This invention relates to calibration of a sense resistor used with power sourcing equipment (PSE) in power over ethernet (POE) applications.
Power sourcing equipment (PSE) compliant with IEEE 802.3 provides power to a powered device (PD) over the Ethernet cables. The power sourcing equipment includes a smart controller that ensures that the power is provided safely. The PSE measures the output power and shuts off power if the load (the PD) is drawing too much power. In some applications, in order to be considered safe the power is limited to 100 W. In many implementations, a current sense resistor is used to measure power being supplied by the PSE to the PD.
Improvements in power measurement allow more precise control over the power being supplied to the PD.
Accordingly, embodiments herein provide improved knowledge of the resistance value of the sense resistor to thereby improve the accuracy of power measurement. An accurate measurement of the resistance value of the sense resistor allows compensation for parasitic resistance, manufacturing variations of the resistor, and long term drift in the resistance value of the resistor. That allows accurate provision of maximum power levels.
In one embodiment, a method includes causing a first current to go through a sense resistor from a first current source and measuring a first voltage across the sense resistor resulting from the first current. The method further includes causing a second current to flow through the sense resistor from a second current source and measuring a second voltage across the sense resistor resulting from the second current. A resistance value of the sense resistor is determined based on a voltage difference between the first and second voltage and a current difference between the first current and the second current.
In another embodiment a method includes injecting a first current at a first node of a sense resistor from a first current source during a first time and injecting a second current at a second node of the sense resistor from a second current source during the first time, and measuring a first voltage across the sense resistor and parasitic resistance. The method further includes injecting a third current at the first node of the sense resistor from a third current source during a second time and injecting a fourth current at the second node of the sense resistor from a fourth current source during the second time and measuring a second voltage across the sense resistor and parasitic resistance. A resistance value of the sense resistor is determined, at least in part, based on a difference between the first voltage and the second voltage, and a current difference between the first current and the third current.
In another embodiment an apparatus includes a transistor having a drain node coupled to a port and a sense resistor coupled between a source node of the transistor and ground. A first current source is coupled to provide a first current to the sense resistor and a second current source is coupled to provide a second current to the sense resistor. An amplifier is coupled to a first node and a second node of the sense resistor to provide an indication of a first voltage across the sense resistor with the first current and to provide an indication of a second voltage across the sense resistor with the second current.
In another embodiment an apparatus includes a transistor having a first current carrying node coupled to a port. A sense resistor has a first node coupled to a second current carrying node of the transistor and a second node coupled to ground. A first current source supplies a first current at a first time to the sense resistor through the first node and a second current source supplies a second current to the second node at the first time. An amplifier circuit is coupled to the first node and the second node of the sense resistor to provide a first voltage measurement indicating a first voltage across the sense resistor at the first time. A third current source is coupled to supply a third current at a second time to the sense resistor through the first node and a fourth current source supplies a fourth current to the second node at the second time. The amplifier circuit provides a second voltage measurement indicating a second voltage across the sense resistor at the second time.
The present invention may be better understood, and its numerous objects, features, and advantages made apparent to those skilled in the art by referencing the accompanying drawings.
The use of the same reference symbols in different drawings indicates similar or identical items.
where ΔV is the difference in the voltage measurements and ΔI is the difference in the currents. The value of the current sources can be determined during manufacturing testing and ΔI stored in non volatile memory (NVM) 221. In calculating the difference between the first and second voltage measurements, note that the offset voltage is canceled.
Since having the gain of the amplifier 209 known is important for accuracy, in an embodiment the gain of the amplifier is measured and stored and the stored gain value is used for appropriate compensation to provide greater accuracy in measuring the voltage value. In addition, the accuracy of the resistance measurement is limited by the resolution of the ADC, which should be chosen to meet desired accuracy. For the ADC implemented, it is desirable to use as much of the range of the ADC as possible in determining the resistance.
where ΔI(I2−I1) is known. The value of Rsense is stored for use in power calculations by the PSE during runtime. However, the embodiment described in
The programmed microcontroller 115 controls the measurement sequence for determining the parasitic resistance, including turning on the current sources at the appropriate times, causing the switches to open and close as needed, ensuring the transistor 105 is on or off as needed during the voltage measurements, storing the digital values of the voltage supplied by the ADC 311, and making the calculations to determine Rsense1, Rsense2, and Rparastic. Software to control the operations to make the parasitic measurement can be stored in NVM 221 with the results stored in SRAM 223, NVM 221 (or other storage locations).
where ΔI is known.
