Here is a totally different take on the Joule Thief (JT) circuit commonly found in garden lights. Instead of charging a 1.2v battery directly from the solar cell and converting the power to run a 3-volt LED, we'll be using the JT to convert the output from the solar cell and charging a Lithium battery first. Then when night falls, the battery is used to drive the LED directly.
This method has some advantages: (1) the Lithium cell that was chosen here (and avialable for $2 here) has an output of 3-volts, which can drive a White LED directly; it also has a huge capacity (800mAH) and very low leakage. (2) The solar cell normally can only charge the NiCd battery in full, direct sunlight, but, with the JT circuit, it is able to deliver power to the Lithium cell even on overcast days.
Step 1: The 'Reversed' layout.
Besides reversing the charge / discharge order, this circuit also reverses the location of the driver transistor and the coil, but wait, that's not all! The transistors all have reversed polarities, and even the output voltage is reversed!
No, it isn't an error! Diode D1, the LEDs and the charged battery all have their polarities reversed! That's because this Joule Thief is configured as a voltage inverter. This arrangement was chosen due to its advantages for this kind of application.
To improve efficiency, the traditional JT relies on a fairly constant battery supply (over a millisecond or so) to give it a boost when it is delivering power. With the limited output from a Solar Cell, we have to store all its power in C2 and feed it into the Lithium in one big pulse, meaning the capacitor will be "empty" for the few critical millisecond, cancelling the 'kick' the normal JT requires to work well.
Our 'Reversed' JT circuit will work as a regular JT - without the 3v Lithium load, an input of 1.2v will light up the LEDs quite nicely. Not strictly necessary, the LEDs are there so you can SEE the system working, and also to prevent the battery overcharging.
Step 2: The Light
Switch S2 is optional and allows you to run the LED at full power, otherwise R2 will only allow 20mA to the LED.
The second picture shows the two halves of the circuit together.
Step 3: Parts List
Solar Cell. 2-volts with 100-ohm load
Q1,Q3 BC327 PNP. Can be any low-signal amp of sufficient current rating (>100mA)
Q2 BC337 NPN. Most will work but if you change Q1, Q2 or L1, you may need to adjust R1 for best performance (Try 3.3k to 15k)
D1 1N4148 or 1N914 or similar
LED1 Blue or White LED
LED2 Red LED
LED3 100mA (1/2W) White LED
C1 220pF. Can be 150-500pF
C2 50-200uF
R1 10k-ohm
R2 330-ohm (use 470-ohm for longer run time)
R3 3.3k-ohm
R4 6.8k-ohm (use these values instead of the one on the schematic)
R5 100-ohm. Go as high as 220-ohm for lower brightness.
L1 100-500uH. Many home-made ones will work.
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The second image shows the waveform measured at the top of the coil. The portion above the tag (2) is the charge stored in C2 fed into the coil. The sharp negative going pulseis the battery being charged.
Step 4: Testing the Solar Cell
A simple test is to take them out on a sunny day and measure their output with a Voltmeter that has 100-ohm resitor across the + and - leads. This puts a load on the Solar Cell and will give you some idea of how 'powerful' it is.
In this picture, the meter shows almost 2 volts in a slight shade. Using Ohm's law, we know that 20mA (2-volt / 100-ohms) is also flowing from the cell, and this is the values we will use to design our circuit.
Step 5: Some Calculations
Using the numbers of 2-volt and 20mA from before, we now know that we can get 40milli-watts by multiplying Volt with Amp. Over the course of an 8-hour sunny day, we should be able to get 320mWH of power from our system.
With a 100mA LED running full steam, it will draw (3.3-volt x 100mA), or 330 milli-Watts! Divide this number into the 320mWH we get from sun-power, it means we'll use it up in less than an hour! Of course the battery will continue to supply current from its reserve, but that is power that would require extra days to replenish.














































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I have some 180 uH inductors that I've used in similar JT circuits -- their DC resistance is probably lower than this one. I've found that it helps to boost the output by putting two in parallel which decreases the DC resistance. Thanks.
Power is proportional to I2 * R so, with any given inductor, the power loss is four times higher for every doubling of the current. Thus to get 3v from 0.5 v, the current draw will be at least 6x, making the losses 36 times higher. Also, getting the proper bias for any semiconductor unit at these voltages will be problematic, to say the least.
Jim
Here you will find a "Joule Thief" circuit that is new and so simple that you may not have to worry about a PCB board...
You can design your own PC board with ExpressPCB which is free software you download. When you have done a design, you submit it to their website, where they bill your CC and it is made and shipped to you. Three PCBs cost about $65.00. ExpressPCB also has ExpressSCH which lets you draw schematics and export them as a .bmp file. It's true that you have to learn to use the prog but it gives you total freedom to make exactly what you want.
http://rustybolt.info/wordpress/?p=65
The idea of a zener is a good one. In fact that is what's being done in an adaptation of this circuit used in an MIT project in rural Africa, you can read more here.
