US20020021175A1 - Transconductance amplifier based precision half wave and full wave rectifier circuit - Google Patents
Transconductance amplifier based precision half wave and full wave rectifier circuit Download PDFInfo
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- US20020021175A1 US20020021175A1 US09/901,260 US90126001A US2002021175A1 US 20020021175 A1 US20020021175 A1 US 20020021175A1 US 90126001 A US90126001 A US 90126001A US 2002021175 A1 US2002021175 A1 US 2002021175A1
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F3/00—Amplifiers with only discharge tubes or only semiconductor devices as amplifying elements
- H03F3/30—Single-ended push-pull [SEPP] amplifiers; Phase-splitters therefor
- H03F3/3066—Single-ended push-pull [SEPP] amplifiers; Phase-splitters therefor the collectors of complementary power transistors being connected to the output
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- the present invention relates in general to communication systems and components, and is particularly directed to a new and improved transconductance amplifier-based, rectifier circuit architecture that is preferably of the type described in my above-referenced '408 application, and is configured to programmably provide precision normal or inverted, half-wave or full-wave rectification of a single ended or differentially derived input signal.
- the transmission channels of subscriber line interface circuits, or SLICs, employed by telecommunication service providers include a very demanding set of performance requirements, including accuracy, linearity, insensitivity to common mode signals, low power consumption, low noise, filtering, and ease of impedance matching programmability, to facilitate interfacing the SLIC with a variety of telecommunication circuits including those providing digital codec functionality.
- the length of the wireline pair to which a SLIC is connected can be expected to vary from installation to installation, may have a significant length (e.g., on the order of multiple miles), and is used to transport both substantial DC voltages, as well as AC signals (e.g., voice and/or ringing).
- transconductance amplifier circuit a schematic diagram of a non-limiting bipolar transistor-configured implementation of which is shown in FIG. 1, that is configured to transform a single ended input voltage into a very precise, single ended output current, without requiring a substantial quiescent current, and in a manner which is effectively independent of (differential) voltage supply rails through which the circuit is powered.
- the transconductance amplifier circuit is shown as including an operational amplifier configured as a unity gain buffer 100 .
- the operational amplifier has a dual polarity input operational amplifier input and gain stage 110 , and a low output impedance, single ended output stage 120 .
- the input and gain stage 110 which may have a conventional high impedance, moderate voltage gain circuit configuration, has a first, non-inverting polarity input 111 , that is adapted to be coupled to a DC reference voltage, shown as a voltage v 0 (relative to ground (GND)), and a second, inverting polarity input 112 , which is adapted to track the voltage v 0 .
- the input voltage v 0 can be selected in compliance with the overhead voltages and power dissipation required by the specific application in which the transconductance amplifier circuit is employed.
- the output stage 120 includes a differentially coupled transistor circuit pair, having a first, diode-connected NPN transistor 130 , whose collector 131 and base 132 are connected in common to a first polarity output port 113 of the amplifier's input stage 110 .
- the emitter 133 of transistor 130 is coupled in common to the emitter 143 of a second, diode-connected PNP transistor 140 .
- PNP transistor 140 has its collector 141 and base 142 connected in common to a second polarity output port 114 of the amplifier input stage 110 .
- the base 132 of NPN transistor 130 is coupled in common with the base 152 of an NPN transistor 150 , the emitter 153 of which is coupled in common to the emitter 163 of a PNP transistor 160 and to an input/output node 123 of output stage 120 .
- the PNP transistor 160 has its base 162 coupled in common with the base 142 of the PNP transistor 140 .
- the output stage has an input/output node 123 is coupled over a negative feedback path 126 to the inverting input 112 of the input stage 110 .
- the input/output node 123 rather than being employed to supply an output current to a downstream load, is coupled to receive one or more input currents, respectively supplied through one or more coupling resistors, to associated voltage feed ports.
- FIG. 1 shows a single coupling resistor Z 1 coupled to an input port 125 .