Next the second resistance measurement is made using a different current path, namely current injection at the source terminal 320. The second measurement sequence starts in 362 by turning off transistor 105, opening switch 307, closing switch 308, and injecting current at the source terminal 320. In 364, the differential amplifier 309 measures the third voltage across the sense resistor and the ADC 311 supplies the third measured voltage to the microcontroller directly or by storing the first measured voltage in a designated storage location. Next in 366, the control sequence turns off the current source 301 supplying I1 and turns on the current source 303 supplying I2. In step 368, the fourth voltage across the sense resistor is measured and the result is supplied to the microcontroller 115 or otherwise stored. In 370 the current source(s) are turned off and in 372 the resistance is calculated as
where ΔI is known. Finally, the microcontroller calculates the Rparasitic=Rsense2−Rsense1 in 374 and stores the measurement of the parasitic for use in future measurements of Rsense. Of course, the two resistance measurements can be stored instead of the value of the parasitic resistance. During operation, knowing the parasitic resistance allows the PSE to make more accurate power measurements and thereby supply the maximum amount of power permitted. Note that the order of some of the steps shown in
where ΔI is known as described earlier. Together with Rsense1 and Rsense2 measurements made during board testing to determine the parasitic resistance, changes in Rsense during the life of the product can be accounted for by only measuring Rsense2 operationally and subtracting out the parasitic resistance. As described earlier, the parasitic resistance measured at board testing may be adjusted by the percentage change in operational Rsense2 from the board testing value of Rsense2.
Vs+=I×(Rp4+Rsense+Rp5+Rp6),
where Rpn are various parasitic resistances shown in
Vs−=I×(Rp6),
also assuming the resistance R 410>>Rsense.
Vout1 (using the current source supplying I1) at node 416 of the differential amplifier 409 can be calculated as
Vout1≅VREF−100(I1×(Rp4+Rsense+Rp5)+Vos).
The voltage measurement is repeated for I=I2 from the current source 403.
Vout2≅VREF−100(I2×(Rp4+Rsense+Rp5)+Vos).
ΔVout=100(ΔI×(Rp4+Rsense+Rp5)), where ΔI is the difference between the currents I1 and I2 and ΔVout is the difference in the two voltage measurements Vout1 and Vout2. Thus,
(Rp4+Rsense+Rp5)=ΔVout/(100ΔI).
Then the switch 407 is opened and the switch 408 closed. The transistor 105 is turned off. Current from the two current sources is sequentially injected on the source terminal 420 resulting in (for the I1 current injection):
Vs+=I
1×(Rp1+Rp2+Rp4+Rsense+Rp5+Rp6),
Vs−=I
1×(Rp6),
Vout1≅VREF−100(I1×(Rp1+Rp2+Rp4+Rsense+Rp5)+Vos),
The voltage measurement is repeated for I2 from the current source 403 and
Vout2≅VREF−100(I2×(Rp1+Rp2+Rp4+Rsense+Rp5)+Vos),
ΔVout=100(ΔI×(Rp1+Rp2+Rp4+Rsense+Rp5)), where ΔI=I2−I1+ and ΔVout=Vout1−Vout2; and
(Rp1+Rp2+Rp4+Rsense+Rp5)=ΔVout/(100ΔI)
Using the drain measured resistance value, the parasitic resistance can be determined from,
(Rp1+Rp2+Rp4+Rsense+Rp5)−(Rp4+Rsense+Rp5)=(Rp1+Rp2).
Microcontroller 115 (or other control logic), controls the switches and current sources, makes the calculations described and stores the parasitic resistance value along with the value of (Rp4+Rsense+Rp5) in memory if needed. The parasitic resistance value can be used during operation of the PSE to more accurately determine power being supplied to the load. The source injection measurements can be repeated during operation to ensure that accurate resistance values are maintained to compensate for, e.g., temperature changes or other resistance drift.
Vs+==I
1×(Rp1+Rp2+Rp4+Rsense+Rp5+2×Rp6),
where Rpn are the various parasitic resistances shown in
Vs−=I
1×(Rp1+Rp2+2×Rp6)),
where I1 is the current from the current source 502. The current sources are assumed to be well matched and supply equal I1 currents but in embodiments, the current sources are measured, e.g., in production test and the current values are stored in non-volatile memory. That way any differences in the current sources can be accounted for during the voltage calculations.
It is assumed that the resistances R 516 and 518>>Rsense. Vout at node 524 for the I1 current sources can be calculated as
Vout1≅VREF−100(I1×(Rp4+Rsense+Rp5)+Vos)
The voltage measurement is repeated with current source 503 and 504 simultaneously supplying the current I2 to the source node 520 and the sense node 522, respectively. Vs+=I2×(Rp1+Rp2+Rp4+Rsense+Rp5+2×Rp6), where Rpn are the various parasitic resistances shown in
Vs−=I
2×(Rp1+Rp2+2×Rp6)),
where I2 is the current from the current source 504. The current sources are assumed to be well matched and supply equal I2 currents but in embodiments, the current sources are measured, e.g., in production test and the current values are stored in NVM. That way any differences in the current sources can be accounted for during the voltage calculations.