A LiFEPO battery has a nominal cell voltage of 3.0V, and an open-cell, fully-charged voltage of around 3.6, as compared to Li-Ion which is typically 3.7 and 4.2 for those conditions. It also has about half the capacity of the Li-Ion batteries, but on the plus side it's a lot cheaper, more rugged and has much longer life (it may last 1000 cycles under circumstances where Li-Ion would only last 200).
So your 3.3V maximum charge voltage is a good maximum, since at that voltage the LiFEPO battery is really nearly fully charged. Don't increase the maximum voltage any more on that battery; although LiFEPO is less likely to behave catastrophically than Li-Ion, you really just don't want to abuse lithium batteries.
that would be 2ma
Just the other day I bought a solar lamp at the hardware store for $3.50 bucks. I bought it just so I could rip it apart. Blows me away - only $3.50.
I'm guessing there is no reason I couldn't use a pair of 1.2V NiMH instead of the Lithium cell. I've got a bunch of 2500mA.hr AA cells.
I'm hoping to keep a Zigbee radio running instead of the LED. The radio uses 200uA while sleeping. When transmitting / receiving the current jump up to 35mA. However, the active time is only for a few seconds. The radio then goes to sleep for a programmed amount of time (15 minutes).
OK, my question, is there anything special about the inductor? Will any old 200uH inductor work? I found a couple at digikey - here is an example: http://search.digikey.com/scripts/DkSearch/dksus.dll?Detail&name=237-1173-ND
I had a hard time seeing your inductor in your pics. Could you put a lasso around the inductor to call it out?
Thanks again for a great instructable.
The combination of the Red and White LEDs is to limit the voltage for 3.6v Lithiums and NiCd packs. Combine different LEDs and diodes for LED1 and LED2 to get regulation for different voltages.
I'm not sure I understand your comment about using the LEDs / diodes for regulation. If there were no LEDs or diodes would the circuit simply keep the 3V battery trickle charged? After becoming fully charged, the battery would simply waste the extra energy by becoming warm.
My Zigbee radio can handle 2 to 3.6 volts. So, if anything, maybe just a 3.6V zener diode to clamp the output from ever going over 3.6V. You see, in my application, I don't want to share any energy with an LED.
Does that make sense?
Thanks again,
Jim
I had the LEDs in as a precaution, since back-EMF can pop the transistors and then found myself 'tuning' the circuit (via R1 & C1) by watching how brightly they glowed. I guess a zener there will do a better job, but I DO like my lights!
In traditional JT circuits where 2 coils are used, it does become a whole lot more critical - as anyone who's tried to power up a 1-watt LED from an AA (and a single transistor) will readily attest to.
You're right in that the inductor determines the frequency - but it also affects the duty cycle which affects brightness and efficiency.
Here's a ROUGH English version of the web page courtesy of Microsoft Translator:
Tung Tai Shing electronics
Professional IC IC, Triodes ....
Solar lawn lights LED driver IC QX52521F TO-94 applies to section battery programme originally proxy, long-term supply ...
Overview
QX52521 is a specially designed for solar-powered LED lighting design of ASIC. It consists of switching driver circuits, light switches, circuit, over-discharge protection circuit, internal integrated Schottky diodes, etc. Only one external inductance can be composed of the solar light fixtures. QX52521 uses patented technology to enable undervoltage shutdown when the LED lights flicker-free.
Features
Working voltage: 0.9V-1.5V
Output current: 3mA-100mA
Patent over discharge protection: turn-off flicker-free
Built-in integrated optically controlled switch
Internal Schottky Diode
External components only need an inductance
High efficiency
TO-94, DIP-8 package
Welcome to contact us ...It should be usable by attaching the solar cell to the battery inputs, and the lithium through a diode (extra) on the output side.
Here is a *ROUGH* translation of the webpage courtesy of Microsoft Translator:
Tung Tai Shing electronics
Professional IC IC, Triodes ....
Solar lawn lights LED driver IC QX52521F TO-94 applies to section battery programme originally proxy, long-term supply ...
Overview
QX52521 is a specially designed for solar-powered LED lighting design of ASIC. It consists of switching driver circuits, light switches, circuit, over-discharge protection circuit, internal integrated Schottky diodes, etc. Only one external inductance can be composed of the solar light fixtures. QX52521 uses patented technology to enable undervoltage shutdown when the LED lights flicker-free.
Features
Working voltage: 0.9V-1.5V
Output current: 3mA-100mA
Patent over discharge protection: turn-off flicker-free
Built-in integrated optically controlled switch
Internal Schottky Diode
External components only need an inductance
High efficiency
TO-94, DIP-8 package
Welcome to contact us ...
A possible hack is to remove the ground connection of the zener and route that to the "Solar+" pin through a 1k resistor. This would 'fool' the device into turning itself off when the battery is fully charged.
Sorry for the image quality - I used an iPad to draw the diagram.
If it is the first, then larger inductors tend to have lower DC resistance (thicker wires) and higher saturation point, which help in the efficiency.
The value of the inductor changes (inversely) the operating frequency and possibly the duty ratio. In general, larger inductances put less stress on the drivers but will require more turns of wire, which means higher resistance. It is usually recommended to use the lowest inductance / highest frequency, subject to the components' operating limits and watching out for possible interference to radios and TV.