- these current mirror circuits serve to isolate the biasing of the amplifier's output stage 120 from its power supply terminals, so that the output current produced at a single ended output port 135 can be accurately controlled independent of the values of the power supply voltages.
- the current mirror circuit 170 includes a first PNP transistor 200 having its emitter 203 coupled to the (Vcc) voltage supply rail 155 , and its base 202 coupled in common with the base 212 and collector 211 of a diode-connected current mirror PNP transistor 210 , whose emitter 213 is coupled to (Vcc) voltage supply rail 155 .
- the current mirror transistor 200 supplies a mirrored output current to the current supply path 172 as a prescribed factor K of the current received by transistor 210 over the current supply path 171 , in accordance with the ratio (1:K) of the geometries of the transistors 210 / 200 .
- the collector 211 and base 212 of transistor 210 are coupled over the first current supply path 171 of the current mirror 170 to the collector 151 of transistor 150 of the output stage 120 .
- the collector 201 of transistor 200 is coupled over a second current supply path 172 of the current mirror 170 to a transconductance stage output node 135 .
- the current mirror circuit 180 includes a first NPN transistor 220 having its emitter 223 coupled to the (Vee) voltage supply rail 156 and its base 222 coupled in common with the base 232 and collector 231 of a diode-connected current mirror NPN transistor 230 , whose emitter 233 is coupled to (Vee) voltage supply rail 156 .
- the collector 231 and base 232 of the current mirror transistor 230 are coupled over the first current supply path 181 of the current mirror 180 to the collector 161 of output stage transistor 160 .
- the collector 221 of transistor 220 is coupled over a second current supply path 182 of the current mirror 180 to the output node 135 .
- the current mirror transistor 220 provides a mirrored output current to current supply path 182 as a factor K of the current received by transistor 230 over current supply path 181 , in accordance with the (1:K) ratio of the geometries of transistors 230 / 220 .
- the single ended output current i 123 delivered to input/output node 123 may be defined in equation (1) as:
- the currents i 171 and i 181 supplied to current mirrors 170 and 180 may be related to the current i 123 at the input/output node 123 by equation (2) as:
- the currents i 172 and i 182 supplied by current mirrors 170 and 180 may be related to the current i 135 at the output node 135 by equation (3):
- Equations (2) and (4) imply that transistor limitations due to beta and early voltage are compensated or minimized (in a manner not specifically shown in the diagrammatic illustration of FIG. 1). It may also be noted that if transistors 130 / 150 and 140 / 160 are matched pairs and the time average value of the input voltage is equal to zero, then the time average values of currents i 171 and i 181 are equal to the DC bias current I DC flowing in the emitter path of the output stage transistors 130 - 140 . As a consequence, if the value of the bias current I DC is relatively low and the current mirror ratio K is equal to or less than 1, the quiescent power consumed by the transconductance amplifier circuit can be reduced to a very small value.
- transconductance amplifier circuit of FIG. 1 is a building block for one or more subcircuits, such as but not limited to those employed within a subscriber line interface circuit, or SLIC.
- the transconductance amplifier circuit of my above-referenced '408 application and shown in FIG. 1 described above is used to realize a new and improved, precision half-wave or full-wave rectifier for a single ended or differentially source signal.
- the very precise output current produced by the commonly connected outputs of the current mirror circuits that isolate the biasing of the transconductance amplifier's output stage from its power supply terminals is coupled to a first pair of rectifier elements arranged in complementary polarity-coupling directions to a first pair of rectifier terminals.
- each of the current mirror circuits includes an additional current mirror output.
- These additional current mirror outputs are coupled to respective auxiliary current mirror stages, whose outputs are coupled in common to a second pair of rectifier elements arranged in complementary polarity-coupling directions to a second pair of rectifier terminals.
- Respective ones of the first and second pairs of rectifier terminals are selectively (programmably) coupled to a prescribed reference voltage (e.g., ground) or to a single ended input terminal of an output amplifier stage.
- the output amplifier stage provides one of a normal or inverted, half-wave or a full-wave rectified voltage output signal.
