EE 420L - Lab 6

Single-stage transistor amplifiers 

 

Authored by Nicholas Moya

March 19th, 2015

moyan1@unlv.nevada.edu

  

In this lab, we detail the operation of Common Drain (CD) amplifiers, also known as source followers, Common Source (CS) amplifiers, and Common Gate amplifiers using both CMOS and NMOS transistors. The circuits are analyzed in both DC and AC while the AC gain is measured with the scope and displayed. The last circuit analyzed is a Push Pull amplifier.

 

This lab will utilize the ZVN3306A and ZVP3306A MOSFETs.

 

Experiment 1: Common Drain (CD) amplifiers

 CD_schematic.JPG

CD NMOS and PMOS amplifiers

 

 Operation

A Common Drain amplifier is DC biased such that the NMOS and PMOS are operating in saturation. Input is supplied through the gateand output is measure at the source. Drain is tied to VDD which in AC is 0v and this is why is is called Common Drain.

Common Drain amplifiers are also called source followers because the gain is often very close to one and no phase shift occurs during amplification thus our input at the gate is almost identical to the output at the source.

 

 Simulations

CD_sims.JPG

 Green: Vin, Red: PMOS Vout, Blue: NMOS Vout

 

 Note: In this lab, we connect the electrolytic capacitor (+) lead to the gate node and the (-) lead to the input node because the gate node has more voltage than the input node. The gate node has a DC offset provided by the voltage divider circuit while the input node has 0v DC with a small AC voltage. 

 

 Input and Output Resistances

 AC_CD_NMOS.JPG     AC_CD_PMOS.JPG      

 CD NMOS Amplifier Input and Output Resistances     CD PMOS Amplifier Input and Output Resistances

 

 Input and output resistance calculation

 CD_NMOS_Input_resistance.JPG         CD_PMOS_Input_resistance.JPG          

NMOS                                                             PMOS

 

 Note: Output resistance includes 1/gmn because 1/gmn is associated with the source node. Also the gmn and gmp value is estimated and not measured.

 

 NMOS Input Resistance                                                                  PMOS Input Resistance

IMG_20150313_094226_219.jpg     IMG_20150313_100904_324.jpg

 

 Gain:

 

 Gain Calculation:

 CD_Gain.JPG       CD_Gain_p.JPG

NMOS                                                                                             PMOS

 

NMOS Gain                                                                                             PMOS Gain

 IMG_20150313_093552_482.jpg          IMG_20150313_100201_721.jpg

 Measured results of the gain, yellow is input, blue is output. As to be expected, it is a gain of 1 and with no phase shift.

 

Table

NMOSCalculated ResultsSimulated ResultsMeasured Results
Input Resistance33.33kN/A33.33k
Output Resistance24.39N/A267.3
Gain0.97560.85810.927

 

PMOSCalculated ResultsSimulated ResultsMeasured Results
Input Resistance33.33kN/A33.33k
Output Resistance90.9N/A180.4
Gain0.910.85880.808

 

 Experiment 2: Common Source CS Amplifiers 

 CS_schematic.JPG

CD NMOS and PMOS amplifiers

 

 Operation

A Common Source amplifier is DC biased such that the NMOS and PMOS are operating in saturation. Input is supplied through the gate and output is measure at the Drain. This amplifer produces high giain due to the parallel resistance at the source node. The output also sees a phase shift of 180 degrees.

 

 Simulations

CS_sims.JPG

 Green: Vin, Red: PMOS Vout, NMOS Vout

 

 Note: In this lab, we connect the electrolytic capacitor (+) lead to the gate node and the (-) lead to the input node because the gate node has more voltage than the input node. The gate node has a DC offset provided by the voltage divider circuit while the input node has 0v DC with a small AC voltage. 

 

 Input and Output Resistances

 AC_CS_NMOS.JPG           AC_CS_PMOS.JPG      

 CS NMOS Amplifier Input and Output Resistances     CS PMOS Amplifier Input and Output Resistances

 

 Input and output resistance calculation

CS_Resistances.JPG

 

Note: Output resistance does not include 1/gmn because 1/gmn is associated with the source node. Also the gmn and gmp value is estimated and not measured. We only include one calculation here because it is the same for NMOS and PMOS.

