.edu/~ece11/spec_sheets/equipment/powersupply_agilent_E3631A.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/Agilent_33522A.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/multimeter_keithley_175.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/oscope_agilent_dso1024a.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/oscope_agilent_dso1024a.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/multimeter_keithley_175.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/Agilent_33522A.pdfhttp://www.seas.gwu.edu/~ece11/spec_sheets/equipment/powersupply_agilent_E3631A.pdf
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    Experiment #11: Final Project Preparation Lab 1 Active Filter Design

    Copyright 2014 GWU SEAS ECE Department ECE 2110: Circuit Theory

    2

    SEAS

    INTRODUCTION

    This lab will introduce you to the concept of active filters and explain how they differ from passive filtersand why they are necessary. In Lab 10, you were introduced to passive filters. Passive filters consist ofonly passive components (inductors, capacitors, resistors). Because passive components cannot provideaverage power to a circuit, you cannot make a filter with a gain greater than 1 using only passive

    components. In many situations, you may wish to create a filter with a gain greater than 1. For this, youmust incorporate an op-amp into the filter design.

    Active 1st

    Order Low-Pass Filter

    Figure 1 Inverting Amplifier Figure 2 Active 1st Order Low-Pass Filter

    Figure 1shows an inverting amplifier. From the lab on DC Operational Amplifiers, we know the gain ofthis amplifier is Vout/Vin= -Rf/Rin. Instead of using just resistors, we can substitute impedances Zfand Zin,and the gain becomes Vout/Vin= -Zf/Zin.

    Figure 2shows the same amplifier, now with a capacitor inserted in the feedback path. Zinis still Rin, butZf is the impedance of the resistor and capacitor in parallel, so Zf = ZRf || ZCL: Substituting in theimpedances as shown in Figure 2:

    1 / 1/ 1Typically, for filters, the transfer function of interest is the voltage gain, defined as T() = Vout/Vin. Sincethe voltage gain of the amplifier in Figure 2is Vout/Vin= -Zf/Zin, the transfer function for the filter becomes:

    1

    1What should be familiar is the expression in parentheses in the equation above, it is the transfer functionfor a low-pass filter. The expression outside of the brackets: -Rf/Rin, means this low-pass filter has gain!

    The cutoff frequencyfor this low-pass filteris:

    1Note: To design this filter, one chooses the appropriate resistors: Rf and Rin to set the gain, thendetermines CLfor the desired cutoff frequency (C).

    inR

    fR

    V

    Vin

    out

    inR

    fR

    V

    Vin

    out

    LC

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    Experiment #11: Final Project Preparation Lab 1 Active Filter Design

    Copyright 2014 GWU SEAS ECE Department ECE 2110: Circuit Theory

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    SEAS

    Active 1st

    Order High-Pass Filter

    Figure 3 Inverting Amplifier Figure 4 Active 1stOrder High-Pass Filter

    Figure 4 shows how we can make the inverting amplifier into a high-pass filter by rearranging thecapacitor to be in series with the input resistor. The transfer function then becomes:

    1/When the frequency is low (e.g. 0), the transfer function approaches 0. As the frequency getshigher and higher (e.g ), the transfer function becomes -Rf/Rin. This is the behavior of a high-passfilter. The cutoff frequencyfor this filter can be derived as:

    1

    inR

    fR

    V

    Vin

    out

    inR

    fR

    V

    Vin

    out

    HC

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    Experiment #11: Final Project Preparation Lab 1 Active Filter Design

    Copyright 2014 GWU SEAS ECE Department ECE 2110: Circuit Theory

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    SEAS

    PRELAB

    Part I Acti ve Band-Pass Filter Design

    Figure P.1 Active Band-Pass Filter with Gain Stage

    1. Using the procedure discussed in the Introduction, designan active band-pass filterwith again of -10, a lower cut-off frequency of 150Hzand an upper cutoff frequency of 5kHz. Be sureto show all work and mention any relevant assumptions or design decisions.

    Note:When choosing resistor values to set the gain for each stage, be certain to keep them verylarge in the high krange.

