Logarithmic amplifiers are used in a variety of measurement applications to amplify signals that span wide dynamic ranges. For example, logarithmic amplifiers disclosed in U.S. Pat. No. 4,996,500 are coupled to detectors in an automatic level control system to amplify signals from the detectors that span multiple voltage decades. The logarithmic amplifiers provide nonlinear amplification, where the amount of amplification depends on the magnitude of the signals that are applied to the logarithmic amplifiers. Higher amplification is provided to an applied signal that has a lower magnitude, and lower amplification is provided to an applied signal that has a higher magnitude.
A conventional logarithmic amplifier, disclosed in engineering texts such as Analysis and Design of Analog Integrated Circuits, Second Edition, by Gray and Meyer, ISBN 0471-87493-0, page 358, includes a voltage amplifier with the collector and emitter of a bipolar junction transistor coupled in a feedback path between the input and output of the voltage amplifier, as shown in
A logarithmic amplifier according to embodiments of the present invention includes the base and emitter of a bipolar junction transistor coupled in a feedback path between the output and the input of a gain element. When the bipolar junction transistor is a PNP transistor, the logarithmic amplifier can be made compatible with CMOS semiconductor circuitry and processes.
Each of the logarithmic amplifiers 10, 12, 14, 16 also include one or more bipolar junction transistors BJT. The base b and the emitter e of the bipolar junction transistors BJT are coupled in feedback paths of the logarithmic amplifiers 10, 12, 14, 16 between an output and an input of the gain element G. In the example shown, the base b of the bipolar junction transistor BJT is coupled to the inverting input of the gain element G, and the emitter e of the bipolar junction transistor BJT is coupled to the output of the gain element G. In the embodiment of the present invention shown in
In an embodiment of the present invention shown in
In other embodiments of the present invention, shown in
The logarithmic amplifiers 10, 12, 14, 16 typically include a feedback capacitor (not shown) in the feedback path between the output and the input of the gain element G, to maintain stable operation of the logarithmic amplifier over a range of operating conditions. The value of the feedback capacitor can be determined empirically or can be determined analytically, for example based on the gain transfer characteristics of the gain element and the junction capacitances of the bipolar junction transistor BJT.
Equation 1 indicates the transfer characteristic of the logarithmic amplifiers 10, 12, 14, 16 of
VOUT=(kT/q)ln(BIIN/ISAT) (1)
In equation 1, kT/q is the known term VT, which is equal to 26 mV at 300 degrees Kelvin. The term B is the current gain of the bipolar junction transistor BJT, and the term ISAT is the saturation current of the bipolar junction transistor BJT.
To achieve a transfer characteristic that is independent of transistor parameters such as the term B and the term ISAT, a reference logarithmic amplifier LOGREF can be included with the logarithmic amplifiers 10, 12, 14, 16 of
VDIFF=VREF−VOUT=(kT/q)(ln(B1IIN1/ISAT1)−ln(B2IIN2/ISAT2)) (2)
In equation 2, the voltage VREF represents a reference output voltage provided by the reference logarithmic amplifier LOGREF. The term B1 is the current gain of the bipolar junction transistor BJT1, the term B2 is the current gain of the reference bipolar junction transistor BJT2, the term ISAT1 is the saturation current of the bipolar junction transistor BJT1, and the term ISAT2 is the saturation current of the reference bipolar junction transistor BJT2. When the bipolar junction transistor BJT1 and the reference bipolar transistor BJT2 in the differential logarithmic amplifier 20 are integrated or commonly fabricated, or otherwise have matched parameters, the current gains B1 and B2 are approximately equal, and ISAT1 and ISAT2 are approximately equal. Assuming that B1=B2, and that ISAT1=ISAT2, the output voltage VDIFF is independent of these transistor parameters as indicated in equation 3.
VDIFF=VREF−VOUT=(kT/q)ln(IIN1/IIN2) (3)
Because the output voltage VDIFF is proportional to the logarithm of the ratio of the input current IIN1 to the current IIN2, the current IIN2 can be adjusted via RREF or VREF as a reference current that is used to set the gain G of the differential logarithmic amplifier 20. An optionally included input polarity switch SW is shown included in the differential logarithmic amplifier 20 in
Once the reference current IIN2 is set, the gain g of the differential logarithmic amplifier 20 adjusts automatically based on the magnitude of the input current IIN1. This makes the differential logarithmic amplifier 20 well-suited to amplify applied signals over a wide dynamic range. Relatively low-level input currents IIN1 provide high resistance in the feedback path between the output and the input of the gain element, resulting in relatively high gain. Relatively high-level input currents provide low resistance in the feedback path, resulting in relatively low gain.
The nonlinear transfer characteristic of the logarithmic amplifier 20 provides a gain g at a given ratio of currents IIN1/IIN2 that is eqivalent to a gain that can be provided by an amplifier with a variable resistor in the feedback path between the output and the input of the gain element G. However, the performance of the differential logarithmic amplifier 20 is distinguished from an amplifier with a variable resistor in the feedback path. For example, when the differential logarithmic amplifier 20 has a gain g equivalent to that of an amplifier with a 2.512 Mohm resistor in the feedback path, the differential logarithmic amplifier 20 has approximately three times the bandwidth of the resistive amplifier. For example, the differential logarithmic amplifier 20 has a 1 MHz bandwidth, whereas the amplifier with the 2.512 Mohm resistor in the feedback path has a 317 KHz bandwidth. The differential logarithmic amplifier 20 also has a lower noise density, for example 56.6 fA/Hz1/2, than the amplifier with the 2.512 Mohm resistor in the feedback path, which has for example, a noise density of 75 fA/Hz1/2.
While the embodiments of the present invention have been illustrated in detail, it should be apparent that modifications and adaptations to these embodiments may occur to one skilled in the art without departing from the scope of the present invention as set forth in the following claims.