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Recall Lecture 17 MOSFET DC Analysis

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1 Recall Lecture 17 MOSFET DC Analysis
Using GS (SG) loop to calculate VGS Remember that there is NO gate current! Assume in saturation Calculate ID using saturation equation Find VDS (for NMOS) or VSD (for PMOS) Using DS (SD) loop Calculate VDS sat or VSD sat Confirm that VDS > VDS sat or VSD > VSD sat Confirm your assumption!

2 CHAPTER 7 Basic FET Amplifiers

3 For linear amplifier function, FET is normally biased in the saturation region.

4 Need to do DC Analysis first to find ID
AC PARAMETERS where Need to do DC Analysis first to find ID vgs gmvgs

5 The MOSFET Amplifier - COMMON SOURCE
The output is measured at the drain terminal The gain is negative value Three types of common source source grounded with source resistor, RS with bypass capacitor, CS

6 Common Source - Source Grounded
A Basic Common-Source Configuration: Assume that the transistor is biased in the saturation region by resistors R1 and R2, and the signal frequency is sufficiently large for the coupling capacitor to act essentially as a short circuit. + vgs - gmvgs

7 EXAMPLE The transistor parameters are:
VDD = 5V RD = 10 k 520 k 320 k 0.5 k The transistor parameters are: VTN = 0.8V, Kn = 0.2mA/V2 and  = 0. Voltage Divider biasing: Change to Thevenin Equivalent RTH = 198 k VTH = V

8 gm = 0.442 mA/V DC ANALYSIS Calculate the value of VGS VGS – VTH = 0
Confirm your assumption: VDS > VDSsat, our assumption that the transistor is in saturation region is correct Assume the transistor is biased in the saturation region, the drain current: Use KVL at DS loop IDRD + VDS – VDD = 0 VDS = VDD – IDRD = 2.56 V Calculate the value of VGS VGS – VTH = 0 VGS = V Calculate VDSsat = VGS – VTN = – 0.8 = V gm = mA/V

9 Equivalent resistance at the output side, ROUT
COMMON EMITTER GROUNDED OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vbeROUT INPUT SIDE Calculate Ri Get vbe in terms of vs – eg: using voltage divider. Go back to vo equation and calculate the voltage gain COMMON SOURCE GROUNDED OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vgs ROUT ____________________________________________ INPUT SIDE Get vgs in terms of vi eg: using voltage divider. Go back to vo equation and calculate the voltage gain

10 The output resistance, Rout = RD The output voltage:
RTH 198.1 k 0.5 k RD = 10 k 0.442 vgs + vgs - The output resistance, Rout = RD The output voltage: vo = - gmvgs (Rout) = - gmvgs (10) = vgs Get vgs in terms of vi - voltage divider vgs = [198.1 / ( )] = vi  vi = vgs Go back to vo equation and calculate the voltage gain Av = vo / vi = vgs / vgs 

11 Current Gain Output side: io = vo / RD = vo / 10
RSi vi RD RTH Output side: io = vo / RD = vo / 10 Input side: ii = vi / (Rsi + RTH ) = vi / ( ) = vi / 198.6 Current gain = io / ii = vo (198.6) = * = vi (10)

12 Type 2: With Source Resistor, RS
VTN = 1V, Kn = 1.0 mA /V2 RTH = k VTH = ( 200 / 300 ) x 3 = 2 V

13 Calculate the value of VGS KVL at GS loop:
DC ANALYSIS Assume the transistor is biased in the saturation region, the drain current: Calculate the value of VGS KVL at GS loop: 0 + VGS+ 3(ID) - 2 = 0 VGS = 2 - 3ID VTN = 1V, Kn = 1.0 mA / V ID = mA Replace in VGS equation in step 1 VGS = 2 - 3ID VGS= V ID = mA VGS = 1.43 V Why choose VGS = 1.43 V ? Because it is bigger than VTN

14 gm = 0.872 mA/V Use KVL at DS loop IDRD + VDS + IDRS – 3 = 0
Calculate VDSsat = VGS – VTN = 1.43 – 1 = 0.43V Confirm your assumption: VDS > VDS sat , our assumption is correct IDRD + VDS + IDRS – 3 = 0 VDS = V gm = mA/V  = 0 ro =  VA = 

