Still open simple question, which circuit are you simulating?
The TI paper doesn't specifically address input impedance at > 10 MHz. It will be obviously affected by input stage common and differential mode bandwidth and gate/base bulk resistances.
1. Seeing a phase of +90° for a capacitiv impedance seems to indicate wrong measurement polarity.
As the stimulus is a current, I think this is ok for a purely capacitive impedance. The (parallel) resistive input impedance could only be seen at much lower frequencies, I'd think.
The voltage across the capacitor will lag the current, in other words should show a phase of -90 degree.As the stimulus is a current, I think this is ok for a purely capacitive impedance.
Yes.The (parallel) resistive input impedance could only be seen at much lower frequencies, I'd think.
As said in post #2, it's obvious that the simulated OP shown th eimpedance plot in post #1 can't be represented by a parallel RC circuit in post #5.
You still didn't tell what's the actually simulated circuit. (e.g. a transistor level OP model with MOS or BJTinput stage, an OP macro model,....).
The voltage across the capacitor will lag the current, in other words should show a phase of -90 degree.
Yes.
In this case, input impedances as shown in post #1 are expectable. You see purely capacitive behaviour up to 100 kHz and almost up to 1 MHz. Above this frequency, various transistor impedances become effective.I am simulating a CMOS current mirror OTA with all MOS transistors. I am simulating with the transistor level.
Mr. erikl
I think you want to say at higher frequency, because at low frequency the resistance is very high and it is approxiametly open circuit.
Yes, you are right. So the polarity must be exchanged, as you told in post #2.The voltage across the capacitor will lag the current, in other words should show a phase of -90 degree.
Yes, I know. The parallel RC circuit is an appropriate equivalent circuit for a real OP, but not in the MHz frequency range. To model an impedance changing from pure capacitive to towards resistive with increasing frequency, you'll need a series RC circuit. But that's only the first order approximation. More circuit elements are required to represent the impedance characteristics shown in post #1.As you see, the response is different from my first assumption (the input resistance and capacitance of the op-amp are in parallel as given in Texaxs Instruments document). it mean that the resistance and capacitance are not actually in parallel.
Yes, I know. The parallel RC circuit is an appropriate equivalent circuit for a real OP, but not in the MHz frequency range. To model an impedance changing from pure capacitive to towards resistive with increasing frequency, you'll need a series RC circuit. But that's only the first order approximation. More circuit elements are required to represent the impedance characteristics shown in post #1.
I'm not sure what you want to achieve. Your simulation "measurements" are showing diffential and single ende input capacitances of 0.8 respectively 8 pF. There will be in principle a parallel resistance, but it's not visible in the shown frequency range because Rp is apparently > 1e12 ohm. So the parallel RC circuit simplifies to C only for the 1 Hz to 100 kHz range.
You can try to find empirical equivalent circuits for the > 100 kHz frequency range, but I don't believe that it would be of much practical interest. If you want it though, a RC ladder network can be tuned to match an empirical impedance characteristic in the 0 to -90 degree range.
I see that this input capacitance is really large, do you think so or it is common in CMOS op-amp
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