Joule thief

A generic, conventional joule thief, shows parts and how they are wired together. The example uses a red LED. A ferrite toroid is wound to form a coil with primary (white) and feedback (green) windings. A PN2222A transistor and 1000 ohm resistor are used.

A joule thief is a minimalist self-oscillating voltage booster that is small, low-cost, and easy to build; typically used for driving light loads. It can use nearly all of the energy in a single-cell electric battery, even far below the voltage where other circuits consider the battery fully discharged (or "dead"). Hence the name suggests the notion that the circuit is stealing energy or "joules" from the source. The term is a pun on the expression "jewel thief", one who steals jewelry or gemstones.

The circuit uses the self-oscillating properties of the blocking oscillator, to form an unregulated voltage boost converter. As with all power conversion technology, no energy is actually created by the circuit (in accordance with the law of conservation of energy). Instead, the output voltage is increased at the expense of higher current draw on the input. As a result, the amount of power entering the circuit is the same as the amount leaving, plus the losses in the conversion process.

History

In the "Ingenuity Unlimited" section (readers' ideas) of the November 1999 issue of Everyday Practical Electronics (EPE), page 804, Z. Kaparnik from Swindon published a simple circuit entitled "Micro-torch Circuit". The circuit consisted of a transformer-feedback single-transistor voltage converter based on the blocking oscillator, which originally used a vacuum tube / thermionic valve and dates prior to World War II. The name "Joule Thief" was coined by Clive Mitchell ^[1] and given to his variant of Kaparnik's circuit which consisted of a single cell, a single BC549 NPN transistor, a coil with two windings, a single resistor (typically 1000 ohms), and a single white LED. The name caught on, became popular, and since then others have borrowed the Joule Thief name and applied it to other circuits. However, those circuits are not true Joule Thief circuits.

Description of operation

Example of a joule thief circuit driving a LED. The coil consists of a standard ferrite toroid core with two windings of 20 turns each using 0.15 mm (0.006 inch) diameter wire (38 swg) (34-35 AWG). The circuit can utilize an input voltage down to about 0.35 V and can run for weeks using a 1.5 V LR6/AA. The battery voltage is usually 1.5 V. The resistor is ~1 kΩ, 1/4 W. The transistor could be a 2N3904, BC547B, 2SC2500, BC337, PN2222, 2N4401 or other NPN. V_ceo = 30 V, P = 0.625 W. A white light-emitting diode with V_f = 3.2 V might be used.^[1]

The circuit works by rapidly switching the transistor. Initially, current begins to flow through the resistor, secondary winding, and base-emitter junction (see diagram), which causes the transistor to begin conducting collector current through the primary winding. Since the two windings are connected in opposing directions, this induces a voltage in the secondary winding which is positive (due to the winding polarity, see dot convention) which turns the transistor on harder. This self-stoking/positive-feedback process almost instantly turns the transistor on as hard as possible (putting it in the saturation region), making the collector-emitter path look like essentially a closed switch (since V_CE will be only about 0.1 volts, assuming that the base current is high enough). With the primary winding effectively across the battery, the current increases at a rate proportional to the supply voltage divided by the inductance. Switch-off of the transistor takes place by different mechanisms dependent upon supply voltage.

The predominant mode of operation relies on the non-linearity of the inductor (this does not apply to air core coils). As the current ramps up it reaches a point, dependent upon the material and geometry of the core, where the ferrite saturates (the core may be made of material other than ferrite). The resulting magnetic field stops increasing and the current in the secondary winding is lost, depriving the transistor of base drive and the transistor starts to turn off. The magnetic field starts to collapse, driving current in the coil into the light emitting diode (raising the voltage until conduction occurs) and the reducing magnetic field induces a reverse current in the secondary, turning the transistor hard off.

At lower supply voltages a different mode of operation takes over: The gain of a transistor is not linear with V_CE. At low supply voltages (typically 0.75V and below) the transistor requires a larger base current to maintain saturation as the collector current increases. Hence, when it reaches a critical collector current, the base drive available becomes insufficient and the transistor starts to pinch off and the previously described positive feedback action occurs turning it hard off.

To summarize, once the current in the coils stops increasing for any reason, the transistor goes into the cutoff region (and opens the collector-emitter "switch"). The magnetic field collapses, inducing however much voltage is necessary to make the load conduct, or for the secondary-winding current to find some other path.

When the field is back to zero, the whole sequence repeats; with the battery ramping-up the primary-winding current until the transistor switches on.

If the load on the circuit is very small the rate of rise and ultimate voltage at the collector is limited only by stray capacitances, and may rise to more than 100 times the supply voltage. For this reason, it is imperative that a load is always connected so that the transistor is not damaged. Note that, because V_CE is mirrored back to the secondary, failure of the transistor due to a small load will occur through the reverse V_BE limit for the transistor being exceeded (this occurs at a much lower value than V_CEmax).

The transistor dissipates very little energy, even at high oscillating frequencies, because it spends most of its time in the fully on or fully off state, thus minimizing the switching losses.

The switching frequency in the example circuit opposite is about 50 kHz. The light-emitting diode will blink at this rate, but the persistence of the human eye means that this will not be noticed.^[1]

A simple shunt-regulator for loads requiring a constant voltage

When a more constant output voltage is desired, a voltage regulator can be added to the output of the first schematic. In this example of a simple shunt-regulator, a blocking diode ("D_rect") allows the secondary winding to charge a filter capacitor ("C_filter") but prevents the transistor from discharging the capacitor. A Zener diode ("Z1") is used to limit the maximum output voltage.

Competing systems

US Patent 4,734,658 describes a low voltage driven oscillator circuit, capable of operating from as little as 0.1 volts. This is a far lower voltage than that at which the Joule Thief will operate. This is achieved by using a JFET, which does not require the forward biasing of a PN junction for its operation, because it is used in the depletion mode. In other words, the drain–source already conducts, even when no bias voltage is applied. The '658 patent is intended for use with thermoelectric power sources, which are inherently low voltage devices. One advantage of this system is that old fashioned and hard to source germanium devices are not necessary; a modern silicon JFET works perfectly well. ^[2]

See also

• Flyback converter
• Boost converter

References

External links

• Joule Thief Simulation
• Supercharged Joule Thief Has High Efficiency
• US4734658, Google patents listing for JFET version of Joule Thief
• espacenet.com: CA1303154 - Low voltage driven oscillator circuit, priority date 1987-08-14