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OPA320: A question about the "1 MHz, Single-Supply, Photodiode Amplifier Reference Design"

Part Number: OPA320

Hi all, 

I am reading the "1 MHz, Single-Supply, Photodiode Amplifier Reference Design" application note and have a question about the pole mentioned on Page 5. Why the R in parallel with C gives a pole of 1/2pi*C*R? 

Thanks.

Transimpedance amplifier_TI.pdf

  • Hi B,

    below this frequency the parallel circuit of C1 and R1 looks mainly like a resistor (R1) and above this frequency this parallel circuit looks mainly like a capacitor (C1).

    A pole is only a certain position in the Bode plot, where something happens. No rocket science...

    Kai
  • Thanks Kai,

    I have figured out. There is a Cj in sereis with R1 // C1 and if you write the transfer function, there is a pole at 1/2piR1C1.

    Thanks
  • Ah, now I see what you mean. But I think you don't need Cj. It's enough to take the photocurrent source into consideration. Then the pole exists even without any Cj.

    Kai
  • Hi Kai,

    Just for clarification, you should always account for the photodiode capacitance (Cj). The interaction of the feedback resistance with the parallel combination of your photodiode capacitance and op-amp input capacitance creates a zero in the feedback network (technically 1/beta). This is the real reason why C1 is added, because without it your transimpedance amplifier will very likely be unstable. Effectively Cj places a limit on the maximum bandwidth you can get out of the circuit, and consequently on the minimum value of C1 you can use and still keep the op-amp stable.

    Also, Go Green!

  • Dear Zak,

    I'm sorry if my bad english lead to confusion. It was never my intention to suggest that Cj can be neglected in the design of a TIA. I only wanted to mention, that for the calculation of the pole R1 // C1 no other component in the equivalent circuit is necessary. Anyway... I know, of course, that Cj leads to a phase lag and that this phase lag would erode the phase margin of operational amplifier. A phase lead capacitance C1 is needed to recover the phase margin, at least partially.

    From my experience I know, that for very high detector capacitances this phase lead compensation can be unsatisfactory, sometimes, especially if R1 is in the kOhm range...

    Kai
  • Hi Kai,

    Why only R1//C1 can give a pole. My comprehension is only R in series with C can give you a pole from the transfer function.

    Thanks,
  •  Hi Zak,

    Do you happen to know how the equation 9 was derived?  where can I find the theory of using 1/beta line to determine the stability?

    Thanks, Go White!

    Bin

  • Bin,

    Please watch the video series under TI Precision Labs covering the topic of stability - see link below:

  • Hi B,

    you wrote: "Why only R1//C1 can give a pole. My comprehension is only R in series with C can give you a pole from the transfer function."

    Maybe this video helps:

    www.youtube.com/watch

    Kai
  • Hi Marek, 

    Thank you very much for your suggestion. I have studied the material you mentioned but still could not figure out why "in the region above the pole, the frequency of intersection is fI = (C1/Cin+C1)fGBW.

    Bin

  • Hi Bin,

    equation 9 is just taken out of figure 6 of the application note you refer to:

    The blue graph is 1/beta = (Cin + C1)/C1. The red graph is a line with the slope of -20db/decade, which crosses the 0dB line at fGBW. And the point of intersection of the blue and red graph is just at

    fi = C1/(Cin +C1) x fGBW

    An example: If 1/beta is 20dB, then the intersection point is one decade under fGBW. If 1/beta is 40dB, then the intersection point is two decades under fGBW.

    Kai