- FIG. 1 schematically shows a transconductance amplifier circuit in accordance with the invention disclosed in the above-referenced '408 application.
- FIG. 2 diagrammatically illustrates a transconductance amplifier-based, rectifier circuit architecture in accordance with the present invention.
- the overall architecture of the transconductance amplifier-based, rectifier circuit architecture of the invention is diagrammatically illustrated in FIG. 2 as comprising a front end, transconductance amplifier stage 300 , the circuit configuration of which corresponds to that of the transconductance amplifier circuit of FIG. 1.
- the front end, transconductance amplifier stage 300 includes a unity gain buffer operational amplifier having a dual polarity input operational amplifier input and gain stage 310 , and a low output impedance, single ended output stage 320 .
- the input and gain stage 310 has a first, non-inverting polarity (+) input 311 , that is coupled to a first input port IN 0 that is adapted to receive a first voltage v 0 , referenced to a prescribed DC voltage (e.g., ground (GND)), as shown.
- a prescribed DC voltage e.g., ground (GND)
- the low impedance output stage 320 is configured identically to the output stage 120 in FIG. 1, so that a description thereof will not be repeated here.
- the low impedance output stage 320 has its input/output node 323 coupled to the second, inverting polarity ( ⁇ ) input 312 of the input gain stage 310 , and through an input resistor 325 to a second input port IN 1 , that is adapted to receive a second voltage v 1 , referenced to a prescribed DC voltage (e.g., GND), as shown.
- a prescribed DC voltage e.g., GND
- the (differential) voltage is applied across the input terminals IN 0 and IN 1 ; for single ended applications, one of the two input terminals IN 0 and IN 1 is coupled to a prescribed reference potential (e.g. GND), and the input signal is coupled to the other input terminal.
- a prescribed reference potential e.g. GND
- the transconductance amplifier-based, rectifier circuit architecture of FIG. 2 has its low impedance output stage 320 coupled to a pair of current mirror circuits 370 and 380 , which isolate the biasing of the amplifier's output stage from its power supply terminals, and have current supply paths 372 and 382 thereof coupled to a current output node 335 (which corresponds to the single ended output node 135 of FIG. 1).
- the current output node 335 is coupled in common to a first pair of rectifier elements (diodes) 341 and 342 , that are coupled in complementary polarity directions to a first pair of rectifier-coupled terminals 345 and 346 , respectively.
- terminals 345 and 346 are selectively coupled to one of a prescribed reference voltage (GND) or an input terminal 401 of a downstream output amplifier stage 400 .
- GND prescribed reference voltage
- each of the current mirror circuits 370 and 380 further includes an additional current mirror output transistor, from which a respective copy of the mirrored current of the current supply path 372 , 382 is supplied.
- these additional mirrored copies of the mirrored currents of the current mirror output paths 372 and 382 are supplied over first and second additional mirror current supply paths 374 and 384 , respectively.
- the first additional mirror current supply path 374 is coupled to an input 351 of a first auxiliary current mirror stage 350 ; the second additional mirror current supply path 384 is coupled to an input 361 of a second auxiliary current mirror stage 360 .
- the auxiliary current mirror stages 350 and 360 have respective outputs 352 and 362 thereof coupled in common via node 365 to a second pair of rectifier elements (diodes) 391 and 392 , that are coupled in complementary polarity directions to a second pair of rectifier-coupled terminals 395 and 396 , respectively.
- the terminals 395 and 396 are selectively coupled to one of a prescribed reference voltage (GND) or the input terminal 401 of the output amplifier stage 400 .
- GND prescribed reference voltage
- the output amplifier stage 400 contains an operational amplifier 410 having its non-inverting (+) input 411 coupled to a prescribed reference voltage (here GND) and its inverting ( ⁇ ) input 412 coupled to the input terminal 401 .
- the operational amplifier 410 has its output 413 coupled to an output voltage Vout terminal 402 and through a feedback resistor 415 to inverting ( ⁇ ) input 412 .
