A system and method for efficiently charging and discharging a capacitive load from a single voltage source. The system includes a first switch for selectively connecting the voltage source to the load and a second switch for selectively providing a short across the load as may be common in the art. A particularly novel aspect of the invention resides in the provision of plural capacitive elements and a switching mechanism for selectively connecting each of the capacitive elements to the load whereby the load is gradually charged or discharged. In the illustrative embodiment, the switching mechanism includes a set of switches for selectively connecting each of the capacitive elements to the capacitive load and a switch control mechanism for selectively activating the switches.
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0. 12. A method for driving a capacitive load, comprising:
minimizing power dissipation by discharging the capacitive load by incremental voltage steps using a switching system which includes a switch for selectively discharging the load; and
electrically coupling a capacitive storage system to the capacitive load at an electrically floating node for discharging the capacitive load by one of the incremental voltage steps.
0. 15. A system for driving a capacitive load, comprising:
means for minimizing power dissipation by discharging the capacitive load by incremental voltage steps using a switching system which includes a switch for selectively discharging the load; and means for electrically coupling a capacitive storage system to the capacitive load at an electrically floating node for discharging the capacitive load by one of the incremental voltage steps.
0. 27. A method for charging and discharging a capacitive load comprising:
selectively coupling and de-coupling a capacitive device to and from the capacitive load to cause the charging and the discharging of the capacitive load to occur in a plurality of steps using a switching system which includes a switch for selectively discharging the load,
whereby energy is recovered from the capacitive load and whereby the recovered energy is always stored substantially only in capacitance.
0. 20. A system for charging and discharging a capacitive load in n steps, n being greater than 1, comprising:
N−1 capacitive devices; and
a first switching device operable to selectively couple and de-couple the N−1 capacitive devices to and from the capacitive load during a charging and a discharging of the capacitive load;
a switching system including a switch for selectively discharging the load,
whereby energy is recovered from the capacitive load and whereby the recovered energy is always stored substantially only in capacitance.
0. 18. A method for driving a load, the method comprising:
charging the load to a first level;
discharging the load to a second level using a switching system which includes a switch for selectively discharging the load, wherein during discharging to the second level, a first capacitor is charged to the second level by using the discharging charge of the load;
discharging the load to a third level using a switch; and
re-charging the load by using the charge of the first capacitor,
wherein the first level is higher from the second level and the second level is higher that the third level.
0. 1. A system for efficiently charging and discharging a capacitive load from a single voltage source of a first potential consisting of:
a first switch for selectively charging the load;
a second switch for selectively discharging the load;
plural capacitive elements; and
switch means for selectively connecting each of the capacitive elements to the capacitive load to gradually charge or discharge the capacitive load.
0. 2. The invention of
0. 3. The invention of
0. 4. The invention of
0. 5. The invention of
0. 6. The invention of
0. 7. The invention of
0. 8. The invention of
0. 9. The invention of
0. 10. The invention of
0. 11. A method for efficiently charging and discharging a capacitive load from a single voltage source including the steps of:
providing a first switch for selectively connecting the voltage source to the load;
providing a second switch for selectively providing a short across the load;
providing plural capacitive elements;
providing plural third switches for selectively connecting each of the capacitive elements to the capacitive load; and
selectively activating the first, second and third switches to gradually charge or discharge the capacitive load.
0. 13. The method of
0. 14. The method of
0. 16. The system of
0. 17. The system of
0. 19. A method of
0. 21. A system of
0. 22. The system of
0. 23. The system of
0. 24. The system of
0. 25. The system of
0. 26. The system of
a second switching device operable to selectively couple the capacitive load to a voltage source, and
a third switching device operable to selectively provide a short across the capacitive load.
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In accordance with the present teachings, power dissipation is reduced by charging the capacitance of the load CL in several steps. This is illustrated in FIG. 2.
If N steps are used, the dissipation per step is again given by the transferred charge and the average voltage drop across the switch resistance:
Estep=QV′=(CV/N) (V/2N)=CV2/2N2 [2]
To charge the capacitance all the way to the supply voltage V, N steps are used, so the total energy dissipation is:
Estepwise = N*Estep [3]
= N*CV2/2N2
= CV2/2N
= Econv/N
Again, a full charge-discharge cycle will cause twice the dissipation of the charging only. Thus, according to this simplified analysis, charging by several steps reduces the energy dissipation per charge-discharge cycle and thereby the total power dissipation, by a factor of N.
The multiple supply voltages of
Timing signals are provided by a system clock (not shown) through the latch 22. In practice, the clock rate should be at least (N+1) times the output signal rate. In the preferred embodiment, switches 0-4 are implemented with n-channel MOSFET devices. Switches 5 and 6 are implemented with p-channel devices.
