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Circuits, electronics and noise

Transimpedance amplifier output voltage

Output of an ideal transimpedance amplifier whose non-inverting input is held at Vref and whose feedback resistor Rf sets the conversion.

Ref
ELN-30
Rev
v1
Field
Circuits, electronics and noise
Result
Vo [V]

A transimpedance amplifier turns an input current into a voltage. With the non-inverting input at Vref, the inverting node also sits at Vref and the current Ii flows through Rf, so Vo = Vref − Ii Rf. A positive current into the inverting node lowers the output. The gain is Rf in volts per amp, so it is set by one resistor; a small capacitor across Rf is needed to keep a photodiode input stable.

Output of an ideal transimpedance amplifier whose non-inverting input is held at Vref and whose feedback resistor Rf sets the conversion. A positive input current into the inverting node lowers the output.

Calculator

Solve for
V
V
05
A
1e-91e-4
Ω
1,0001e8
  • Transimpedance gain, −Rf−1,000,000 V/A
  • Voltage drop across Rf, Ii Rf2 V
  • Largest current before the output reaches 0 V2.5×10−6 A

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Output voltage (V) current value 0.5 V
RfFeedback resistorKey driver
−1982.5
IiInput current into the inverting node
−97.52.5
VrefReference voltage at the non-inverting input
−23
  • A 2 µA photocurrent through 1,000,000 Ω moves the output 2 V below the 2.5 V reference, to 0.5 V.
  • A larger Rf gives a larger signal and, since its noise rises only with the square root of Rf, a better signal-to-noise ratio.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing (V)Local stepChange in result
Rf Feedback resistor1,000 to 1e8 Ω−197.52.498200+10%−40 %
Ii Input current into the inverting node1e-9 to 1e-4 A−97.52.499100+10%−40 %
Vref Reference voltage at the non-inverting input0 to 5 V−235+10%+50 %

Sweep of Feedback resistor

Feedback resistor (Ω)Output voltage (V)
1,0002.498
4,2172.492
17,7802.464
74,9902.35
316,2001.868
1,334,000−0.167
5,623,000−8.747
2.371e7−44.93
1e8−197.5

Sweep one variable

Output voltage (V)Hover, touch, or use the arrow keys on the chart
−200−150−100−500 100010k100k1M10M100M Feedback resistor (Ω), log scale now 0.5

Variables and how each one contributes

Vo

Output voltage

Result · V

What the equation gives you. Everything else feeds it.

Vref

Reference voltage at the non-inverting input

V · typical 0 to 5

The reference voltage at the non-inverting input, in V. Shifts the output up one for one. Raising it by 10 % (to 2.75) moves the result by +50 %, from 0.5 to 0.75 V.

Ii

Input current into the inverting node

A · typical 1e-9 to 1e-4

The input current into the inverting node, in A. A larger current lowers the output in direct proportion. Raising it by 10 % (to 2.2×10−6) moves the result by −40 %, from 0.5 to 0.3 V.

Rf

Feedback resistor

Ω · typical 1,000 to 1e8

The feedback resistor, in Ω. A larger Rf gives more volts per amp, so the output drops further. Raising it by 10 % (to 1,100,000) moves the result by −40 %, from 0.5 to 0.3 V.

Worked example with the values above

  1. Drop across Rf: Ii Rf = 2×10−6 × 1,000,000 = 2 V.
  2. Subtract from the reference: 2.5 − 2.
  3. Vo = 0.5 V.

Assumptions and limits

  • An ideal op amp with infinite gain and no input current, in its linear range with negative feedback.
  • Output limited only by the supply, and signals within the useful bandwidth.

Common mistakes

  • Forgetting that a current into the inverting node lowers the output.
  • Leaving out a small capacitor across Rf, so the circuit oscillates with a photodiode.
  • Ignoring the bias current and the leakage of the diode.

Statistics and uncertainty

Resistor tolerances set the gain accuracy, so use 1 % parts or better for precision, and a matched network for the difference amplifier, where mismatch converts common-mode voltage into error. Real op amps add offset, bias current and finite gain.

Where it is used

  • Signal mixing, scaling, integration and current-to-voltage conversion in instrumentation.
  • Photodiode, sensor and ramp-generator circuits.

Maths you need

  • Virtual ground: the inverting input sits at the non-inverting voltage
  • Negative feedback: the output acts to cancel the input difference
  • Kirchhoff’s current law: currents at a node add to zero

Related formulas

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