It is assumed that the resistances R 516 and 518>>Rsense. Vout at node 524 for the I2 current sources can be calculated as
Vout2=VREF−100(I2×(Rp4+Rsense+Rp5)+Vos)
Again, the current sources are assumed to be well matched and supply equal I2 currents but in embodiments the values of the current sources are measured during production test and stored in NVM for use during sense resistor measurement. Mismatch in the current sources can be compensated for digitally or as described further herein. With two voltage measurements made from the two pairs of current sources, ΔVout=100(ΔI×(Rp4+Rsense+Rp5), where ΔVout=(Vout2−Vout1) and ΔI is the difference in the currents (I2−I1). Thus, the resistance used for a current measurement to determine if the power supplied to the load is within appropriate limits is given by, (Rp4+Rsense+Rp5)=ΔVout/(100ΔI). While Rp4 and Rp5 and parasitic resistances, those resistances are part of the sense resistance and thus when measuring the voltage across the sense resistance, the parasitic resistances Rp4 and Rp5 are necessarily present and considered part of Rsense for measurement purposes. While switch 514 is shown in the embodiment of
The topology shown in
(1) ΔI mismatch×(Rp1+Rp2)<<Rsense, and
(2) Rp1 mismatch+Rp2 mismatch<<Rsense.
Both conditions are met when (Rp1+Rp2)<<Rsense. That suggests that mismatch of the current sources and Rp should be minimized to the extent possible.
In order to address current mismatch in the current sources, an embodiment swaps the current sources that are coupled to the source and sense terminals during measurements and the measurements are averaged. Referring to
Vsource=I1×[1.1×(Rp2+Rp4+Rsense+Rp5+Rp6)+(0.9×Rp6)].
Injection on the sense terminal 722 from current source 702 results in
Vsense=I1×[0.9×(Rp2+Rp6)+(1.1×Rp6)].
Vsource−Vsense−=I1×[1.1×(Rp4+Rsense+Rp5)+(0.2×Rp2)]
The current sources are then swapped through additional switches not shown and for the second voltage measurement current source 702 supplies the current I1×0.9 to the source terminal 720 and current source 701 supplies the current I1×1.1 to the sense terminal 722. For the second voltage measurement, injection on the source terminal from current source 702 results in
Vsource=I1×[0.9×(Rp2+Rp4+Rsense+Rp5+Rp6)+(1.1×Rp6)],
Injection at the sense terminal from current source 701
Vsense=I1×[1.1(Rp2+Rp6)+(0.9×Rp6)],
Vsource−Vsense=I1×[0.9×(Rp4+Rsense+Rp5)−(0.2×Rp2)]
In order to address the current mismatch, the two voltage measurements are averaged resulting in,
Average(Vsource−vsense)=I1×(Rp4+Rsense+Rp5).
The voltage measurements are then repeated for the current sources supplying I2 (not shown in
Note that averaging has no impact on Rp2 mismatch, so for a 1% calibration Rp2 should be matched, e.g., within 1 mOhm. For ease of illustration, Rp1 was omitted from
Measuring the resistance of Rsense using the source path (after having previously made the drain path injection) or measuring by injecting simultaneously at the source and sense nodes, allows a load to be on the port terminal during measurements. That assumes that the external load does not change during the measurements. Given the POE environment, the external load should generally be stable. Of course, measurements can be made injecting at the source terminal with transistor 105 off or by injecting at the source and sense terminals simultaneously with transistor 105 off. An accurate resistance measurement can then be used to accurately measure power being supplied to the load by measuring the voltage across the sense resistor.
Thus, various aspects of a calibration system to measure the resistance value of a sense resistor in a POE environment. The description of the invention set forth herein is illustrative, and is not intended to limit the scope of the invention as set forth in the following claims. Other variations and modifications of the embodiments disclosed herein, may be made based on the description set forth herein, without departing from the scope of the invention as set forth in the following claims.
This application is a continuation of U.S. application Ser. No. 16/846,731, filed Apr. 13, 2020, entitled “CALIBRATION OF THE EXTERNAL RESISTANCE VALUE IN THE POWER SOURCING EQUIPMENT OF A POE SYSTEM.” Each of the foregoing applications are incorporated herein by reference in their entirety.
Number | Date | Country | |
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Parent | 16846731 | Apr 2020 | US |
Child | 17991543 | US |