experiment # 3
DESCRIPTION
Experiment # 3. EE 312 Basic Electronic Instrument Laboratory September 13, 2000 See Lecture 5 Filters on 1999 EE 312/352 Website www.ee.buffalo.edu/~whalen/ee352. Objectives:. Design and assemble of Resistance- Capacitance (RC) and Resistance-Inductance (RL) filters. - PowerPoint PPT PresentationTRANSCRIPT
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Experiment # 3
EE 312 Basic Electronic Instrument LaboratorySeptember 13, 2000
See Lecture 5 Filters on 1999 EE 312/352 Websitewww.ee.buffalo.edu/~whalen/ee352
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Objectives:• Design and assemble of Resistance-
Capacitance (RC) and Resistance-Inductance (RL) filters.
• Measure the frequency response (magnitude & phase) of RC and RL filters.
• Examine the time-domain responses of these filters to a square-wave voltage .
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Background:
R
j
C
j L
Impedance
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Rj
C
R
j LHigh-Pass RL Filter
Low Pass RL Filter
High-Pass RC Filter
Low-Pass RC Filter
High
Low
Low
High
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time0
time
Vout(t)
Rj
C
0
Vin(t)
Example: Low-Pass RC Filter
0
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A tV t
V t
out
in( )
( )
( ) ? & Phase shift ?
time0
time
Vout(t)
Rj
C
0
Vin(t)Low-Pass RC Filter
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Calculation for a High Pass Filter(Steady State Response)
)1()(1
1
)(
)(
2
22
R
Xj
RX
jXRXR
R
jXR
jXR
jXR
R
jXR
R
V
V
C
C
C
C
C
C
C
Cin
out
R
-jXc
CfXC
2
1
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X
R fCR
fRC
X
R
f
f
V
V f
f
jf
f
c
x
c x
out
in x
x
1
2
1
2
1
11
2
( )( )
but
Define crossover frequency, fx, as
Then
so
First, look at this factor
fx, roughly speaking, is the frequency that separate the frequency range for which a filter passes signals from the range for which the filter attenuates signals
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1 jf
f
x?
1 1
1
1
2 2
2
2
( ) cos ( ) sin
( ) (cos sin )
( )
f
fj
f
f
f
fj
f
fe
x x
x
x j
1
1 2 ( )f
f
x
f
f
x
tan f
f
x tan ( )1 f
f
xPhase shift
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V
V f
f
f
fe
V
V f
f
e
out
in x
x j
out
in x
j
1
11
1
1
2
2
2
( )( )
( )
so:
or
Amplitude
Phase
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V
V f
f
eout
in x
j
1
1 2( )
When f >> fx, Amplitude 1, 0
Thus, this is high pass
When f << fx, Amplitude 0, 90
Low frequencies are blocked
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Step ResponseHigh-Pass Low-Pass
Vin
Vout Vout
Vin
Voltage on capacitor cannot change instantaneously. So Vout = Vin initially.
Voltage on capacitor cannot change instantaneously. So Vout = 0 initially.
Vin Vout Vin Vout
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RC
Fall Time
Vout
time
1.00.9
0.1 10%
90%
100%
1/e~37%
et
RC
Fall Time & Time Constant ( )
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Relationship Between Time Constant T & Rise-Time or Fall-Time
T = RC or L/R
Rise-Time (Fall-Time) = T X ln9 = 2.2T
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Components:
• Resistor Substitution Box
• Capacitor Substitution Box
• 1 mH Inductor
• 100 Ohms Resistor
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RFunction Generator
oscilloscope
Filter ScopeOscillator
FG has 50 ohm internal resistance- keep R high enough so that crossover freq. has no more than a 10% dependence upon it. e. g. R > 500 ohm
CRO has 1 M input impedance - keep R low enough so that crossover freq has no more than a 10% dependence upon it. R < 100k
Choose C so that crossover frequency fx = 1/(2RC) is well within FG frequency range. E.G. fx ~ 3 kHz.
Comment:
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Procedures:• 1- Determine internal impedance of the function
generator which is expected to be ~50 ohms
• 2- Measure low-pass RC filters characteristics
• 3- Measure low-pass RL filters characteristics
• 4- Simulate RC & RL low-pass filters (Bell 242)
• 5-Measure time constant and fall time in a high-pass RC filter using a square wave
• 6- Measure time constant and rise time in a low-pass RL filter using a square wave
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1- Internal Impedance of Function Generator
Filter impedance >> Generator impedanceRload > 10 X Rinternal
Rinternal
RLoadFunction Generator
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Step 2- Measure the decreased amplitude of the output signal and Ix with 100 ohms resistor
Rinternal
Function Generator
oscilloscope 1M
Step 1- Set Vp-p=10V
Step 3- Determine Rinternal
Rinternal
100Function Generator
oscilloscopeIx
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2- Low-Pass RC Filter
~
CRO CH2CRO CH1
Assemble a low-pass RC filter having a Crossover frequency of about 3 kHz
fRC
x 1
2
R
C
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~
CRO CH2CRO CH1
Vp-p=10V Vout
VoutFrequency..
fx..
a) b)
Use Digital CRO to readout directly phase difference between input and output
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3- Low-Pass RL Filter
~
L=1 mH
R VoutVin
Repeat the procedure in step 2 for an appropriate crossover frequency in the range 100 kHz to 150 kHz.
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4- Simulation (PSpice)
• Simulate the RC and RL low-pass filters in parts 2 and 3. Do so in Bell 242.
• Perform an ac sweep between frequencies of 1Hz and 1 MHz (or from fx/100 to 100 fx) with 20 to 50 data points per decade.
• Display experimental and PSPICE values for the magnitude (dB) and phase of the output voltage on the same graph.
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5- Time Constant and Fall Time in a High-Pass RC Filter
to oscilloscope
Vout
Vin R
C
Measure the time constant and fall time.Use Digital CRO to readout directly fall time.Use Digital CRO Cursors to determine T = RC
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6- Time Constant & Rise Time in a Low-Pass RL Filter
L=1 mH
R VoutVin
Measure the time constant and fall time.Use Digital CRO to readout directly fall time.Use Digital CRO Cursors to determine T = L/R