1. Field of the Invention
This invention relates to current sources, and particularly to current sources capable of providing a second current in a constant ratio to a first current.
2. Description of the Related Art
There are many circuit applications in which a second current is needed which is in a constant ratio to a first current. Circuits which provide currents that compensate for the base currents of a differential input stage typically require the generation of a second current that varies with the input stage's tail current. If the second current closely tracks the tail current, it can be used to provide compensation currents which substantially reduce the stage's input currents.
Difficulties can arise when there is a differential voltage between the first and second current sources. For example, one way in which ratioed currents can be generated is shown in
where Vdiff is the differential voltage between the two collectors, and VA is the Early voltage. As the current ratio varies significantly with Vdiff, this approach is unacceptable for many applications in the differential voltage is likely to vary.
The performance of the circuit of
where Vdeg is the voltage across the degeneration resistors. Here, the variation of the current ratio with Vdiff is significantly reduced, but the addition of Ra and Rb results in the circuit requiring additional headroom.
Another way to improve the performance of the circuit of
This approach also reduces the variation of current ratio with Vdiff, but at the expense of additional headroom and an extra bias voltage generator.
A basic current mirror can also be used to generate a second current which is proportional to a first current. However, since the output impedance of each mirror transistor is proportional to its Early voltage divided by its collector current, the mirror's output impedance will be low—causing the current ratio to vary significantly with Vdiff. This can be improved by adding emitter degeneration resistors Ra and Rb as shown in
Another way to improve the performance of the current mirror of
A constant ratio current source is presented which overcomes the problems noted above, providing a current ratio which is nearly constant with differential voltage, without requiring extra headroom.
The present constant ratio current source comprises a first current branch which includes a first transistor that conducts a current I1 from a first current input to a first node and a resistor R1 connected between the first node and a circuit common point, and a second current branch which includes a second transistor that conducts a current I2 from a second current input to a second node and a resistor R2 connected between the second node and the circuit common point. The first and second current branches are arranged such that current I2 varies with current I1. The current source also requires a linear negative resistance circuit connected between the first and second nodes, which provides an apparent negative resistance that increases the differential output impedance at the first and second current inputs such that the ratio of I2:I1 is maintained approximately constant for a varying differential voltage applied across the first and second current inputs.
The present current source is easily configured to provide a nearly constant I2:I1 ratio of 1:1, or ratios other than 1:1. The current source is useful in many applications, such as a bias current compensation circuit as discussed above.
Further features and advantages of the invention will be apparent to those skilled in the art from the following detailed description, taken together with the accompanying drawings.
a-1e are schematic diagrams of known current sources.
The basic principles of a constant ratio current source per the present invention are illustrated in
The current source also includes a linear negative resistance circuit 34 connected between nodes 24 and 30. The linear negative resistance provides an apparent negative resistance, which acts to increase the effective resistance of emitter resistors R1 and R2, and thereby increase the current source's output impedance, such that the variation of the I2:I1 ratio with differential voltage that would occur in the absence of linear negative resistance circuit 34 is reduced. Furthermore, the negative resistance circuit is arranged such that its apparent negative resistance varies linearly with the difference voltage between nodes 24 and 30. This enables the ratio of I2:I1 to be maintained approximately constant for a varying differential voltage (Vdiff) applied across first and second current inputs 22 and 24, without requiring any additional headroom.
Linear negative resistance circuit 34 could be implemented in many different ways; one possible embodiment is shown in
When so arranged, cross-coupled transistors Q3 and Q4 respond to changes in Vdiff by dividing bias current I3 between Q3 and Q4 to produce a differential correction current (Icorr) that maintains the ratio of I2:I1 approximately constant.
In one embodiment, a diode-connected transistor Q5 is connected in series between Q3 and node 24, and a diode-connected transistor Q6 is connected in series between Q4 and node 30. Resistance circuit 40 comprises a resistor R3 connected between the emitter of Q3 and current source 42, and a resistor R4 connected between the emitter of Q4 and current source 42. When R1=R2=R3=R4=R, and neglecting base currents:
Ic(Q3)=Ic(Q5) (Eq. 1)
Ic(Q4)=Ic(Q6) (Eq. 2)
Vbe(Q3)=Vbe(Q5) (Eq. 3)
Vbe(Q4)=Vbe(Q6) (Eq. 4)
where Ic refers to collector current flowing through a particular transistor and Vbe refers to the base-emitter voltage of a particular transistor.
