This invention relates to electronic protection systems, in particular for lighting systems.
LED and other light sources are typically sensitive to high current or voltage. Excessive electricity can overheat or otherwise damage them.
Some protection circuits put a resistor in series with a lamp load. This prevents externally applied power from overdriving the lamp circuit, but consumes power that could otherwise produce light.
Yet other protection circuits act as an “all or nothing” safeguard, as with opening a fuse or a relay. These safeguards either allow all voltage and current to pass through to the load, or completely shut off the load in case of excess voltage or amperage. Some protection systems do not allow lights to go on again until a fuse is replaced or a circuit breaker is reset. Thus a customer may literally be left in the dark from an excess voltage or current situation.
A need exists for a circuit that provides at least some light output in an electrically overdriven condition, without consuming excess power or producing waste heat.
The present invention meets this need through efficiently protecting a lighting system, while allowing some light output in a protection mode.
The waveform 351 in
Still, nothing limits overall current draw if applied voltage exceeds nominal AC peak voltage, for example 170 volts.
This type of direct drive circuit does not use a power transformer between the AC mains and the LEDs. This configuration has many advantages, including power efficiency and reduction in materials cost and weight. However at least one disadvantage exists in not using a power transformer to couple the mains electricity to the lighting system. For example, any mains power electrical surge will meet with one less intermediate circuit element to limit current and voltage reaching the lights.
To protect a direct drive lighting circuit without the bulk and weight of a power transformer, the present disclosure provides other means of surge and overvoltage protection. The disclosed inventive protection circuit uses semiconductors to efficiently limit the amount of power transfer during overvoltage conditions.
Here is a theory of operation. Diode bridge D1 rectifies externally supplied AC source voltage to provide a rectified voltage waveform 452 that is applied to the protection block 420. A symbolic AC source 403 is shown separately.
Within block 420, below a voltage protection threshold, the series combination of R1, R2, and ZD2 will keep Q2 turned on. This allows Q2 to pass current to the lighting system under normal conditions, below an over voltage threshold.
A voltage protection threshold results from a pathway of the rectified output from rectifier bridge D1 being passed through Zener diode ZD1 and the voltage divider comprised of R3 and R4. Above a certain applied voltage output 452 from the bridge rectifier D1, the Q1 base to emitter voltage will reach approximately 0.7 volts, thus turning on Q1. This will in turn reduce the gate to source voltage on Q2, consequently reducing current flow through block 420.
Methods for determining switch on and switch off threshold voltages for a combination of diodes, transistors, and passive components are well known in the art.
Other detail is that having a combination of R1 and R2 instead of just one resistor is to reduce the voltage drop per resistor. C1 retains charge from times when cyclic voltage 452 is high to keep Q2 turned on when the voltage 452 is near zero.
In summary, with excessive applied voltage from the AC source 403, the Zener diode ZD1 turns on, passing current to turn on transistor Q1. Turning on Q1 reduces the Q2 gate to source voltage, causing less conduction through Q2. The rectified voltage 452 and hence supply voltage 403 will therefore effectively be disconnected from the lighting system 450 under excessive voltage conditions.
Beneficially, this arrangement prevents the disadvantage of completely turning off the LEDs through the entire conduction cycle. Some current can still pass through to the LEDs at the low voltage regions of the conduction cycle. A sequence of oscilloscope screen captures show the behavior given different applied voltage amplitudes.
The oscilloscope trace 501 in
As the voltage increases, the Toff duration increases and the LEDS receive less power through the conduction cycle. Thus some light output occurs without damaging the IC and lamp load. This situation is shown in oscilloscope trace 541
Though the above descriptions may imply a sharp turnoff voltage threshold, this need not be the case for the protection circuit to be effective. An effective protection results when the output current is substantially reduced above an input voltage threshold, substantially here meaning that the current through the load is reduced to a safe level compared to what it would be without the protection circuit.
To further generalize the circuit behavior,
While the circuit implementation shows a particular arrangement of bipolar and FET transistors, substitution of other transistor types in place of those shown is expected to produce substantially the same results. Also the polarity of each element could be reversed without substantially changing the operation of the circuit.
Further, the dividing line between the voltage threshold detector and the device responsive to the detector is subject to interpretation. For example, the boundary could be drawn as in the circuit partition 701 of
Further a pathway between the input voltage detection circuitry and the output current control device could be through an optoisolator instead of direct electrical connection.
Overall, the protection circuit provides an advantage over previous prior art systems that shut down completely well before reaching twice nominal input voltage. Though it performs better than prior art, its range to allow some light output has limitations. Were applied voltage to exceed well over twice mains voltage, there would be substantial power shutdown over the entire AC cycle, as Toff duration increases to fit nearly the entire cycle time. However the circuit could withstand moderate overvoltage without damage to the lighting load, and the circuit would automatically recover.
Because the design shuts off current for at least part of the power cycle during excessive voltage input, this may result in noticeable flicker at the light output. One way to reduce this is to position LED strings so that those with the shortest ON duty cycle are close to those with the longest duty cycle. Also, at least one capacitor in parallel with at least one LED string may reduce noticeable flicker.
It would be reasonable to use the protection circuit in conjunction with other lighting systems supplied by a pulsed or rectified time varying waveform. This could include LEDs in series with a resistor, or even an incandescent bulb.
Whether alone or in combination with a parallel transient protection system, the direct drive protection system effectively prevents lighting circuit damage, while allowing some light output where other protection systems don't, and without wasting electricity.
This application claims the benefit, under 35 USC sections 119 and 120, of the filing date of a current pending U.S. Provisional Application Ser. No. 62/865,286, filed on Jun. 23, 2019, entitled, “DIRECT DRIVE LIGHTING PROTECTION CIRCUIT”, the entirety of which is incorporated by reference herein and priority of which is claimed herein.
| Number | Date | Country | |
|---|---|---|---|
| 62865286 | Jun 2019 | US |