The present disclosure relates to reference voltage generators and, more particularly, to a generator of a voltage variable with temperature to a bandgap voltage generator and to a related method of generating a temperature compensated bandgap voltage.
Most electronic circuits may require a stable direct current (DC) voltage reference, particularly with regard to fluctuations of working temperature for the circuits. Usually, such stable voltage reference circuits are bandgap voltage generators that are based upon the property of a bipolar transistor to produce a base-emitter voltage with well known temperature dependence.
According to a theoretical analysis in the article: Yannys P. Tsividis, “Accurate analysis of temperature effects in IC-VBE characteristics with application to bandgap reference sources”, IEEE Journal of solid-state circuits, Vol. SC-15, No. 6, December 1980, pages 1076-1084, the following equation holds:
where VBE is the base-emitter voltage, VBG0 is the bandgap voltage expected at a null temperature, TREF is a reference temperature, α is a coefficient, and VT is the voltage equivalent of temperature. The following equation holds for VT:
Neglecting the (generally) small term α·VT·ln(T/TREF), VBE voltage is complementary to the absolute temperature (CTAT). In literature, two main classes of bandgap generators are disclosed:
In known bandgap voltage reference generators, for example, the generator disclosed in U.S. Pat. No. 4,249,122 to Widlar, a pair of transistors are operated at different current densities and are coupled to generate a voltage that is proportional to the difference between the base-emitter voltages of the two transistors. This difference voltage has a positive temperature coefficient, i.e. the difference voltage is proportional to the absolute temperature (PTAT) of the circuit. The PTAT voltage provided by the difference in the base-emitter voltages is properly scaled and summed with the complementary to absolute temperature voltage of one of the transistors to generate a stable bandgap voltage reference.
In first-order bandgap compensation, the first derivative of the base-emitter voltage with respect to temperature is nullified in correspondence to a reference temperature TREF, as shown in
In widely diffused second order bandgap voltage generators, a voltage proportional to the square absolute temperature (PSTAT) is used to compensate the second order term of the Taylor expansion of a α·VT·ln(T/TREF), such to nullify at the reference temperature TREF the first derivative and the second derivative of the output voltage VOUT with respect to the absolute temperature, obtaining a voltage-temperature characteristic as shown by way of example in
In other second order bandgap voltage generators, a nonlinear current is generated. This current is proportional to T*ln(T/Tref) and it is added to compensate for the term α·VT·ln(T/TREF). An exemplary architecture implementing such a second order bandgap compensation is shown in
Even if voltage fluctuations with temperature are limited in a smaller range than that of first-order bandgap voltage generators, these architectures may be complicated to realize and/or cannot accurately and independently adjust the PTAT and logarithmic terms. In other words, the generated bandgap voltage, after the trimming procedure, may vary greatly in temperature ranges from −40° C. up to 150° C.
According to a method for having a stable bandgap voltage, it may be necessary to realize a generator of a voltage that varies logarithmically with the working absolute temperature, exactly as the logarithmic addend in equation (1), then to add such a logarithmically varying voltage with a first-order bandgap voltage.
Studies carried out show that it is possible to realize a generator of a voltage that varies logarithmically with temperature using a simple architecture, based on a typical differential amplifier, that may be used at the same time also as an adder.
More precisely, according to this disclosure, a generator of a voltage logarithmically variable with temperature may comprise a differential amplifier comprising a pair of transistors (Q1, Q2), i.e. first (Q1) and second (Q2), each coupled with a respective bias network adapted to bias in a conduction state the transistors first (Q1) and second (Q2) respectively with a constant current and with a current proportional to the working absolute temperature. The pair of transistors (Q1, Q2) may be adapted to generate between its control nodes the voltage logarithmically variable with temperature, a common bias current generator (IBIAS) coupled between the common terminal of the differential pair of transistors (Q1, Q2) and a node at a reference potential, and a feedback line adapted to constitute a free-wheeling path for the current difference between the common bias current (IBIAS) and the sum of the currents flowing through the transistors of the differential pair (Q1, Q2).
