MOSFET amplifier input resistance

In summary, the author found that by calculating input resistance, they mean "real part of input impedance." They also found an example where input resistance is infinity with the input capacitor in series with the input. Finally, they found an example where input resistance is found by solving a circuit.
  • #1
etf
179
2
Hi!
My task is to calculate input resistance for circuit below:

original.jpg

VDD=10V, Vtn=1V, β=1mA/V^2, VA=100V, load resistance RL=20k.

Here is model for AC analysis (DC source and infinite capacitances are short circuits, current directions chosen arbitrarily):

kokol.jpg


After calculationg input current iin, I found input resistance Rin=vin/iin=1/((1/RL+1/RD)*(1/rds+gm)/(1/RL+1/RD+1/rds)+1/Rs).

Here is solution from my book: Rin=(rds+RD)*RS/(rds+RD+(1+gm*rds)*RS). I double checked my result and it's correct.I simulated circuit in Multisim and value for input resistance I got matches with value I got by hand. What's wrong? Any idea? :)
 
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  • #2
We can see in solution from book there is no RL included in input resistance. If I remove RL from my model and analyse that circuit then I got result from book but question is, why should I remove RL?
 
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  • #3
Because they asked for input RESISTANCE. The infinite decoupling capacitor to R_L gets rid of R_L in the gain calculation. Had they asked for input IMPEDANCE you would have been right.

Actually, an uncharged "infinite" capacitor WOULDbe a short. They really meant a "large" capacitor I believe.
 
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  • #4
So for example if there is resistor in series with vin it will be also removed when calculating input or output resistance?
 
  • #5
etf said:
So for example if there is resistor in series with vin it will be also removed when calculating input or output resistance?

Whoops. EDIT:

Actually, input resistance is infinite with the input capacitor in series with the input!

You need to have "input resistance" better defined for you. Are you sure they didn't mean "real part of input impedance"? In which case you'd be right, R_L would have to be included. And so would any resistance in series with the input.

So either they mean 'resistance' in which case Rin = infinity with or without any added resistance, or they mean 'real part of input impedance' in which case any input resistor would have to be added to the real part of input impedance.

Since they said both capacitors are infinite I think your original answer is correct (i.e. include R_L).
 
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  • #6
When I studied amplifiers like this in third year I started off being really confused as how to calculate input and out put resistances.
Then later on in the course the professor pointed out to us that there are pretty much static formulas for the different amplifier types (Common Base, Collector, Emitter), I'd look into those and learning them.

On our final exam I pissed off a few friends on the amplifier input resistance question. It was a nasty chain of 3 amp's, it too my buddies a page and a half of calculations to get the answer where I used the formulas and arrived at same result with a few lines :)
 
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  • #7
etf said:
We can see in solution from book there is no RL included in input resistance. If I remove RL from my model and analyse that circuit then I got result from book but question is, why should I remove RL?
Most likely they are including RL within their RD. It's a common dodge to simplify the number of terms in the maths. You appreciate that the pair are effectively in parallel?
 
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  • #8
rude man said:
Are you sure they didn't mean "real part of input impedance"?
They always do mean that.
 
  • #9
rude man said:
Are you sure they didn't mean "real part of input impedance"? In which case you'd be right, R_L would have to be included. And so would any resistance in series with the input.
NascentOxygen said:
They always do mean that.
NascentOxygen said:
Most likely they are including RL within their RD. It's a common dodge to simplify the number of terms in the maths. You appreciate that the pair are effectively in parallel?


So we conclude that by "input resistance" they mean "real part of input impendance" and my original calculations are ok?

Here is another example from my book, now there is resistance in series with vin and Rout has to be found:
R1=100kΩ, R2=47kΩ, RD=3.3kΩ, VDD=5V, Vtn=1.2V, β=1mA/V^2, internal generator resistance Rg=1kΩ, load resistance RL=10kΩ, VA=50V.

semaaa.jpg


Here is solution from book:

grdghdfdh.jpg


R12=R1*R2/(R1+R2)

Rout=Vtest/itest=rDS*RD/(rDS+RD)=3.203kΩ.
Here we can see that input voltage vin is shorted (it's ok, when calculating output (or input) resistance we short all independant voltage sources and remove independant current sources), capacitor acts like a short and internal source resistance is also shorted.
So according to these examples, general conclusion would be:
When calculating output resistance, (real part of output impendance), input voltage should be shorted altogether with it's internal resistance (if it has internal resistance), load resistance should be removed and in place it was we put test voltage, solve circuit and find Rout as vtest/itest.
Do you agree? :)
 
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  • #10
Delete me. I am too rusty.
 
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  • #11
NascentOxygen said:
They always do mean that.

No.

Tale a series R-C network. The dc resistance is infinite (try it with your DVM).
The real part of impedance is R.
Any real capacitor is not infinite so sooner or later it gets charged up.

Another example: a 'scope input might be described as Rin = 1Meg, Cin = 10 pF. The 1 Meg is the input resistance, as measured by a DVM. The R and C are in parallel, not in series. So we have
input resistance = R
real part of input impedance = R/(1 + w^2 R^2 C^2).
 
