Log amplifier explained

A log amplifier, also known as logarithmic amplifier or logarithm amplifier or log amp, is an amplifier for which the output voltage Vout is K times the natural log of the input voltage Vin. This can be expressed as,

Vout=Kln\left(

Vin
Vref

\right)

where Vref is the normalization constant in volts and K is the scale factor.

The log amplifier gives an output voltage which is proportional to the logarithm of the applied input voltage.To design a log amplifier circuit, high performance op-amps like LM1458, LM771, LM714 are commonly used and a compensated log amplifier may include more than one. In some situations, especially in RF domain, monolithic log amplifiers are also used to reduce number of components and space used, as well improve bandwidth and noise performance.

The log amplifier's operation can be inverted by an exponentiator, such as an op-amp configured for exponential output.[1]

Log amplifier applications

Log amplifiers are used in many ways, such as:

Drawbacks of basic log amplifier configuration

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]

Basic op-amp diode circuit

The relationship between the input voltage

Vin

and the output voltage

Vout

is given by:

Vout=-VTln\left(

Vin
ISR

\right)

where

IS

and

VT

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]

Transdiode configuration

A necessary condition for successful operation of a log amplifier is that the input voltage, Vin, 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 Vin is positive, Vout 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,

\begin{align} VBE&=-Vout\\ IC&=

VBE
VT
I
S\left(e

-1\right)IS

VBE
VT
e

\\ VBE&=VTln\left(

IC
IS

\right) \end{align}

where

IS

is the saturation current of the emitter-base diode and

VT

is the thermal voltage. Due to the virtual ground at the op amp differential input,

IC=

Vin
R
, and

Vout=-VTln\left(

Vin
ISR

\right)

The output voltage is expressed as the natural log of the input voltage. Both the saturation current

IS

and the thermal voltage

VT

are temperature dependent, hence, temperature compensating circuits may be required.

See also

External links

Notes and References

  1. Web site: 2013 . AN-311 Theory and Applications of Logarithmic Amplifiers . live . https://web.archive.org/web/20240619045645/https://www.ti.com/lit/an/snoa575b/snoa575b.pdf . 2024-06-19 . 2024-07-30 . Texas Instruments. }
  2. https://www.analog.com/media/en/reference-design-documentation/design-notes/dn288f.pdf RMS-to-DC Conversion Just Got Easy
  3. Web site: 2009 . MT-077 Tutorial: Log Amp Basics . live . https://web.archive.org/web/20221029071227/https://www.analog.com/media/en/training-seminars/tutorials/MT-077.pdf . 2022-10-29 . 2023-06-28 . Analog Devices.