- I 346 and I 396 are phase complementary.
- the voltage Vout at the output terminal 402 can be programmed as one of the following rectified output voltages.
- Vout a half-wave rectified voltage signal, where the output amplifier input terminal 401 is coupled to diode-coupled terminal 395 .
- Vout an inverted half-wave rectified voltage signal, where the output amplifier input terminal 401 is coupled to diode-coupled terminal 345 .
- Vout a full-wave rectified voltage signal, where the output amplifier input terminal 401 is coupled in common to diode-coupled terminals 346 and 395 .
- Vout an inverted full-wave rectified voltage signal, where the output amplifier input terminal 401 is coupled in common to diode-coupled terminals 345 and 396 .
- crossover distortion in the rectifier architecture of the present invention is limited to that resulting from the time required to turn-on the diodes 341 , 342 , 391 or 392 , and not from the diode voltage itself.
- Time distortion improvement over conventional rectification schemes can be substantial, especially at low signal frequencies, such as voice frequencies of SLIC applications.
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Abstract
Description
- The present application is a continuation-in-part of my co-pending U.S. patent application Ser. No. 09/639,408, entitled: “Transconductance Amplifier Circuit,” filed Aug. 14, 2000 (hereinafter referred to as the '408 application), assigned to the assignee of the present application, and the disclosure of which is incorporated herein.
- The present invention relates in general to communication systems and components, and is particularly directed to a new and improved transconductance amplifier-based, rectifier circuit architecture that is preferably of the type described in my above-referenced '408 application, and is configured to programmably provide precision normal or inverted, half-wave or full-wave rectification of a single ended or differentially derived input signal.
- As described in the above-referenced '408 application, the transmission channels of subscriber line interface circuits, or SLICs, employed by telecommunication service providers include a very demanding set of performance requirements, including accuracy, linearity, insensitivity to common mode signals, low power consumption, low noise, filtering, and ease of impedance matching programmability, to facilitate interfacing the SLIC with a variety of telecommunication circuits including those providing digital codec functionality. In a typical application, the length of the wireline pair to which a SLIC is connected can be expected to vary from installation to installation, may have a significant length (e.g., on the order of multiple miles), and is used to transport both substantial DC voltages, as well as AC signals (e.g., voice and/or ringing). As a consequence, it has been difficult to realize a SLIC implementation that has ‘universal’ use in both legacy and state of the art installations.
- In accordance with the invention disclosed in the above-referenced '408 application, such shortcomings of conventional transconductance amplifier circuits are effectively obviated by a transconductance amplifier circuit, a schematic diagram of a non-limiting bipolar transistor-configured implementation of which is shown in FIG. 1, that is configured to transform a single ended input voltage into a very precise, single ended output current, without requiring a substantial quiescent current, and in a manner which is effectively independent of (differential) voltage supply rails through which the circuit is powered.