The operation of the circuits of
On the trailing edge of input pulse, a discharge cycle is initiated by when the switches are momentarily closed in reverse order. Thus, switch N is opened and switch N−1 is closed. Then switch N−1 is opened and switch N−2 is closed and etc. On the closure of switch N−1, the associated tank capacitor will receive most of the charge on the load capacitance. Each capacitor down the line will receive a lower charge than the immediately proceeding capacitor. After switch 1 opens, switch 0 closes to complete the cycle dumping the remaining charge on the load CL to ground. Thus, over several cycles the tank capacitors will approach their steady state voltages, for example, the (N−1) th through 1st tank capacitors may have charges of say 5, 4, 3, 2 and 1 volts respectively. Then, at the beginning of the next cycle, on the closure of the first switch, the voltage on the first tank capacitor is applied to the load, then the voltage on the second capacitor is applied to the load and so on. Thus, in the example, first 1 volt is applied to the load, then 2 volts, then three volts and etc. As a result, the voltage on the load will gradually increase as shown in FIG. 5(j).
The circuits of
q=CLV/N [4]
Since the tank capacitors are much larger than the load, the tank voltages do not change significantly, so the dissipation in the switches will be the same as for the case in
The voltages of the tank capacitor bank are self-stabilizing. To appreciate this, assume that the voltage of one of the tank capacitors is slightly higher than it should be. Then, the charge delivered by this tank capacitor during the charging of the load will be somewhat larger than that given by equation [4], since the “step” from the voltage below is now slightly larger. During the discharge phase, the step from the voltage above is slightly smaller and the charge received is therefore smaller as well. Therefore, over the full cycle, a net decrease of the charge on the storage capacitor occurs, which causes a decrease in the capacitor voltage. The initial deviance is automatically counteracted.
Even if the tank capacitor voltages differ from the “correct” values, the circuit will work logically correctly, since each charging (discharging) cycle ends by connecting the load to he supply rail (ground). Voltage deviations simply bring higher dissipation. This happens during start-up, before the tank voltages have had time to converge to the even distribution between the supply voltage and ground.
The implementation cost of a driver such as that shown in
The problem of maintaining the appropriate voltages on the tank capacitors is obviated by the fact that the capacitor voltages will converge automatically to the desired voltages. No additional circuitry is required. Only one supply line must be routed to the chip and the power supply need not be any more complicated than a conventional supply. In practice, the tank capacitors would be located off-chip.
For a CMOS implementation, the following design procedure may be followed to provide a driver configuration which exhibits minimal power dissipation.
Equation [3] indicates that dissipation decreases monotonically with increasing N. The number N cannot, however, be usefully made arbitrarily large because each step requires that a switch be turned on and off, which itself causes dissipation. Also, the energy used to drive each switch depends on the width of the device, which should be just enough to allow the charging to complete before the next step commences. Thus, for a given total allowable charging time ‘T’, there is an optimal number of steps and a set of optimal device sizes which lead to minimal total dissipation determined as follows.
Again, consider the circuit in FIG. 3 and assume the gates of the switch devices are driven conventionally. The load is charged and discharged once; the energy needed to drive the gates of the switch devices is:
Allot each step one Nth of the total charging time T. Then:
T/N=mRiCL [6]
Here, m is the number of RC time constants spent waiting for each charging step to complete. From equation [6], it is evident that all the switch devices should have equal on-resistance: Ri=Rsw. Decreasing the on-resistance of device i by increasing the width means increasing the gate capacitance:
RiCi=ρi [7]
ρi is a quality measure of the switch. It varies with i, since the bulk-to-channel and gate-to-channel voltages are different for different switches. Combining equations [5], [6], and [7] yields:
Introducing
If N is sufficiently large,
The number N that minimizes Etot is given by:
The corresponding energy dissipation is:
It remains to select the value for m. If it is chosen too small, there will still be a significant voltage across a switch when the next switch is to close. Hence, there is an increase in the average voltage across each switch and therefore a dissipation increase (the first term in equation [10] is changed slightly). If on the other hand, m is chosen unnecessarily large, time is wasted that could have been used to increase the number of steps. Thus, in general, optimization methods for the value of m vary according to the application, however, one skilled in the art will be able to select a suitable value for m using conventional teachings (e.g., a simulation program).
By using the number of stages given by equation [10], the designer can minimize the power dissipation of the driver. The minimum is rather shallow, however, so a lower N (as would most often be dictated by practical considerations) will still give a considerable improvement over the conventional case; N=2 already gives almost 50% reduction. Once N and m have been selected, the on-resistance of each switch is given by equation [6]. The corresponding gate capacitance, and thereby the width of the device, is given by equation [7]. The values of ρ for a certain process can be found by circuit simulation or by measuring the on-resistances of test devices of known widths.
Thus, the present invention has been described herein with reference to a particular embodiment for a particular application. Those having ordinary skill in the art and access to the present teachings will recognize additional modifications applications and embodiments within the scope thereof. For example, the switches may be closed in some other sequence as may be appropriate for a given application without departing from the scope of the present invention. In addition, alternative circuit topologies for the network of tank capacitors and switches may be appropriate. The second terminal of the load may be connected to a potentially variable) voltage other than ground.
It is therefore intended by the appended claims to cover any and all such applications, modifications and embodiments within the scope of the present invention.
Accordingly,
Athas, William C., Koller, Jeffrey G., Svensson, Lars G.
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Jun 08 1998 | KOLLER, JEFFREY G | University of Southern California | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 025174 | /0247 | |
Jun 09 1998 | SVENSSON, LARS | University of Southern California | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 025174 | /0247 | |
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