op-amps in signal processing applications
TRANSCRIPT
OP-AMPS in SIGNAL PROCESSING APPLICATIONS
Filters, Integrators, Differentiators, and Instrumentation Amplifier
Sensors :definition and principles
Sensors : taxonomies• Measurand
– physical sensor– chemical sensor– biological sensor(cf : biosensor)
• Invasiveness– invasive(contact) sensor– noninvasive(noncontact) sensor
• Usage type– multiple-use(continuous monitoring) sensor– disposable sensor
• Power requirement– passive sensor– active sensor
What is electronics engineering all about?Process
Sensors/ transducers
Filters
Amplifiers Feedback
Actuators/transducers
New process
A/D converters Computers
D/A converters
Physical variables
Electrical variablesV, I, t, f
Physical variables
F, P, d, v, t, f
What is a Signal Processor?
• It selects useful parts of a signal
• It cleans signal from impurities
• It compares signals
• It converts signals into forms that can be easily recognized
The ECG wave in it’s raw form
Examples of biomedical
signals
Examples of Signal Processors
• Basic amplifiers – already discussed
• Instrumentation amplifier – an improved differential amplifier
• Active filters
• Integrators and differentiators
• Extra Reading:– Precision rectifiers
– Logarithmic amplifiers
– Negative capacitance amplifiers
Signal Conditioning
• Ideal operational amplifier
• Inverting, non-inverting and instrument amplifier
• Integrator, differentiator
• Filters
• Examples of signal conditioning module
Ideal Operational Amplifier
Operational (OP) amplifier is a high-gain dc differential amplifier. It is made of an integrated circuit chip. It has two inputs, negative terminal v1 and positive terminal v2 and one output v0. The effective input to the amplifier is the voltage difference of the two inputs v1-v2.
Properties of Ideal OP Amplifier
• Gain if infinity (A=∞).
• V0 = 0, when v1 = v2
• Input impedance is infinity.
• Output impedance is zero.
• Bandwidth is infinitely wide and has no phase shift.
Basic Rules for Ideal OP Amplifier
• When the OP amplifier output is in its linear range, the two input terminals are at the same voltage.
• No current flows into either input terminal of the OP amp.
Inverting Amplifier
Non-inverting Amplifier
Instrument Amplifier
Active Filters
• Low-pass
• High-pass
• Band-pass
• Band-stop (notch)
• All-pass (phase-shift)
Low-pass filter: circuit
i
f
ZZ
G −=
V0 Vi A +
- Ri Rf
Cf
GL = Rf/Ri ; τf = RfCf ; fc = 1/2πτf
Derive the equation for gain G
What are the important parameters?
)()(0
ωω
jVjVG
i
=
i
ff
f
f
R
RCj
CjR
+
−=ω
ω
1
( ) f
L
fi
f
iff
f
jG
jRR
RCRjR
ωτωτω +=
+−=
+−=
111
1
Low-pass filter: characteristics
Gain/GL
f/fc
0.1 1 10 100
0.1
0.01 Slope = -1
1
-3π/2
Phase f/fc
-5π/4
-π
GL = Rf/Ri ; τf = RfCf ; fc = 1/2πτf
V0 Vi A +
- Ri Cf
Integrator – ideal: circuit
i
f
i
f
i RCj
ZZ
jVjVG
ωωω
1
)()(0 −=−==
VirtualGround
i
i
∫ +−=t
iCifi
VdtVCR
V00
1
dtdVC
RVi f
i
i 0==
Express V0 in terms of Vi Write expression for gain G
ffi jCRj ωτω11
−=−=
Where τ = RiCf
Integrator – ideal: characteristics
G/GL
f/fc
0.1 1 10 100
0.1
0.01
0
10
100
Slope = -1
1
-3π/2
Phase f/fc
-5π/4
-π
Draw G/GL versus f/fc
Draw phase versus f/fc
ffG cc ====
ωω
ωτ1
°−=−= 2702/3πθ
The integrator with bias currents
Through which component the bias current flows?