- In FIG. 1, the transconductance amplifier circuit is shown as including an operational amplifier configured as a
unity gain buffer 100. The operational amplifier has a dual polarity input operational amplifier input andgain stage 110, and a low output impedance, singleended output stage 120. The input andgain stage 110, which may have a conventional high impedance, moderate voltage gain circuit configuration, has a first,non-inverting polarity input 111, that is adapted to be coupled to a DC reference voltage, shown as a voltage v0 (relative to ground (GND)), and a second, invertingpolarity input 112, which is adapted to track the voltage v0. The input voltage v0 can be selected in compliance with the overhead voltages and power dissipation required by the specific application in which the transconductance amplifier circuit is employed. - The
output stage 120 includes a differentially coupled transistor circuit pair, having a first, diode-connectedNPN transistor 130, whosecollector 131 andbase 132 are connected in common to a firstpolarity output port 113 of the amplifier'sinput stage 110. Theemitter 133 oftransistor 130 is coupled in common to theemitter 143 of a second, diode-connectedPNP transistor 140. In a complementary fashion,PNP transistor 140 has itscollector 141 andbase 142 connected in common to a secondpolarity output port 114 of theamplifier input stage 110. Thebase 132 ofNPN transistor 130 is coupled in common with thebase 152 of anNPN transistor 150, theemitter 153 of which is coupled in common to theemitter 163 of aPNP transistor 160 and to an input/output node 123 ofoutput stage 120. - The
PNP transistor 160 has itsbase 162 coupled in common with thebase 142 of thePNP transistor 140. The output stage has an input/output node 123 is coupled over anegative feedback path 126 to the invertinginput 112 of theinput stage 110. Unlike a conventional amplifier circuit, the input/output node 123, rather than being employed to supply an output current to a downstream load, is coupled to receive one or more input currents, respectively supplied through one or more coupling resistors, to associated voltage feed ports. In order to reduce the complexity of the drawing FIG. 1 shows a single coupling resistor Z1 coupled to aninput port 125. - The series-connected, collector-emitter current paths through the
150 and 160 of the transconductance amplifier'soutput transistors output stage 120, rather than being biased via a direct coupling to respective (Vcc and Vee) 155 and 156, are coupled in circuit with firstvoltage supply rails 171 and 181 of first and secondcurrent supply paths 170 and 180, respectively. As pointed out briefly above, these current mirror circuits serve to isolate the biasing of the amplifier'scurrent mirror circuits output stage 120 from its power supply terminals, so that the output current produced at a singleended output port 135 can be accurately controlled independent of the values of the power supply voltages. - The
current mirror circuit 170 includes afirst PNP transistor 200 having its emitter 203 coupled to the (Vcc)voltage supply rail 155, and itsbase 202 coupled in common with thebase 212 andcollector 211 of a diode-connected currentmirror PNP transistor 210, whoseemitter 213 is coupled to (Vcc)voltage supply rail 155. Thecurrent mirror transistor 200 supplies a mirrored output current to thecurrent supply path 172 as a prescribed factor K of the current received bytransistor 210 over thecurrent supply path 171, in accordance with the ratio (1:K) of the geometries of thetransistors 210/200. Thecollector 211 andbase 212 oftransistor 210 are coupled over the firstcurrent supply path 171 of thecurrent mirror 170 to thecollector 151 oftransistor 150 of theoutput stage 120. Thecollector 201 oftransistor 200 is coupled over a secondcurrent supply path 172 of thecurrent mirror 170 to a transconductancestage output node 135. - The
current mirror circuit 180 includes afirst NPN transistor 220 having itsemitter 223 coupled to the (Vee)voltage supply rail 156 and itsbase 222 coupled in common with thebase 232 andcollector 231 of a diode-connected currentmirror NPN transistor 230, whoseemitter 233 is coupled to (Vee)voltage supply rail 156. Thecollector 231 andbase 232 of thecurrent mirror transistor 230 are coupled over the firstcurrent supply path 181 of thecurrent mirror 180 to the collector 161 ofoutput stage transistor 160. Thecollector 221 oftransistor 220 is coupled over a secondcurrent supply path 182 of thecurrent mirror 180 to theoutput node 135. Thecurrent mirror transistor 220 provides a mirrored output current tocurrent supply path 182 as a factor K of the current received bytransistor 230 overcurrent supply path 181, in accordance with the (1:K) ratio of the geometries oftransistors 230/220. - An examination of current node equations, set forth below, that define the transfer function of the transconductance amplifier circuit of FIG. 1, reveals that it has a very wide dynamic range and is capable of accommodating single or multiple, differential polarity voltages applied at its one or more voltage feed ports. This wide dynamic range is obtained at a very low quiescent power dissipation.