The voltages at the emitters of transistors Q3 and Q4 are given by:
Ve(Q3)=V30−Vbe(Q6)−Vbe(Q3) (Eq. 5)
and
Ve(Q4)=V24−Vbe(Q5)−Vbe(Q4) (Eq. 6)
where V30 and V24 are the voltages at nodes 30 and 24, respectively.
The voltage across emitter resistor R3 (Ve(Q3)) and emitter resistor R4 (Ve(Q4)) is found by subtracting equation 5 from equation 6 and substituting the relationships in equations 1-4, such that:
Ve(Q4)−Ve(Q3)=V24−V30 (Eq. 7)
Thus, the polarity of the differential voltage Ve(Q4)−Ve(Q3) has been effectively reversed, so that viewed from nodes 24 and 30 the resistance of negative resistance circuit 34 appears to be −2R.
The total differential current in negative resistance circuit 34 is characterized by:
Substituting equation 7 and solving for Icorr gives:
where Icorr is the correction current produced by linear negative resistance 34, which is added to I2 and subtracted from I1 as needed to maintain the ratio of I2:I1 approximately constant.
Bias current I3 reduces the magnitude of values of I1 and I2, and can potentially create an error in these currents. However, this error can be compensated for by adjusting the value of bias voltage BIAS such that I1 and I2 are increased by an amount equal to the magnitude of I3. The magnitude of I3 should not be so large as to require a substantial increase in BIAS, as this increases the circuit's power consumption. However, if I3 is too small, transistors Q1 and Q2 may be cut off. I3 should be selected such that
where (V24−V30)max is the maximum possible difference voltage between nodes 24 and 30.
Another possible embodiment of a constant ratio current source in accordance with the present invention is shown in
When the ratio of I1 to I2 is to be 1:1 and the linear negative resistance circuit is implemented as shown in
However, using unequal resistors in this way also gives rise to an error in the I1:I2 ratio due to Q3 and Q4 having unequal base currents. This error can be compensated for by adding a resistor (R5) to the base circuit of Q6, and/or to the base circuit of Q3 (R6), as shown in
If a resistor R6 is also added, it should be sized such that:
Adding these resistors will equalize the base currents of Q3 and Q4, and thereby substantially reduce the error that might otherwise arise when I1≠I2. The formulas above assume that R3 and R4 are large, and that I2>I1.
One possible application of a constant ratio current source as described herein is in a bias current compensation circuit for a differential amplifier; one possible embodiment is shown in
where βQ7 and βQ8 are the beta values for Q7 and Q8, respectively.
Ideally, the net currents into base terminals 50 and 52 are zero. One way of accomplishing this is to replicate tail current I1, and to mirror the replicated current back to base terminals 50 and 52 as needed to compensate for the base currents. A constant ratio current source per the present invention is suitably employed to replicate the tail current. Thus, in
The bias current compensation circuit also includes a current mirroring circuit 58, which receives I2 and is arranged to provide first and second output currents 60 and 62 to the bases of Q7 and Q8, respectively. Current mirroring circuit 58 could be implemented in numerous ways; when arranged as shown in
at their respective emitters. Then, assuming βQ7=βQ8=βQ9, if
the net currents into base terminals 50 and 52 will be approximately zero, as long as the ratio of I1 and I2 remain approximately constant as provided by the present constant ratio current source.
Note that the bias current compensation circuit implementation shown in
While particular embodiments of the invention have been shown and described, numerous variations and alternate embodiments will occur to those skilled in the art. Accordingly, it is intended that the invention be limited only in terms of the appended claims.
| Number | Name | Date | Kind |
|---|---|---|---|
| 4769617 | Mizuide | Sep 1988 | A |
| 4904952 | Tanimoto | Feb 1990 | A |
| 5587689 | Bowers | Dec 1996 | A |
| 6229394 | Harvey | May 2001 | B1 |
| 6667654 | Behzad et al. | Dec 2003 | B2 |
| Number | Date | Country | |
|---|---|---|---|
| 20080042732 A1 | Feb 2008 | US |