Gain/GL
f/fc
0.1 1 10 100
0.1
0.01 Slope = -1
Integrator - practical
V0 Vi A +
- Ri
Rf
Cf
f
L
fi
f
i jG
jRR
jVjVG
ωτωτωω
+=
+−==
111
)()(0
Without Rf
With Rf
Rf provides route for DC bias currents 1Phase f/fc
-3π/2
-5π/4
-π
Without Rf
Low-pass filter Integ.
fcfff fCR
πττ
21; ==
Charge amplifier
vo
Electrode
The piezoelectric sensor generates charge, which is transferred to the capacitor, C, by the charge amplifier. Feedback resistor Rcauses the capacitor voltage to decay to zero
Charge amplifier: circuit
V0 IsC
FET +
-
Rf
Cf
IsR
dtKdxidtdq ss // ==
Piezoelectric sensor
Is
VirtualGround
IsC = IsR = 0 ∫ −=−=−=t
ff CKXdt
dtKdx
CVV
001
Step response of a charge amplifierxi
Deflection
vo
vo max
vo max /e
Time
Time
The charge amplifier responds to a step input with an output that decays to zero with a time constant τ = RfCf
High-pass filter: circuit
V0 Vi A +
- Ri Rf Ci
i
f
i ZZ
jVjVG −==
)()(0
ωωGH = -Rf/Ri ; τi = RiCi ; fc = 1/2πτi
Derive the equation for gain G
What are the important parameters?
i
Hi
i
i
i
f
jGj
jj
RR
ωτωτ
ωτωτ
+=
+−=
11ii
if
ii
f
CRjCRj
CjRR
Gω
ω
ω +−=
+−=
11
High-pass filter: characteristicsGain/GH
f/fc
0.1 1 10 100
0.1
0.01Slope = +1
1
-π
Phase f/fc
-3π/4
-π/2
Draw G/GH versus f/fc
Draw phase versus f/fc
Differentiator - ideal
V0 Vi A +
- Rf Ci
I
I
dtdVCRV
dtdVCi
iif
ii
−=
=
0
ωτωωω
ω
jCRjGCj
RZZ
jVjVG
if
i
f
i
f
i
−=−=
−=−== 1)()(0
Slope = +1
fc = 1/2πτ
Phase shift = - 90o
Gain
f/fc
0.1 1 10 100
0.1
0.01
1
10
100
Express V0 in terms of Vi
Write expression for gain G
Differentiator - practical
V0 Vi A +
- Rf Ci
Cf
f
f
f
i
ff
if
i
ff
ff
i
f
i jj
CC
CRjCRj
Cj
CjRCjR
ZZ
jVjVG
ωτωτ
ωω
ω
ω
ω
ωω
+−=
+−=
+−=−==
111
1
1
)()(0
In an ideal differentiator, the highfrequency response is limited by theopen-loop gain of the op-amp yieldinga very noisy output voltage.
τf = RfCf ; fc = 1/2πτf
Cf is used to limit the hf gain, hence the hf noise.
The gain at hf: GH = - Ci/Cf
Differentiator characteristics
Slope = +1
1
-π
Phase f/fc
-3π/4
-π/2
Gain/GH
f/fc
0.1 1 10 100
0.1
0.01
10 Without Cf
With Cf
With Cf
Differentiator High-pass filter
Measurement of integrator and differentiator characteristics
V0 Vi A +
- 1k5
15 k
10 nF
Integrator
• Form your lab team and assign duties.
• Go to the lab bench.
• Built the circuit given: integrator for team 1 and differentiator for team 2
• Connect the power supply.
• Connect the CRO
• Do the experiment according to the procedures in the sheet - 6.
• Switch off the PS and signal generator
• Return your seat
V0 Vi A +
- 15 k 0.1µF
10 nF Differentiator
Band-pass filter: circuit
V0 Vi A +
- Ri Rf
Cf
Ci
( )( )
)1)(1()1)(1(
111
1
)()(0
fi
iMB
fi
i
i
f
iiff
fi
ii
ff
f
f
i
f
i
jjjG
jjj
RR
G
CRjCRjRCj
CjR
RCj
CjR
ZZ
jVjVG
ωτωτωτ
ωτωτωτ
ωωω
ω
ω
ω
ωω
++=
++−=
++−=
+
+
−=−==
Mid-band gain =GMB = - Rf/Ri
Time-constants: τI= RiCi ; τf = RfCf
Critical frequencies: fL = 1/2πτI ; fH = 1/2πτf
Band-pass filter: characteristics
Gain/GH
f/fc
0.1 1 10 100
0.1
0.01
Slope = -1Slope = +1
Band-pass filter (non-inverting)
Frequency response of bpf
BPF with bias compensation
Comparators: Basic Rules
• V0=A(V2-V1)• V0 = 0 if V1 = V2
• V0 = +VSAT if V1 < V2
• V0 = -VSAT if V1 > V2
• No current flows into either input terminals of the op-amp.