- More particularly, the single ended output current i 123 delivered to input/
output node 123 may be defined in equation (1) as: - i 123=(v 125-1 −v 111)/R 1 (1)
- The currents i 171 and i181 supplied to
170 and 180 may be related to the current i123 at the input/current mirrors output node 123 by equation (2) as: - The currents i 172 and i182 supplied by
170 and 180 may be related to the current i135 at thecurrent mirrors output node 135 by equation (3): - i 172 +i 135 =i 182 (3)
- and equation (4) as:
- Substituting equation (1) into equation (4) yields equation (5) as:
- i out =K(v 125 −v 111)/R 1 (5)
- Equations (2) and (4) imply that transistor limitations due to beta and early voltage are compensated or minimized (in a manner not specifically shown in the diagrammatic illustration of FIG. 1). It may also be noted that if
transistors 130/150 and 140/160 are matched pairs and the time average value of the input voltage is equal to zero, then the time average values of currents i171 and i181 are equal to the DC bias current IDC flowing in the emitter path of the output stage transistors 130-140. As a consequence, if the value of the bias current IDC is relatively low and the current mirror ratio K is equal to or less than 1, the quiescent power consumed by the transconductance amplifier circuit can be reduced to a very small value. - As described above, a particularly useful application of the transconductance amplifier circuit of FIG. 1 is a building block for one or more subcircuits, such as but not limited to those employed within a subscriber line interface circuit, or SLIC.
- In accordance with the present invention, the transconductance amplifier circuit of my above-referenced '408 application and shown in FIG. 1 described above, is used to realize a new and improved, precision half-wave or full-wave rectifier for a single ended or differentially source signal. To this end, the very precise output current produced by the commonly connected outputs of the current mirror circuits that isolate the biasing of the transconductance amplifier's output stage from its power supply terminals, is coupled to a first pair of rectifier elements arranged in complementary polarity-coupling directions to a first pair of rectifier terminals.
- In addition, each of the current mirror circuits includes an additional current mirror output. These additional current mirror outputs are coupled to respective auxiliary current mirror stages, whose outputs are coupled in common to a second pair of rectifier elements arranged in complementary polarity-coupling directions to a second pair of rectifier terminals. Respective ones of the first and second pairs of rectifier terminals are selectively (programmably) coupled to a prescribed reference voltage (e.g., ground) or to a single ended input terminal of an output amplifier stage. Depending on this set of programmable connections, the output amplifier stage provides one of a normal or inverted, half-wave or a full-wave rectified voltage output signal.
- FIG. 1 schematically shows a transconductance amplifier circuit in accordance with the invention disclosed in the above-referenced '408 application; and
- FIG. 2 diagrammatically illustrates a transconductance amplifier-based, rectifier circuit architecture in accordance with the present invention.
- The overall architecture of the transconductance amplifier-based, rectifier circuit architecture of the invention is diagrammatically illustrated in FIG. 2 as comprising a front end,
transconductance amplifier stage 300, the circuit configuration of which corresponds to that of the transconductance amplifier circuit of FIG. 1. As described above, and as shown in FIG. 2, the front end,transconductance amplifier stage 300 includes a unity gain buffer operational amplifier having a dual polarity input operational amplifier input andgain stage 310, and a low output impedance, singleended output stage 320. The input andgain stage 310 has a first, non-inverting polarity (+)input 311, that is coupled to a first input port IN0 that is adapted to receive a first voltage v0, referenced to a prescribed DC voltage (e.g., ground (GND)), as shown. - The low
impedance output stage 320 is configured identically to theoutput stage 120 in FIG. 1, so that a description thereof will not be repeated here. The lowimpedance output stage 320 has its input/output node 323 coupled to the second, inverting polarity (−)input 312 of theinput gain stage 310, and through aninput resistor 325 to a second input port IN1, that is adapted to receive a second voltage v1, referenced to a prescribed DC voltage (e.g., GND), as shown. For differential applications, the (differential) voltage is applied across the input terminals IN0 and IN1; for single ended applications, one of the two input terminals IN0 and IN1 is coupled to a prescribed reference potential (e.g. GND), and the input signal is coupled to the other input terminal. - Also, like the transconductance amplifier of FIG. 1, the transconductance amplifier-based, rectifier circuit architecture of FIG. 2 has its low
