Log amplifiers are used in many ways, such as:

• To perform mathematical operations like multiplication, division and exponentiation. Multiplication is also sometimes called mixing. This is similar to operation of a slide rule, and is used in analog computers, audio synthesis methods, and some measurement instruments (i.e. power as multiplication of current and voltage).
• To calculate the dB value of a given quantity.
• As a True RMS converter.
• Extending dynamic range of other circuits, like automatic gain control of transmit power in RF circuits, or analog-to-digital converters.

The reverse saturation current for the diode doubles for every ten degree Celsius rise in temperature. Similarly the emitter saturation current varies significantly from one transistor to another and also with temperature. Hence, it is very difficult to set the reference voltage for the circuit.^[2]

The relationship between the input voltage ${\displaystyle V_{\text{in}}}$  and the output voltage ${\displaystyle V_{\text{out}}}$  is given by:

${\displaystyle V_{\text{out}}=-V_{\text{T}}\ln \left({\frac {V_{\text{in}}}{I_{\text{S}}\,R}}\right)}$ 

where ${\displaystyle I_{\text{S}}}$  and ${\displaystyle V_{\text{T}}}$  are the saturation current and the thermal voltage of the diode respectively.

The dynamic range of this basic op-amp diode circuit is limited to 40-60 dB because of non-ideal diode characteristics, but the dynamic range can be increased to over 120 dB by replacing the diode with a transistor in a "transdiode" configuration.^[3]

A necessary condition for successful operation of a log amplifier is that the input voltage, V_in, is always positive. This may be ensured by using a rectifier and filter to condition the input signal before applying it to the log amplifier's input. As V_in is positive, V_out is obliged to be negative (since the op amp is in the inverting configuration) and is large enough to forward bias the emitter-base junction of the BJT keeping it in the active mode of operation. Now,

${\displaystyle {\begin{aligned}V_{\text{BE}}&=-V_{\text{out}}\\I_{\text{C}}&=I_{\text{S}}\left(e^{\frac {V_{\text{BE}}}{V_{\text{T}}}}-1\right)\approx I_{\text{S}}e^{\frac {V_{\text{BE}}}{V_{\text{T}}}}\\\Rightarrow V_{\text{BE}}&=V_{\text{T}}\ln \left({\frac {I_{\text{C}}}{I_{\text{S}}}}\right)\end{aligned}}}$ 

where ${\displaystyle I_{\text{S}}\,}$  is the saturation current of the emitter-base diode and ${\displaystyle V_{\text{T}}\,}$  is the thermal voltage. Due to the virtual ground at the op amp differential input,

${\displaystyle I_{\text{C}}={\frac {V_{\text{in}}}{R}}}$ , and

${\displaystyle V_{\text{out}}=-V_{\text{T}}\ln \left({\frac {V_{\text{in}}}{I_{\text{S}}R}}\right)}$ 

The output voltage is expressed as the natural log of the input voltage. Both the saturation current ${\displaystyle I_{\text{S}}\,}$  and the thermal voltage ${\displaystyle V_{\text{T}}\,}$  are temperature dependent, hence, temperature compensating circuits may be required.

• Diode
• Operational amplifier applications § Logarithmic output

• Integrated DC logarithmic amplifiers from Maxim's AN 36211
• Analog electronics with Op Amps by A. J. Peyton, V. Walsh