15 Equivalent resistance at the output side, ROUT
COMMON EMITTER with RE OUTPUT SIDE Get the equivalent resistance at the output side, ROUT Get the vo equation where vo = -  ib ROUT INPUT SIDE Calculate Rib = vb / ib : KVL at loop (extra step) Calculate Ri Get vb in terms of vs – eg: using voltage divider. Go back to vo equation and calculate the voltage gain COMMON SOURCE with RS OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vgs ROUT ________________________________________________________ INPUT SIDE Get v’ in terms of vgs : KVL Get v’ in terms of vi – eg: using voltage divider Go back to vo equation and calculate the voltage gain

16 v’ = vgs + gmvgs RS  v’ = vgs(1 + 2.616) = 3.616 vgs
RTH 66.67 k RD = 10 k RS = 3 k + v’ - The output resistance, Rout = RD The output voltage: Find v’ v’ = vgs + gmvgs RS  v’ = vgs( ) = vgs vo = - gmvgsRD = ( vgs) (10) = vgs

17 5. Calculate the voltage gain
RTH 66.67 k RD = 10 k RS = 3 k + v’ - 4. Find v’ in terms of vi v’ = vi  in parallel vi = vgs 5. Calculate the voltage gain AV= vo / vi = vgs / vgs =

18 Current Gain Output side: io = vo / RD = vo / 10
vi RD RTH Output side: io = vo / RD = vo / 10 Input side: ii = vi / (RTH ) = vi / ( ) = vi / 66.67 Current gain = io / ii = vo (66.67) = * = vi (10)

19 Type 3: With Source Bypass Capacitor, CS
Circuit with Source Bypass Capacitor An source bypass capacitor can be used to effectively create a short circuit path during ac analysis hence avoiding the effect RS CS becomes a short circuit path – bypass RS; hence similar to Type 1

20 Equivalent resistance at the output side, ROUT
COMMON EMITTER with CE OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vbeROUT INPUT SIDE Calculate Ri Get vbe in terms of vs – eg: using voltage divider. Go back to vo equation and calculate the voltage gain COMMON SOURCE with CS OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vgs ROUT ____________________________________________ INPUT SIDE Get vgs in terms of vi eg: using voltage divider. Go back to vo equation and calculate the voltage gain

21 IQ = 0.5 mA hence, ID = 0.5 mA ro =  gm = 1.414 mA/V + vgs -
RG 200 k RD = 7 k 1.414 vgs + vgs -

22 The output resistance, Rout = RD The output voltage:
RG 200 k RD = 7 k 1.414 vgs + vgs - The output resistance, Rout = RD The output voltage: vo = - gmvgs (RD) = (7) vgs = vgs 3. The gate-to-source voltage: vgs = vi  in parallel ( no need voltage divider) 4. So the small-signal voltage gain: Av = vgs / vgs =

23 Current Gain Output side: io = vo / RD = vo / 7
vi RD RG Output side: io = vo / RD = vo / 7 Input side: ii = vi / (RG ) = vi / ( ) = vi / 200 Current gain = io / ii = vo (200) = * = vi (7)

24 The MOSFET Amplifier - COMMON DRAIN
The output is measured at the source terminal The gain is positive value

25 VTN = 0.92 V, Kn = 4 mA /V2 ,  = 0.01 V-1 VDD = 11 V 0.5 k
RS = 0.75 k 0.5 k VDD = 11 V VTN = 0.92 V, Kn = 4 mA /V2 ,  = 0.01 V-1 RTH = k VTH = ( 470 / 620 ) x 11 = 8.34 V

26 Calculate the value of VGS KVL at GS loop:
DC ANALYSIS Assume the transistor is biased in the saturation region, the drain current: Calculate the value of VGS KVL at GS loop: 0 + VGS (ID) – 8.34= 0 VGS = 8.34 – 0.75ID ID = mA Replace in VGS equation in step 1 VGS = 2 - 3ID VGS= V ID = 8 mA VGS = 2.34 V Why choose VGS = 2.34 V ? Because it is bigger than VTN

27 gm = 11.3 mA/V Use KVL at DS loop VDS + IDRS – 11 = 0 VDS = 5 V
Calculate VDSsat = VGS – VTN = 2.34 – 0.92 = 1.42 V Confirm your assumption: VDS > VDS sat , our assumption is correct VDS + IDRS – 11 = 0 VDS = 5 V gm = 11.3 mA/V ro = 12.5 k VA = 100 V  = 0.01 V-1