impedance output stage 320 coupled to a pair of 370 and 380, which isolate the biasing of the amplifier's output stage from its power supply terminals, and havecurrent mirror circuits 372 and 382 thereof coupled to a current output node 335 (which corresponds to the single endedcurrent supply paths output node 135 of FIG. 1). - Pursuant to the invention, the
current output node 335 is coupled in common to a first pair of rectifier elements (diodes) 341 and 342, that are coupled in complementary polarity directions to a first pair of rectifier-coupled 345 and 346, respectively. As will be described, depending upon intended rectifier functionality,terminals 345 and 346 are selectively coupled to one of a prescribed reference voltage (GND) or anterminals input terminal 401 of a downstreamoutput amplifier stage 400. - In addition to having its
output node 335 coupled to the first pair of 341 and 342, each of therectifier elements 370 and 380 further includes an additional current mirror output transistor, from which a respective copy of the mirrored current of thecurrent mirror circuits 372, 382 is supplied. In FIG. 2, these additional mirrored copies of the mirrored currents of the currentcurrent supply path 372 and 382 are supplied over first and second additional mirrormirror output paths 374 and 384, respectively.current supply paths - The first additional mirror
current supply path 374 is coupled to aninput 351 of a first auxiliarycurrent mirror stage 350; the second additional mirrorcurrent supply path 384 is coupled to aninput 361 of a second auxiliarycurrent mirror stage 360. The auxiliary current mirror stages 350 and 360 have 352 and 362 thereof coupled in common viarespective outputs node 365 to a second pair of rectifier elements (diodes) 391 and 392, that are coupled in complementary polarity directions to a second pair of rectifier-coupled 395 and 396, respectively. As is the case with rectifier-coupledterminals 345 and 346, depending upon intended rectifier functionality, theterminals 395 and 396 are selectively coupled to one of a prescribed reference voltage (GND) or theterminals input terminal 401 of theoutput amplifier stage 400. - The
output amplifier stage 400 contains anoperational amplifier 410 having its non-inverting (+)input 411 coupled to a prescribed reference voltage (here GND) and its inverting (−)input 412 coupled to theinput terminal 401. Theoperational amplifier 410 has itsoutput 413 coupled to an outputvoltage Vout terminal 402 and through afeedback resistor 415 to inverting (−)input 412. - In operation, let each of the diode-coupled
345, 346 and 395, 396 be initially coupled to ground (or a virtual ground). In this condition, if a current I325-1 through theterminals input resistor 325 from thenode 323 into the input terminal IN1 as a result of the relative polarity between input terminals IN0 and IN1, then the following equations (6) and (7) hold: - I 395 =I 345 =I 325-1, (6)
- I 396 =I 346=0 (7)
- where I 345 and I395 are phase complementary.
- Conversely, when a current I 325-2 through the
input resistor 325 from the input terminal IN1 into thenode 323 as a result of the relative polarity between input terminals IN1 and IN0, then the following equations (8) and (9) hold: - I 395 =I 345=0, (8)
- I 396 =I 346 = I 325-2, (9)
- where I 346 and I396 are phase complementary.
- From these relationships, it can be seen that, depending upon which of the diode-coupled
345, 346, 395, 396 are selectively disconnected from ground and reconnected to theterminals input terminal 401 of the output amplifier stage 400 (the remaining diode-coupled output terminals being grounded), the voltage Vout at theoutput terminal 402 can be programmed as one of the following rectified output voltages. - 1: Vout=a half-wave rectified voltage signal, where the output
amplifier input terminal 401 is coupled to diode-coupledterminal 395. - 2: Vout=an inverted half-wave rectified voltage signal, where the output
amplifier input terminal 401 is coupled to diode-coupledterminal 345. - 3: Vout=a full-wave rectified voltage signal, where the output
amplifier input terminal 401 is coupled in common to diode-coupled 346 and 395.terminals - 4: Vout=an inverted full-wave rectified voltage signal, where the output
amplifier input terminal 401 is coupled in common to diode-coupled 345 and 396.terminals - It should also be noted that crossover distortion in the rectifier architecture of the present invention is limited to that resulting from the time required to turn-on the
341, 342, 391 or 392, and not from the diode voltage itself. Time distortion improvement over conventional rectification schemes can be substantial, especially at low signal frequencies, such as voice frequencies of SLIC applications.diodes - While I have shown and described an several embodiment in accordance with the present invention, it is to be understood that the same is not limited thereto but is susceptible to numerous changes and modifications as known to a person skilled in the art, and I therefore do not wish to be limited to the details shown and described herein, but intend to cover all such changes and modifications as are obvious to one of ordinary skill in the art.
