Zero Volt Diode
From BEAM Robotics Wiki
- A term used when referring to a novel circuit in which a power MOSFET acts like a very low voltage drop diode that switches state at 0V and which is used to conduct negative current from drain to source.
The following article cannot be edited. It was Wilf Rigter, and as such represents an important historic and technical BEAM reference.to the (see: ) by
The Zero Volt Diode (ZVD) is a circuit useful in a variety of applications including solar chargers of all types. It is a novel circuit in which a power MOSFET acts like a very low voltage drop diode that switches state at 0V and which is used to conduct negative current from drain to source.
In D1 type solar engines, a low loss diode can be used to charge a cap to the open circuit voltage of the solar cell and used in solar battery chargers, the battery is charged at the maximum rate when the source voltage is highest. The diode must be used in series with the solar panel or else the cap or battery would discharge through the solar panel when the panel voltage drops below the stored voltage.
Most diodes used in BEAM SEs and solar chargers are Silicon diodes like the 1N4001 which have a voltage drop of 0.6V to 1V at currents up to 1A. More efficient diodes for currents form >100mA to tens of amps applications are the Schottky type rectifiers with a voltage drop of from 200mV to 1000mV depending on the current level. For <100mA applications a Germanium diode can used with 200mV or less drop.
This voltage drop issue is important in competition solar engines since you would like to have the maximum voltage to charge the cap and supply the load (low diode drop) and keep the charge stored on the cap when the lightlevel drops (leakage current cut off) and the SE triggers. Moreover, since the energy in the cap is proportional to the square of the voltage even the small voltage drop of a diode reduces available energy.
The solution is to use a MOSFET as a rectifier just like the synchronous rectifier applications in voltage converters. The MOSFET should be switched ON when the solar voltage is larger than the capacitor or battery] voltage and switch OFF when the solar voltage is lower than the stored voltage.
Here is a little design for charging capacitors from solar cells with zero voltage drop at the end of the charge cycle. It can be easily scaled to higher currents by changing the 2N7000 for a larger MOSFET. If a parallel load is present, the circuit also delivers maximum voltage with minimum insertion loss from the solar cell. The MOSFET turns on when the voltage difference is zero and turns off when the solar voltage drops less than 100mV below the cap or battery.
The NPN transistor is normally ON when the cap voltage is more than .6V and this clamps the gate of the 2N7000 which is turned OFF. The PNP transistor is connected to the negative terminal of the solar panel and when the voltage on that terminal drops below 0V the PNP turns ON. This in turn turns the NPN OFF and the 2N7000 turns ON. MOSFETs have an interesting characteristic in that they act like bi-directional switches, so the 2N7000 is perfectly happy to have it's drain conduct a negative current to the 0V line. When the voltage on the negative terminal of the solar panel is more positive than 0V the PNP turns OFF and the NPN ON and the 2N7000 turns off with the drain voltage positive with respect to the source voltage and 0V line. Since the 2N7000 does not turn on until the gate voltage is more than 2V (in practice: higher according to the data book) a logic FET with a lower gate turn on voltage would be preferred. In any case the MOSFET has a integral reverse diode from drain to source which will carry the current until the voltage on the cap reaches 2V at which point the MOSFET turns on and the forward voltage drops to a few 10s of mV.
Anyway it's a start to revisit some of the more primitive solar circuits and get the technological edge on your competitors in the solar races!
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