V0
V1
V2 A
+
-
Simple comparator (inverting)
V0 Vref A
+
- R1
R2
Vi
V-
Output stays at +VSAT if V-<0
V- = (Vi*R2+Vref*R1)/(R1+R2)
Output goes to -VSAT if V->0
+10V
-10V
V0
Time
-Vref*R1/(R1+R2)
Vi*R2/(R1+R2)
V0
Vi
10V
10V -10V
-10V -Vref*R1/R2
-VSAT
VSA
T
Comparator with hysteresis
V0 Vref A
+
- R1
R2
Vi
V-
R3 R4
V+
V- = (Vi*R2+Vref*R1)/(R1+R2)
V+ = V0*R3 /(R3+R4)
Output stays at +VSAT if V-<V+
Output goes to -VSAT if V->V+
Characteristics
V0 Vref A
+
- R1
R2
Vi
V-
R3 R4
V+
V0
Vi
10V
10V -10V
-10V VL
+VSAT
-VSAT
VH
Vhys
VH = -Vref*R1/R2 – VSAT*R3/(R3+R4)
VL = -Vref*R1/R2 + VSAT*R3/(R3+R4)
+10V
-10V
V0
Time
-Vref*R1/(R1+R2)
Vi*R2/(R1+R2)
VH
VL
Vhys
Op-Amps in Reality
• Fabricated using integrated-circuit technologies– Inside an op-amp:
1) Transistors
2) Parasitic capacitors
3) Internal resistors
• Op-amp chip configuration that we will use: Quad-channel (i.e. 4-in-1)– 14 pins in the op-amp chip
Instrumentation Amplifier
Overall Circuit Structure
• Overall differential gain is given by:
R4
R3
vo
R3
R4
R2
va
R2
R1
vb
VS+
VS+
VS+
1
221RRG +=α
3
4
RRG =β
+==
3
4
1
221RR
RRGGGD βα
DifferenceAmplifier
Input Conditioner
VS–
VS–
VS–
In-Amp: Input Conditioner
• Note that iR1 = iR2a = iR2b. Then the diff. output voltage is given by:
• The diff. input voltage is equal to:
• The differential gain is thus equal to:
R2
va
R2
R1
vb
VS+
VS+
va'
vb'
iR1
iR2a( )211 2'' RRivv Rab +=−
iR2b
1
221''RR
vvvvG
ab
abD +=
−−
=
11Rivv Rab =−VS–
VS–
In-Amp: Input Conditioner
• This input conditioner does not amplify common-mode signals!
• Brief proof of principle:– Since vb – va = iR1R1:
– The output voltages are thus equal to:
01 =⇒== Rcmba ivvv
cmba vvv == ''
R2
va
R2
R1
vb
VS+
VS+
va'
vb'
iR1
iR2a
iR2b
VS–
VS–
In-Amp: Difference Amplifier
1) From voltage divider principles:
2) Note that iR1a = iR2a. Thus:
R2
R1
vbvo
va
R1
R2
VS+
+
=+21
2
RRRvv b iR1a
iR2a
12 Rvv
Rvv ao −
=− −−
1122
11Rvv
RRRv ao −
+=⇒ −
VS–
In-Amp: Difference Amplifier
3) Note that v– = v+. So from the voltage divider expression:
4) Substituting the above into the output voltage expression, we get:
R2
R1
vbvo
va
R1
R2
VS+iR1a
iR2a
1
2
1
2 )(RR
vvvGvv
RRv
ab
odabo =
−=⇒−=⇒
+
=−21
2
RRRvv b
112
2
12
12
2 Rvv
RRR
RRRR
Rv a
bo −
+
+=
VS–