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  • #12
cpscdave said:
When I studied amplifiers like this in third year I started off being really confused as how to calculate input and out put resistances.
Then later on in the course the professor pointed out to us that there are pretty much static formulas for the different amplifier types (Common Base, Collector, Emitter), I'd look into those and learning them.

On our final exam I pissed off a few friends on the amplifier input resistance question. It was a nasty chain of 3 amp's, it too my buddies a page and a half of calculations to get the answer where I used the formulas and arrived at same result with a few lines :)

It pays to know how to play the game! (Later, in your career, you'll know what to solve for since there isn't anyone to tell you what to find per their definitions.)
 
  • #13
etf said:
So we conclude that by "input resistance" they mean "real part of input impendance" and my original calculations are ok?

Here is another example from my book, now there is resistance in series with vin and Rout has to be found:
R1=100kΩ, R2=47kΩ, RD=3.3kΩ, VDD=5V, Vtn=1.2V, β=1mA/V^2, internal generator resistance Rg=1kΩ, load resistance RL=10kΩ, VA=50V.

https://www.physicsforums.com/attachments/70588

Here is solution from book:

https://www.physicsforums.com/attachments/70589

R12=R1*R2/(R1+R2)

Rout=Vtest/itest=rDS*RD/(rDS+RD)=3.203kΩ.
Here we can see that input voltage vin is shorted (it's ok, when calculating output (or input) resistance we short all independant voltage sources and remove independant current sources), capacitor acts like a short and internal source resistance is also shorted.
So according to these examples, general conclusion would be:
When calculating output resistance, (real part of output impendance), input voltage should be shorted altogether with it's internal resistance (if it has internal resistance), load resistance should be removed and in place it was we put test voltage, solve circuit and find Rout as vtest/itest.
Do you agree? :)

Well, I don't see the correspondence between the circuit and its equivalent circuit. At all! Different connections, different values, etc. ...

I agree with what you wrote though. I still think the word 'resistance' is misplaced, but if 'real part of impedance' is understood then that's fine.

If the input is via the gate, remember that the input impedance at the gate is infinite. So it doesn't matter if there is input resistance in series with the input, the gate is always at zero potential. Nice thing about MOSFETs!
 
  • #14
It was my fault, I draw it wrong! I will correct it.
 
  • #15
NascentOxygen said:
They always do mean that.

rude man said:
No.

Tale a series R-C network.
The subject under discussion in this thread is the capacitor-coupled amplifier. An unqualified statement relating to input resistance is synonymous with midband input impedance. Always.

I'm not dismissing your examples; in appropriate threads they may be helpful. But in this amplifier thread a tale about a passive circuit is at best tangential.
 
  • #16
etf said:
So we conclude that by "input resistance" they mean "real part of input impendance" and my original calculations are ok?
I wouldn't even put it that way. The unqualified term "input resistance" when applied to general amplifiers can be taken as meaning the input resistance where all capacitors are doing what is intended.

That is, conditions where coupling capacitors are coupling to perfection, bypass-capacitors are bypassing dazzlingly well, and any frequency-response shaping capacitors are shaping up spectacularly to their appointed task. These conditions are often referred to as the midband, so you have terms such as midband gain, and midband input and output resistance/impedance, etc. (It is not the same as considering the components to be ideal.)
 

Related to MOSFET amplifier input resistance

1. What is the definition of input resistance in a MOSFET amplifier?

The input resistance of a MOSFET amplifier refers to the resistance seen at the input terminal, looking into the amplifier from the input source. It is a measure of how easily the amplifier can accept a signal from the input source.

2. How is input resistance calculated for a MOSFET amplifier?

The input resistance of a MOSFET amplifier can be calculated using the formula Rin = Vgs/Iin, where Vgs is the voltage at the gate terminal and Iin is the current flowing into the input terminal. This formula is derived from Ohm's law.

3. What factors affect the input resistance of a MOSFET amplifier?

The input resistance of a MOSFET amplifier is affected by the transconductance (gm) of the MOSFET, the biasing network, and the source resistance. The transconductance is a measure of how much the output current changes in response to a change in the input voltage. A higher transconductance will result in a lower input resistance. The biasing network and source resistance also contribute to the overall input resistance.

4. How does input resistance impact the performance of a MOSFET amplifier?

The input resistance of a MOSFET amplifier affects the gain and bandwidth of the amplifier. A lower input resistance can result in a higher gain, but it may also decrease the bandwidth of the amplifier. On the other hand, a higher input resistance can result in a lower gain and a wider bandwidth.

5. What are some practical ways to increase the input resistance of a MOSFET amplifier?

One way to increase the input resistance of a MOSFET amplifier is to use a cascode configuration, where two MOSFETs are connected in series. Another way is to use a bootstrapping circuit, where the source resistor is bypassed with a capacitor. Additionally, increasing the biasing network resistance and using a MOSFET with a higher transconductance can also increase the input resistance.

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