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Frequency Response of Amplifier
Jack OuSonoma State University
RC Low Pass (Review)
𝑉 𝑜𝑢𝑡 (𝑆 )𝑉 𝑖𝑛 (𝑆 )
=1/(1+𝑠𝑅𝐶)
A pole: a root of the denomintor1+sRC=0→S=-RC
Laplace Transform/Fourier Transform
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
(𝑠)=1/(1+𝑠𝑅𝐶)
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
( 𝑗ω)=1 /(1+ 𝑗ω 𝑅𝐶)
𝑠= 𝑗ω
)|=1/| +p|
Phase=-tan-1(/p)
p=1/(RC)
(Fourier Transform)
(Laplace Transform)
𝑗ω
-p
𝑗ω| +p|
Location of the zero in the left complexplane
𝜎
Complex s plane
Rules of thumb: (applicable to a pole)Magnitude:1. 20 dB drop after the cut-off frequency2. 3dB drop at the cut-off frequencyPhase:3. -45 deg at the cut-off frequency4. 0 degree at one decade prior to the cut-frequency5. 90 degrees one decade after the cut-off frequency
RC High Pass Filter (Review)
𝑉 𝑜𝑢𝑡 (𝑆 )𝑉 𝑖𝑛 (𝑆 )
=𝑠𝑅𝐶 /(1+𝑠𝑅𝐶)
A zero at DC.A pole from the denominator.1+sRC=0→S=-RC
Laplace Transform/Fourier Transform
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
(𝑠)=𝑠𝑅𝐶 / (1+𝑠𝑅𝐶)
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
( 𝑗ω)= 𝑗ω𝑅𝐶 /(1+ 𝑗ω𝑅𝐶)
𝑠= 𝑗ω
)|=| |/| +p|
Phase=90-tan-1(/p)
p=1/(RC)Zero at DC.
(Fourier Transform)
(Laplace Transform)
𝑗ω
-p
𝑗ω| +p|
Location of the zero in the left complexplane
𝜎
Complex s plane
Zero at the origin.Thus phase(f=0)=90 degrees.The high pass filter has a cut-off frequency of 100.
RC High Pass Filter (Review)
𝑉 𝑜𝑢𝑡 (𝑆 )𝑉 𝑖𝑛 (𝑆 )
= 𝑅1𝑅1+𝑅2
1+𝑠𝑅1𝐶1+𝑠𝑅12𝐶
R12=(R1R2)/(R1+R2)A pole and a zero in the left complex plane.
Laplace Transform/Fourier Transform (Low Frequency)
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
(𝑠)=𝑅1
𝑅1+𝑅21+𝑠𝑅1𝐶1+𝑠𝑅12𝐶
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
( 𝑗ω)=𝑅1
𝑅1+𝑅21+ 𝑗ω𝑅1𝐶1+ 𝑗ω𝑅12𝐶
𝑠= 𝑗ω
z=1/(RC)p=1/(R12C)
(Fourier Transform)
(Laplace Transform)
𝑗ω
-p
𝑗ω| +p|
Location of the zero in the left complexplane
𝜎
Complex s plane
| +z|
-z
At low frequencies, | +p|>| +p|.
Laplace Transform/Fourier Transform (High Frequency)
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
(𝑠)=𝑅1
𝑅1+𝑅21+𝑠𝑅1𝐶1+𝑠𝑅12𝐶
𝑉 𝑜𝑢𝑡𝑉 𝑖𝑛
( 𝑗ω)=𝑅1
𝑅1+𝑅21+ 𝑗ω𝑅1𝐶1+ 𝑗ω𝑅12𝐶
𝑠= 𝑗ω
z=1/(RC)p=1/(R12C)
(Fourier Transform)
(Laplace Transform)
𝑗ω
-p
𝑗ω| +p|
Location of the zero in the left complexplane
𝜎
Complex s plane| +z|
-z
At high frequency, | +p|is almost equal to | +p|.
Design
• ωz=1/R1C
• ωp=1/(R12)C
• Note that R12<R1
• If R2<<R1, ωp/ ωp=R1/R2
• Design for ωp/ ωp=1000
High Frequency
Examples
Source Follower
Device Setup
Gmoverid:
Gm=17.24 mSRS=1000 OhmsGMBS=2.8 mSCGS=62.79 fF
Small Signal Parameters
Design Constraints:1. 1/(gm+gmbs)=50 Ohms2. Large R1 to minimize Q
R2=58 OhmsR1=1102 OhmsL=4.013 nH
Simulation Results
Current Mirror Example
Gm1=201.3uSGM3=201uSCGS3=CGS4=306.9fFGDS4=3.348uSGDS2=5.119uSRload=118 KohmsCload=1 pF
Fp1=1.347 MHzFp2=52.11 MHzFz=104.2 MHz
Magnitude
AvDC,matlab=27.52AvDC,sim=27.45
Fp1matlab=1.34MHzFp1sim=1.23 MHz
Phase
Transit Frequency
Transit Frequency Calculation
Understanding Transit Frequency
Since fT depends on VGS-VT, fT depndes on gm/ID.fT depends on L.
Overdrive Voltage as a function of gm/ID
gm/ID=2/(VOV)
Transit Frequency as function of gm/ID
gm/gds as a function of gm/ID
Trade-off of gm/gds and fT
15-20
fT
gm/gds
gm/ID
Numerical Example
L=120n gm/gds fT(Hz)
gm/ID=5 12.05 84.32G
gm/ID=10 15.71 64.05G
gm/ID=15 17.19 43.94G
gm/ID=20 17.54 22.76G
gm/ID=25 17.05 0.42 G
VDS=0.6 V
Numerical Example
gm/ID=20 gm/gds fT(Hz)
L=0.12um
17.54 22.7 G
L=0.18 um
29.88 12.6 G
L=0.25 um
37.35 7.96 G
L=1 um 46.00 714.4 M
L=2 um 47.26 190.3 MVDS=0.6 V
gm/ID Principle
Use to gm/ID principle to find capacitance
• gm/ID→(fT,I/W,gm/gds)
• fT=gm/cgg, cgg=cgs+cgb+cgd
• cgs/cgg is also gm/ID dependent.
Example
• Assume gm/ID=20, L=120 nm, VDS=0.6V, I=100uA.
• fT=22.76 GHz• cgg=gm/fT=13.98 fF
• cgd/cgg=0.29→cgd=4.1 fF
• cgs/cgg=0.75 →Cgs=10.5 fF
Noise
Noise is not deterministic
The value of noise cannot be predicted at any time even if the past values are known.
Average Power of a Random Signal
Observe the noise for a long time.
Periodic voltage to a loadresistance.
Unit: V2 rather than W.
It is customary to eliminate RL from PAV.
Power Spectral Density
PSD shows how much Power the signal carriesat each frequency.
Sx(f1) has unit of V2/Hz.
PSD of the Output Noise
PSD of the Output Noise
Output Noise
PSD of the Input Noise
Input Noise
Noise Shaping
Correlated and Uncorrelated Sources
(How similar two signals are.)
Pav=Pav1+Pav2
Superposition holds for only for uncorrelated sources.
Uncorrelated/Correlated Sources
(Multiple conversations in progress)
(clapping)
Resistor Thermal Noise
Example
Vnr1sqr=2.3288 x 10-19
Vnr3sqr=7.7625 x 10-20
Vnoutsqr=3.1050 x10-19
Analytical Versus Simulation
as a function of length
Corner Frequency (fco)
fco as a function of length