This architecture may be used as the input stage of an operational amplifier, or as an operational amplifier, for adding the logarithmically variable voltage with a first-order bandgap voltage, without requiring further active components. This approach may allow for independently and accurately adjusting, by trimming procedures, the PTAT and logarithmic terms, in order to get the maximum achievable accuracy.
The disclosed generator of a voltage logarithmically variable with temperature may be used for realizing a bandgap voltage generator. A particularly effective trimming sequence of the herein proposed voltage generator is disclosed.
a depicts a generator of a voltage logarithmically variable with temperature, according to the present invention.
b is an operational amplifier comprising the generator of
The term that compensates for the logarithmic addend in equation (1) is generated with a logarithmic voltage generator, an embodiment of which is shown in
The currents Iconstant and IPTAT, together with the bias current generator IBIAS, force the two transistors Q1 and Q2 of the differential pair into a conduction state. The feedback line, that in the shown example is a MOS controlled in a conduction state by the voltage on the current terminal of Q1 not in common with the transistor Q2, provides a free-wheeling path to the currents entering in the common node of the two transistors Q1 and Q2.
The transistors Q1 and Q2 are matched, thus the voltage difference between their control terminals is proportional to the product of the voltage equivalent of temperature by the natural logarithm of the ratio of the collector currents flowing therethrough. Therefore, the architecture of
It is thus possible to realize a bandgap voltage generator of a voltage substantially independent from temperature in a broad range of temperature variation by adding the voltage generated by any first-order bandgap generator with an adjusted replica of the logarithmically varying voltage available between the control nodes of the differential pair of transistors.
According to an aspect of this disclosure, an adder adapted for performing this sum may be realized using the same differential pair of transistors as an operational amplifier or as the input stage of an operational amplifier, as depicted in
Of course, it is possible to connect the resistive voltage divider between the output and the non-inverting input of the operational amplifier and to connect the middle node of the voltage divider to the inverting input. The voltage generated by the operational amplifier Vref is the sum of the voltage applied on the first input node of the operational amplifier and an amplified replica of the voltage difference between the two input nodes of the operational amplifier. Therefore, if the input nodes of the operational amplifier of
A circuit scheme of a logarithmically compensated bandgap voltage generator is shown in
In the example of
A constant current generator, that may realized for example using the bandgap voltage VBG, generates a constant current ICONSTANT that is mirrored to bias the other transistor of the differential pair of transistors of
The disclosed embodiment of
According to the disclosed procedure, the first-order bandgap generator (in the shown example, the resistor R2) is trimmed at a first temperature in order to make the voltage VBG equal to a target voltage VBG0. In some embodiments, the first temperature is conveniently chosen in the middle of the operating temperature range.
At the same temperature, a second trimming step may be performed. This second trimming step is aimed to adjust one of the two currents biasing the logarithmic voltage generator by adjusting the mirror ratio of the current mirror Q5, Q6. As shown in
As an alternative, it is possible to execute the second trimming step for adjusting the current IPTAT instead of the current ICONSTANT. At a second temperature, the ratio RA/RB may be trimmed to obtain an output VREF voltage equal to the target VBG0. This third trimming step allows for adjusting the logarithmic voltage contribution independently from PTAT voltage contribution. In some embodiments, the third trimming step may be conveniently chosen at one of the end values of the operating temperature range.
Differently from typical bandgap voltage generators, the disclosed architecture may have a reduced number of components and may be realized using any first-order bandgap voltage generator and any constant current generator. Conveniently, the constant current generator may be obtained using the same bandgap voltage made available by the first-order generator, though any constant current generator may be used.
Optionally, the resistive voltage divider RA, RB may be realized as a series of resistors of small value, as shown in
A simulation voltage-temperature characteristic of the bandgap voltage generator is depicted in
Number | Date | Country | Kind |
---|---|---|---|
MI2011A000584 | Apr 2011 | IT | national |