 

 Gain:

 

 Gain Calculation:

 CS_Gain.JPG      CS_Gain_p.JPG      

 NMOS                                               PMOS

 

NMOS                                                                                                    PMOS

 IMG_20150313_102024_572.jpg     IMG_20150313_105722_448.jpg            

 

Table

NMOSCalculated ResultsSimulated ResultsMeasured Results
Input Resistance33.33kN/A33.33k
Output Resistance1kN/A1k
Gain-8.63-5.33-7.33

 

PMOSCalculated ResultsSimulated ResultsMeasured Results
Input Resistance33.33kN/A33.33k
Output Resistance1kN/A1k
Gain-5.23-6.94-5.25

 

 Experiment 3: Common Drain (CG) amplifiers

 CG_schematic.JPG

CG NMOS and PMOS amplifiers

 

 Operation

A Common Gate amplifier is DC biased such that the NMOS and PMOS are operating in saturation. Input is supplied through the source and output is measure at the drain. The common gate amplifier also sees high gain but this time no phase shift occurs. 

 

 Simulations

CG_sims.JPG

 Green: Vin, Red: PMOS Vout, Blue: NMOS Vout

 

 Note: In this lab, we connect the electrolytic capacitor (+) lead to the gate node and the (-) lead to the input node because the gate node has more voltage than the input node. The gate node has a DC offset provided by the voltage divider circuit while the input node has 0v DC with a small AC voltage. 

 

 Input and Output Resistances

 AC_CG_NMOS.JPG     AC_CG_PMOS.JPG      

 CG NMOS Amplifier Input and Output Resistances     CG PMOS Amplifier Input and Output Resistances

 

 Input and output resistance calculation

 CG_NMOS_resistance.JPG         CG_PMOS_resistance.JPG          

NMOS                                                                              PMOS

 

 Note: Output resistance includes 1/gmn because 1/gmn is associated with the source node. Also the gmn and gmp value is estimated and not measured.

 

 Gain:

 

 Gain Calculation:

 CG_Gain.JPG       CG_Gain_p.JPG

NMOS                                             PMOS

 

NMOS Gain                                                                                             PMOS Gain

 IMG_20150313_103922_330.jpg         IMG_20150313_094226_219.jpg

 

Table

NMOSCalculated ResultsSimulated ResultsMeasured Results
Input Resistance124.4N/A166.5
Output Resistance1kN/A1.325k
Gain8.046.226.5

 

PMOSCalculated ResultsSimulated ResultsMeasured Results
Input Resistance191N/A275
Output Resistance1kN/A1.25k
Gain5.244.775.1

 

 

 Experiment 4: Push-pull Amplifier

 

 Operation:  The push-pull amplifier works as a AB Class amplifier, meaning that different parts of the transistors can be on at a time. Also, the DC operation depends on the inout voltage. For the AB class amplifier, the NMOS and PMOS will be activated at different situations; if the inout voltage is low, the NMOS will turn off and the PMOS will turn on, but if the input voltage is high, the PMOS will turn off and the NMOS will turn on. When the PMOS is on, the amplifier sources current from VDD to Vout and when the NMOS is on, it will sink current from Vout to ground. The circuit is naturally good at sourcing and sinking current bacuase it uses both a PMOS to source and an NMOS to sink current. 

 

 Schematic

 ppa.JPG

 

 Calculations

 ppa_calc.JPG

When R1 = 100k, our simulations clipped too hard to see accurate results so we had to use a 50 ohm resistor to get actual results that we could measure.

 Given our gain calculations, if we replace our 100k resistor with 510k, we expect the gain to increase to 25.5k and we also expect our signal to clip, heavily.

 

Simulations

 ppa_sim.JPG

 R1=100K, Gain=-3780

 

 ppa_sim_2.JPG

 R1=50, Gain=-0.864

 

 Scope

 IMG_20150313_111557_479.jpg

 Gain with R1 = 50

 

 Table

Push-Pull Amplifier Calculated ResultsSimulated ResultsMeasured Results
Gain-2.5-0.864-5