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Reference: JC's posts "Another Idea" 2 Jan 02
JC describes a system for using energy recovered from the flyback pulse to "jump-start" the transmit pulse, allowing improved efficiency and increasing sensitivity to high-conductivity and iron objects.
Here is a different topology for accomplishing the same thing. Sorry, I don't have the ability to publish a drawn schematic, so this will have to be done awkwardly with words. Voltages, component types, etc. are given for the purpose of illustration, and it will be evident to those skilled in the art that the invention comprises a particular operating principle and is not constrained to the details given here for convenience in explanation.
This implementation uses three diodes.
BASIC TRANSMIT DRIVE ARCHITECTURE
The power supply is +12 volts. This voltage is switched with a PNP transistor to the coil, the other end of which is grounded. Therefore, the transmit voltage is positive and the flyback is negative.
For reasons which will become apparent later, a first diode is wired in series with the collector of the transistor, the cathode of the diode being connected to the coil.
BASIC FLYBACK ARCHITECTURE
The hot side of the coil goes to the cathode of a catch diode (the second diode), which stores the energy on the negative end of a capacitor. The positive end of the capacitor is wired in series with a third diode the anode of which goes to the +12 supply. The purpose for the third diode will be explained later.
For the sake of illustration, we'll say that the voltage on the negative end of the capacitor is -100 volts. The actual voltage will depend on a variety of other variables, particularly the electrical Q of the coil, and the ratio of transmit jump-start time to total transmit on-time.
BASIC CHARGE PUMP ARCHITECTURE
A PNP transistor is wired with the emitter to +12 volts, and the collector to the negative end of the capacitor.
When it is time to begin the transmit pulse, this transistor is turned on. The negative end of the capacitor goes to +12 volts and the positive end goes to +112 volts. The third diode is now reverse biased, which leaves the positive end of the capacitor floating.
THE JUMP-START CIRCUIT
A PNP transistor is connected with its emitter going to the positive end of the capacitor and its collector to the hot side of the coil. If base current is furnished, the transistor will be switched on, pulling the hot end of the coil up to +112 volts. The first diode prevents the main transmit transistor from being subjected to reverse voltage.
One way to turn the jump-start transistor on is to wire a biasing resistor from the +12 supply to its base. When the emitter goes up to +112 volts, the bias circuit will turn on. If this proves to be too slow, a capacitor can be wired in parallel with the resistor.
TERMINATION OF THE JUMP-START PULSE
To terminate the jump-start pulse and begin the main transmit-on period, first the main transmit transistor is turned on (timing not critical), and then the charge pump transistor is turned off.
When the charge pump transistor which had been shorting out the negative end of the capacitor to the +12 rail is turned off, the negative end of the capacitor is left floating. Current can no longer flow through the capacitor, turning off the jump-start transistor. Without the jump-start transistor being turned on, the voltage on the coil collapses until the first diode is forward biased, clamping the coil voltage at approximately +11 volts.
The main transmit drive transistor is kept turned on until it is turned off in order to initiate flyback.
FLYBACK VOLTAGE
In a given design, the flyback voltage can be regulated by varying the on-time of the charge pump transistor. Long on-time will give low voltage; short on-time will give high voltage.
Alternatively it could be regulated with an avalanche diode wired across the capacitor; however, this sacrifices some of the energy efficiency benefits of the design.
COMPARISON WITH JC'S METHOD
The circuit complexity is about the same either way, when you include the base/gate drive need to time the jump-start transistor in JC's design. Efficiency is also about the same.
The choice between one or the other probably comes down to the following factors:
1. Compatibility with other aspects of the design, for instance receiver circuitry, or constant-current regulation circuitry.
2. Whether or not the designer likes charge pumps.
3. Whether or not the designer dislikes high-side transistor base/gate drive circuits.
4. As fully implemented, comparing two otherwise equivalent designs, one may be more economical than the other.
5. As fully implemented, comparing two otherwise generally similar designs, one may be faster than the other.
6. It may be that one design is more compatible with MOSFETS than the other, and that the designer prefers MOSFETS. (or vice versa, and bipolars.)