    1= 150Hz

    2= 5kHz

    Gain = -10

    2. Save this design as you will need to simulate it later in this prelab.

    in1R

    f1R

    Vin

    LC

    in2R

    f2R

    HC

    in3R

    f3R

    Vout

    +

    -

    +

    -

    Stage 1:Low-Pass Filter

    Stage 2:High-Pass Filter

    Stage 3:Inverter Gain Stage

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    Experiment #11: Final Project Preparation Lab 1 Active Filter Design

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    SEAS

    Part II Active Low-Pass Filter Simulation

    Figure P.2 Active 1stOrder Low-Pass Filter

    1. Simulate the active low-pass filter section of the band-pass filter in Multisim using the LM741.

    DC Supply Voltage (VCC+and VCC-): 12V

    Vin: 300mVrmssine wave

    Load: 1k

    2. Run an AC Analysis from 10Hzto 6kHz. MeasureVout(in RMS voltage) across the 1kload atthe following frequencies: 10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    3. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the 1kloadresistor at each frequency.

    4. Calculatethe current drawn by the 1kload resistor at the peak output power in each case.

    5. Recordthese values in Table P.2.

    6. Plotthe magnitudeand phaseof Vout/Vin(in dB) versus frequency from 10Hz to 6kHz.

    7. Determinethe -3dB frequencyfrom this plot.

    Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    -3dB Freq.

    Simulated

    Table P.2 Low-Pass Filter Simulation Data

    inR

    fR

    V

    Vin

    out

    LC

    300m 299.9961m .9999987 44.9988mu 299.9961mu

    300m 299.8591m .99953 44.9577mu 299.8591mu

    300m 294.0536m .98017 43.234mu 294.0536mu

    300m 233.3358m .777795 27.2228mu 233.3358mu

    300m 211.0610m .70354 22.2734mu 211.0610mu

    300m 190.9126m .6365 18.224mu 190.9126mu

    2.7924kHz

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    Experiment #11: Final Project Preparation Lab 1 Active Filter Design

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    SEAS

    Part III Active High-Pass Filter Simulation

    Figure P.3 Active 1stOrder High-Pass Filter

    1. Simulate the active high-pass filter section of the band-pass filter in Multisim using the LM741.

    DC Supply Voltage (VCC+and VCC-): 12V

    Vin: 300mVrmssine wave

    Load: 1k

    2. Run an AC Analysis from 10Hzto 6kHz. MeasureVout(in RMS voltage) across the 1kload atthe following frequencies: 10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    3. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the 1kload

    resistor at each frequency.4. Calculatethe current drawn by the 1kload resistor at the peak output power in each case.

    5. Recordthese values in Table P.3.

    6. Plotthe magnitudeand phaseof Vout/Vin(in dB) versus frequency from 10Hz to 6kHz.

    7. Determinethe -3dB frequencyfrom this plot.

    Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    -3dB Freq.

    Simulated

    Table P.3 High-Pass Filter Simulation Data

    inR

    fR

    V

    Vin

    out

    HC

    300m 20.0485m .06683 200.973n 20.0485mu

    300m 212.6401m .70880 22.6097mu 212.6401mu

    300m 296.7496m .98916 44.0302mu 296.7496mu

    300m 299.8064m .99935 44.9479mu 299.8064mu

    300m 299.8668m .999556 44.96mu 299.8668mu

    300m 299.8896m .999632 44.9669mu 299.8896mu

    264.5417Hz

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    SEAS

    Part IV Active Band-Pass Filter Simulation

    Figure P.4 Active Band-Pass Filter with Gain Stage

    1. Simulate the cascaded active band-pass filter, including the inverter gain stage, in Multisimusing the LM741.

    DC Supply Voltage (VCC+and VCC-): 12V

    Vin: 300mVrmssine wave

    Load: 1k

    2. Run an AC Analysis from 10Hzto 6kHz. MeasureVout(in RMS voltage) across the 1kload atthe following frequencies: 10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    3. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the 1kloadresistor at each frequency.

    4. Calculatethe current drawn by the 1kload resistor at the peak output power in each case.

    5. Recordthese values in Table P.4.

    6. Plotthe magnitudeand phaseof Vout/Vin(in dB) versus frequency from 10Hz to 6kHz.7. Determineboth the lower and upper -3dB frequenciesfrom this plot.

    Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    Lower -3dB Upper -3dB

    SimulatedTable P.4 Band-Pass Filter Simulation Data

    in1R

    f1R

    Vin

    LC

    in2R

    f2R

    HC

    in3R

    f3R

    Vout

    +

    -

    +

    -

    Stage 1:Low-Pass Filter

    Stage 2:High-Pass Filter

    Stage 3:Inverter Gain Stage

    300m 200.4703m .668 20.0942mu 200.4703mu

    300m 2.1307 7.102 2.2584m 2.1307m

    300m 2.9084 9.695 4.2293m 2.9084m

    300m 2.3294 7.765 2.7131m 2.3294m

    300m 2.1063 7.021 2.2181m 2.1063m

    300m 1.9040 6.347 1.8126m 1.9040m

    66.5 440000

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    SEAS

    LAB

    Part I Active Low-Pass Filter

    Figure 1.1 Active 1stOrder Low-Pass Filter

    1. Buildthe active low-pass filter section on a breadboard. Show the GTA your setup beforeapplying power.

    DC Supply Voltage (VCC+and VCC-): 12V Vin: 300mVrmssine wave

    Load: 1k

    2. MeasureVoutusing the DMM (RMS voltage) across the 1kload at the following frequencies:10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    3. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the 1kloadresistor at each frequency.

    4. Calculatethe current drawn by the 1kload resistor at the peak output power in each case.

    5. Recordthese values in Table 1.1.

    6. Adjustthe frequencyof the function generator until you find the exact -3dB frequencyof the

    filter, where max.Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas.

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    -3dB Freq.

    Simulated

    Measured

    Error

    Table 1.1 Low-Pass Filter Output Characteristics with 1kLoad

    inR

    fR

    V

    Vin

    out

    LC

    300mV 255mV 299.9961mV 247mV .9999987 44.9988W 299.9961A 247A

    300mV 319mV 299.8591mV 312mV .99953 44.9577W 299.8591A

    300mV 279mV 294.0536mV 267mV .98017 43.234W 294.0536A

    300mV 292mV 233.3358mV 234mV .777795 27.2228W 233.3358A

    300mV 298mV 211.0610mV 215mV .70354 22.2734W 211.0610A

    300mV 302mV 190.9126mV 196mV .6365 18.224W 190.9126A

    5.1835kHz

    ~5kHz

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    SEAS

    Part II Active High-Pass Filter

    Figure 2.1 Active 1stOrder High-Pass Filter

    1. Buildthe active high-pass filter section on a breadboard. Show the GTA your setup beforeapplying power.

    DC Supply Voltage (VCC+and VCC-): 12V

    Vin: 300mVrmssine wave

    Load: 1k

    2. MeasureVoutusing the DMM (RMS voltage) across the 1kload at the following frequencies:10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    3. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the 1kloadresistor at each frequency.

    4. Calculatethe current drawn by the 1kload resistor at the peak output power in each case.

    5. Recordthese values in Table 2.1.

    6. Adjustthe frequencyof the function generator until you find the exact -3dB frequencyof the

    filter, where max.Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas.

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    -3dB Freq.

    Simulated

    Measured

    Error

    Table 2.1 High-Pass Filter Output Characteristics with 1kLoad

    inR

    fR

    V

    Vin

    out

    HC

    300mV 267mV 20.0485mV 11.3mV .06683 200.973nW 20.0485A

    300mV 315mV 212.6401mV 228mV .70880 22.6097W 212.6401A

    300mV 282mV 296.7496mV 279mV .98916 44.0302W 296.7496A

    300mV 307mV 299.8064mV 304mV .99935 44.9479W 299.8064A

    300mV 302mV 299.8668mV 300mV .999556 44.96W 299.8668A

    300mV 300mV 299.8896mV 297mV .999632 44.9669W 299.8896A

    264.5417Hz

    160.57Hz

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    SEAS

    Part III Active Band-Pass Filter

    Figure 3.1 Active Band-Pass Filter with Gain Stage

    7. Buildthe active low-pass filter section on a breadboard. Show the GTA your setup beforeapplying power.

    DC Supply Voltage (VCC+and VCC-): 12V

    Vin: 300mVrmssine wave

    Load: 1k

    8. MeasureVoutusing the DMM (RMS voltage) across the 1kload at the following frequencies:10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    9. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the 1kloadresistor at each frequency.