28 RTH k 0.5 k vgs gmvgs

29 COMMON COLLECTOR COMMON DRAIN OUTPUT SIDE
Get the equivalent resistance at the output side, ROUT At node x, use KCL and get io in terms of ib where io = ib +  ib Get the vo equation where vo = io ROUT INPUT SIDE Find vb in terms of ib using supermesh Calculate Rib – input resistance seen from base: Rib = vb / ib Calculate Ri Get vb in terms of vs. Go back to vo equation and get the voltage gain COMMON DRAIN OUTPUT SIDE Equivalent resistance at the output side, ROUT Calculate vo = gmvgsRout ________________________________________________________ INPUT SIDE Find v’ in terms of vgs : supermesh Find v’ in terms of vi Go back to vo equation and get the voltage gain

30 vo = gmvgs (ro  RS) = 11.3 vgs (0.70755) = 8 vgs
+ v’ - k RS = 0.75 k 12.5 k The output resistance: The output voltage v’ in terms of vgs using supermesh: v’ in terms of vi: The voltage gain Ro = ro || Rs = k vo = gmvgs (ro  RS) = 11.3 vgs ( ) = 8 vgs vgs + vo– v’ = 0 v’ = vgs + 8 vgs = 9 vgs v’ = (RTH / RTH + RSi) vi = vi 9vgs = vi  vi = vgs Av = vo / vi = 8 vgs / vgs = 0.885

31 Current Gain Output side: io = vo / Rs = vo / 0.75
RSi vi Rs = 0.75 k RTH RTH k Output side: io = vo / Rs = vo / 0.75 Input side: ii = vi / (Rsi + RTH ) = vi / ( ) = vi / Current gain = i / ii = vo (114.21) = * = vi (0.75)

32 Output Resistance for Common Drain
vgs + - Vx Ix RSi Independent voltage source turned off 12.5 k RS 0.75 k RTH 11.3 vgs ro In parallel ro|| Rs = k vgs in terms of Vx where vgs = - Vx 0.708 k 11.3 vgs vgs + - Vx Ix

33 - 1.412 Vx – 11.3 Vx + Ix = 0 Ix = 12.712 Vx 0.079 k vgs + - Vx Ix
Use nodal analysis - Vx gmvgs Ix = 0 0.708 vgs = - Vx and gm = 11.3 mA/V - Vx gmVx Ix = 0 0.708 Vx – 11.3 Vx + Ix = 0 Ix = Vx 0.079 k

34 SUMMARY

35 COMMON EMITTER GROUNDED
OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vbeROUT INPUT SIDE Calculate Ri Get vbe in terms of vs – eg: using voltage divider. Go back to vo equation and calculate the voltage gain COMMON SOURCE GROUNDED OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vgs ROUT ____________________________________________ INPUT SIDE Get vgs in terms of vi eg: using voltage divider. Go back to vo equation and calculate the voltage gain

36 Equivalent resistance at the output side, ROUT
COMMON EMITTER with RE OUTPUT SIDE Get the equivalent resistance at the output side, ROUT Get the vo equation where vo = -  ib ROUT INPUT SIDE Calculate Rib = vb / ib : KVL at loop (extra step) Calculate Ri Get vb in terms of vs – eg: using voltage divider. Go back to vo equation and calculate the voltage gain COMMON SOURCE with RS OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vgs ROUT ________________________________________________________ INPUT SIDE Get v’ in terms of vgs : KVL Get v’ in terms of vi – eg: using voltage divider Go back to vo equation and calculate the voltage gain

37 COMMON EMITTER with CE OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vbeROUT INPUT SIDE Calculate Ri Get vbe in terms of vs – eg: using voltage divider. Go back to vo equation and calculate the voltage gain COMMON SOURCE with CS OUTPUT SIDE Equivalent resistance at the output side, ROUT Get the vo equation where vo = - gm vgs ROUT ____________________________________________ INPUT SIDE Get vgs in terms of vi eg: using voltage divider. Go back to vo equation and calculate the voltage gain

38 COMMON COLLECTOR COMMON DRAIN OUTPUT SIDE
Get the equivalent resistance at the output side, ROUT At node x, use KCL and get io in terms of ib where io = ib +  ib Get the vo equation where vo = io ROUT INPUT SIDE Find vb in terms of ib using supermesh Calculate Rib – input resistance seen from base: Rib = vb / ib Calculate Ri Get vb in terms of vs. Go back to vo equation and get the voltage gain COMMON DRAIN OUTPUT SIDE Equivalent resistance at the output side, ROUT Calculate vo = gmvgsRout ________________________________________________________ INPUT SIDE Find v’ in terms of vgs : supermesh Find v’ in terms of vi Go back to vo equation and get the voltage gain


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