--Dave J.
JC describes a system for using energy recovered from the flyback pulse to "jump-start" the transmit pulse, allowing improved efficiency and increasing sensitivity to high-conductivity and iron objects.
Here is a different topology for accomplishing the same thing. Sorry, I don't have the ability to publish a drawn schematic, so this will have to be done awkwardly with words. Voltages, component types, etc. are given for the purpose of illustration, and it will be evident to those skilled in the art that the invention comprises a particular operating principle and is not constrained to the details given here for convenience in explanation.
This implementation uses three diodes.
BASIC TRANSMIT DRIVE ARCHITECTURE
The power supply is +12 volts. This voltage is switched with a PNP transistor to the coil, the other end of which is grounded. Therefore, the transmit voltage is positive and the flyback is negative.
For reasons which will become apparent later, a first diode is wired in series with the collector of the transistor, the cathode of the diode being connected to the coil.
BASIC FLYBACK ARCHITECTURE
The hot side of the coil goes to the cathode of a catch diode (the second diode), which stores the energy on the negative end of a capacitor. The positive end of the capacitor is wired in series with a third diode the anode of which goes to the +12 supply. The purpose for the third diode will be explained later.
For the sake of illustration, we'll say that the voltage on the negative end of the capacitor is -100 volts. The actual voltage will depend on a variety of other variables, particularly the electrical Q of the coil, and the ratio of transmit jump-start time to total transmit on-time.
BASIC CHARGE PUMP ARCHITECTURE
A PNP transistor is wired with the emitter to +12 volts, and the collector to the negative end of the capacitor.
When it is time to begin the transmit pulse, this transistor is turned on. The negative end of the capacitor goes to +12 volts and the positive end goes to +112 volts. The third diode is now reverse biased, which leaves the positive end of the capacitor floating.
THE JUMP-START CIRCUIT
A PNP transistor is connected with its emitter going to the positive end of the capacitor and its collector to the hot side of the coil. If base current is furnished, the transistor will be switched on, pulling the hot end of the coil up to +112 volts. The first diode prevents the main transmit transistor from being subjected to reverse voltage.
One way to turn the jump-start transistor on is to wire a biasing resistor from the +12 supply to its base. When the emitter goes up to +112 volts, the bias circuit will turn on. If this proves to be too slow, a capacitor can be wired in parallel with the resistor.
TERMINATION OF THE JUMP-START PULSE
To terminate the jump-start pulse and begin the main transmit-on period, first the main transmit transistor is turned on (timing not critical), and then the charge pump transistor is turned off.
When the charge pump transistor which had been shorting out the negative end of the capacitor to the +12 rail is turned off, the negative end of the capacitor is left floating. Current can no longer flow through the capacitor, turning off the jump-start transistor. Without the jump-start transistor being turned on, the voltage on the coil collapses until the first diode is forward biased, clamping the coil voltage at approximately +11 volts.
The main transmit drive transistor is kept turned on until it is turned off in order to initiate flyback.
FLYBACK VOLTAGE
In a given design, the flyback voltage can be regulated by varying the on-time of the charge pump transistor. Long on-time will give low voltage; short on-time will give high voltage.
Alternatively it could be regulated with an avalanche diode wired across the capacitor; however, this sacrifices some of the energy efficiency benefits of the design.
COMPARISON WITH JC'S METHOD
The circuit complexity is about the same either way, when you include the base/gate drive need to time the jump-start transistor in JC's design. Efficiency is also about the same.
The choice between one or the other probably comes down to the following factors:
1. Compatibility with other aspects of the design, for instance receiver circuitry, or constant-current regulation circuitry.
2. Whether or not the designer likes charge pumps.
3. Whether or not the designer dislikes high-side transistor base/gate drive circuits.
4. As fully implemented, comparing two otherwise equivalent designs, one may be more economical than the other.
5. As fully implemented, comparing two otherwise generally similar designs, one may be faster than the other.
6. It may be that one design is more compatible with MOSFETS than the other, and that the designer prefers MOSFETS. (or vice versa, and bipolars.)
--Dave J.