    10. Calculatethe current drawn by the 1kload resistor at the peak output power in each case.

    11. Recordthese values in Table 3.1.

    12. Adjustthe frequencyof the function generator until you find the exact -3dB frequencies (upperand lower) of the filter, where max.

    Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas.

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    Lower -3dB Upper -3dB

    Simulated

    Measured

    Error

    Table 3.1 Band-Pass Filter Output Characteristics with 1kLoad

    in1R

    f1R

    in

    LC

    in2R

    f2R

    HC

    in3R

    f3R

    Vout

    +

    -

    Stage 1:Low-Pass Filter

    Stage 2:High-Pass Filter

    Stage 3:Inverter Gain Stage

    298mV 288mV

    315mV 2.07V

    293mV 3V

    293mV 2.5V

    300mV 2.33V

    303mV

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    SEAS

    Part IV Active Band-Pass Filter wi th Small Load

    1. For the band-pass filter you have simulated and measured, calculatethe amount of current a 6load would draw at the highest valueof Voutyou recorded in Table 3.1.

    a. Whatis the value in mA? Include this in your lab write-upb. Canthe LM741 op-amp provide this much current to a 6load?

    i. Downloadthe LM741 specification sheet from the lab website.

    ii. Lookfor the electrical parameter: Output Short Circuit Currentiii. Isthis value moreor lessthan the amount of current a 6load would draw?

    c. Replacethe 1kload in your Multisimsimulation with a6load.i. Run an AC Analysis from 10Hzto 6kHz. MeasureVout(in RMS voltage) across

    the 6load at the following frequencies: 10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHzii. Whatdo you notice about your results?

    2. From Step 1 you should realize that the LM741 cannot supporta small loadlike 6.a. We need an amplifierfor the 3

    rdstage of our band-pass filter that can provide enough

    current to our 6load.b. For this, we will replace Stage 3 of our amplifier with a power amplifier called the LM386.

    i. The LM386 is not an op-amp. It is a self-contained amplifier that can provide agreat deal of current to small loads.

    ii. Downloadthe LM386 specification sheet from the lab website.

    3. On page 5 of the LM386 specification sheet a sample configuration is shown.a. Replacethe 3

    rdstageof your amplifier with this sample configuration.

    b. Instead of a 6load, use the speakerprovided in your kit.

    4. MeasureVoutusing the DMM (RMS voltage) across the speaker at the following frequencies:10Hz, 150Hz, 1kHz, 4kHz, 5kHz, 6kHz

    5. Usingthe peak output voltage of Vout, calculatethe peak power dissipatedby the speaker ateach frequency.

    6. Calculatethe current drawn by the speaker at the peak output power in each case.

    7. Recordthese values in Table 4.1.

    8. Adjustthe frequencyof the function generator until you find the exact -3dB frequencies(upper

    and lower) of the filter, where max.Frequency Vin(rms) Vout (rms) Gain (Vout /Vin) Pout (peak) Iout (peak)

    Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas. Sim. Meas.

    10Hz

    150Hz

    1kHz

    4kHz

    5kHz

    6kHz

    Lower -3dB Upper -3dB

    Simulated

    Measured

    Error

    Table 4.1 Band-Pass Filter Output Characteristics with 6Load

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    SEAS

    POST-LAB ANALYSIS

    Be certain to include:1. Your calculationsfor how you designed the band-pass filter.

    2. The Multisimschematicfor the band-pass filter.

    3. The Multisimoutputshowing Vout/Vin(in dB) versus frequency for the low-pass filter, high-pass

    filter, and finally the band-pass filter.

    Answer the following questions and provide some discussion on the following:1. Whywas the LM741 incapable of driving a 6load?

    2. Whyis the LM386 capable of driving the 6load?

    3. Whydid we use the speaker instead of a 6resistor in Part IV?

    REFERENCES

    [1] Thomas, Roland E., Albert J. Rosa, and Gregory J. Toussaint. The Analysis and Design of LinearCircuits. 7

    thed. Hoboken, NJ: Wiley, 2012.