Claims (15)
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US09/901,260 US6452450B1 (en) | 2000-08-14 | 2001-07-09 | Transconductance amplifier based precision half wave and full wave rectifier circuit |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US09/639,408 US6411163B1 (en) | 2000-08-14 | 2000-08-14 | Transconductance amplifier circuit |
| US09/901,260 US6452450B1 (en) | 2000-08-14 | 2001-07-09 | Transconductance amplifier based precision half wave and full wave rectifier circuit |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US09/639,408 Continuation-In-Part US6411163B1 (en) | 2000-08-14 | 2000-08-14 | Transconductance amplifier circuit |
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| US20020021175A1 true US20020021175A1 (en) | 2002-02-21 |
| US6452450B1 US6452450B1 (en) | 2002-09-17 |
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| US7981023B2 (en) | 2005-07-25 | 2011-07-19 | Boston Scientific Scimed, Inc. | Elastic sling system and related methods |
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| US8049487B2 (en) * | 2008-11-25 | 2011-11-01 | Linear Technology Corporation | Power measurement circuit |
| US20100127754A1 (en) * | 2008-11-25 | 2010-05-27 | Linear Technology Corporation | Power measurement circuit |
| US8472221B1 (en) | 2010-05-07 | 2013-06-25 | Alfred E. Mann Foundation For Scientific Research | High voltage rectifier using low voltage CMOS process transistors |
| US9636201B2 (en) | 2011-05-12 | 2017-05-02 | Boston Scientific Scimed, Inc. | Delivery members for delivering an implant into a body of a patient |
| US9113991B2 (en) | 2011-05-12 | 2015-08-25 | Boston Scientific Scimed, Inc. | Anchors for bodily implants and methods for anchoring bodily implants into a patient's body |
Family Cites Families (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4091333A (en) | 1977-07-25 | 1978-05-23 | Valhalla Scientific Incorporated | Transconductance amplifier circuit |
| JPS60103814A (en) | 1983-11-11 | 1985-06-08 | Toshiba Corp | Signal processing circuit |
| DE59109062D1 (en) | 1991-04-16 | 1998-11-12 | Siemens Ag | Output buffer amplifier with a large signal swing |
| US5410274A (en) * | 1992-09-16 | 1995-04-25 | Hughes Aircraft Company | Single-ended and differential amplifiers with high feedback input impedance and low distortion |
| US5357210A (en) | 1993-07-07 | 1994-10-18 | National Research Council Of Canada | Transconductance amplifier circuit |
| US5671272A (en) | 1995-01-30 | 1997-09-23 | Harris Corporation | Current mode ring trip detector |
| US5521552A (en) * | 1995-06-06 | 1996-05-28 | Analog Devices, Inc. | Bipolar micro-power rail-to-rail amplifier |
| JP3697679B2 (en) | 1997-09-25 | 2005-09-21 | ローム株式会社 | Stabilized power circuit |
| US5973563A (en) | 1997-12-10 | 1999-10-26 | National Semiconductor Corporation | High power output stage with temperature stable precisely controlled quiescent current and inherent short circuit protection |
| US6259322B1 (en) * | 1999-10-28 | 2001-07-10 | Texas Instruments Incorporated | Current efficient, ultra low noise differential gain amplifier architecture |
-
2001
- 2001-07-09 US US09/901,260 patent/US6452450B1/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| US6452450B1 (en) | 2002-09-17 |
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