High power LEDs:
The recent availability of high-powered
LEDs provide an alternative to Lasers for high intensity light sources
that can be easily modulated. Because the only practical means of
modulating most light sources is through intensity (or "amplitude")
modulation, these modulation schemes invariably the varying of the
current through the LED to achieve the desired modulation.
As with any electrical device, there are some practical current limits
that must be observed in order to avoid destruction of the
device. One of these is excess voltage (from static discharge,
for example) but most high-powered LEDs are rather well protected in
this regard.
Excess current, however is another story.
The Luxeon III LEDs are rated for a (nominal) 3 watts of dissipation,
but some of the devices in the series (the Red, Red-Orange, and Amber)
are actually rated for continuous operation at a bit over 4 watts -
somewhat higher power than the other colors in the Luxeon III product
line.
For the remainder of this discussion, we will be assuming the use
of the Red, Red-Orange, and Amber devices with the higher power
capability.
Given an "infinite" heat sink, the absolute maximum continuous current
permitted for these devices is 1.544 amps with a peak pulse current of
2.2 amps although the parameters of that pulse (e.g. width and duty
cycle) are not noted.
Through testing, I have determined that a properly heatsinked Luxeon
III will probably tolerate
continuous operation at 2.5 amps for a short period (30 seconds or so)
without damage Other experience has shown that at a current of
somewhere between 3 and 8 amps, the bond wire on the negative lead of
the Luxeon will fuse (open) and render the LED inoperable.
Figure 1:
LM317-based current limiter circuit
Click on image for a larger version.

|
Having accidentally made
several Luxeon III's "inoperable" I
decided that all optical modulator will contain circuitry to limit the
current to a value that will be safe enough to protect the LED during
short-term accidents.
A note concerning use with Luxeon I LEDs:
- Red, Red-Orange, and Amber Luxeon I LEDs have a much
lower peak current rating - about 550 mA. At this lower current,
R1 would need to be above 2.5 ohms and R2/R3 would be adjusted
accordingly. If a precise value of R1 (around 2.2 ohms) can be
selected, R2 and R3 can be eliminated and the "adjust" terminal can be
connected directly to the "load" side of R1. This lower
current/voltage also means that the total drop of this circuit will be
in the 3.5-4 volt range at the limiting current.
Current limiting circuitry:
The simplest current
limiter is a series resistor. While simple, its somewhat costly
in
terms of power dissipation and its effectiveness (both in preventing
damage and in allowing normal operation) is somewhat dictated by the
available supply voltage: Too high a value and the LED cannot be
driven to full current. Too low a value and the LED is not
adequately
protected. If the supply voltage is lower or higher than
expected, the
effects are similar.
A solution to this problem is the use of a common 3-terminal voltage
regulator, the LM317. This device is commonly used to regulate
voltages, using a simple resistive divider to set the output voltage,
but it can also be used as a fairly precise current source.
Even though the "official" rating of the LM317 in the "K" (metal TO-3)
or "T" (TO-220 "tabbed) packages is 1.5 amps, it is perfectly capable
of operating at somewhat higher currents than this. One of the
features of the the LM317 is its built-in current limiting. A
quick peek at the data sheet will reveal that its internal current
limit is typically 2.2 amps - but it could be anywhere from 1.5 to 3.5
amps. In testing dozen or so devices from different manufacturers
made over the past two decades or so, I observed that they all
exhibited a current limit in the 2.25-2.75 amp area and none limited at
less than 2 amps when cool.
It is important to note that this "maximum current limit" is only valid
when the device is at room temperature. As the device warms up,
the "thermal protection" begins to take effect, reducing the current
with increasing temperature. I also observed that at "touchable"
temperatures (e.g. temperatures at which one could touch the device for
5 seconds or so before deciding that it was too hot) that the reduction
in the maximum current was minimal: It wasn't until the device
got well above about 150 degrees F (about 65 C) that it really started
to limit its current.
Figure 1 shows such a circuit. This is a
modification of the typical LM317-based current source in that R2 and
R3 have been added, but its operation is the same:
- As the current increases, a voltage appears across R1.
- When the voltage on the "Adjust" terminal is about 1.245 volts
below that of the "Output" terminal, the current is reduced.
Normally, the adjust terminal is connected directly to the "load" side
of R1: When the voltage drop across R1 exceeds about 1.245 volts,
the current reduction occurs. In testing, I built such a circuit,
using only R1, but I found that in order to set the limiting current
within the 2.25-2.5 amp range, I needed a resistor of about 0.6 ohms -
not a common value.
While it would have been possible to synthesize such a resistance by
paralleling resistors, I decided to construct a circuit that used more
common resistor values and
Figure 1 is the result. In
this case, R1 is set for a slightly higher resistance to effect a
higher voltage drop while R2 and R3 divide that voltage such that at
2.25-2.5 amps, the Adjust-to-Output differential is in the 1.245 volt
range.
Figure 2:
Two examples of Luxeon III emitters with current limiters.
Note that these pictures do not include the bypass capacitors C1 and C2.
Click on either image for a larger version.
 |

|
Connected in parallel with this circuit is bypass capacitance. If
the LED is modulated with waveforms that contain high frequency
components (like those in a PWM circuit, high frequency subcarrier, or
video modulation) the bypass capacitance (C1 and C2) allows high
frequency components to pass around the LM317 while still offering
protection to the LED from a DC current fault. The use of two
capacitors is recommended, as the 0.1uF capacitor will be transparent
to the highest frequency components, while the larger electrolytic will
better-pass the lower frequency components. It is recommended
that 105C (high temperature) electrolytics be used - particularly if
the capacitor is exposed to the heat from the LM317.
Total voltage drop of the circuit in
Figure 1 at 2.5 amps is
around 4.5-5.0 volts. This, in series with a Luxeon III LED would
imply that there is a total voltage drop of as much as 7.75-8.25 volts
- but this is still enough headroom for many circuits that operate from
a 12 volt source - but some circuits may need to be modified. As
mentioned before, if R2/R3 are omitted and the Adjust terminal is
connected to the load side of R1, the value of R1 can be reduced to an
experimentally-derived value in the 0.6 ohm area, reducing the voltage
drop at 2.5 amps by a volt or so.
Constructing the circuit:
As can be seen from the pictures in
Figure 2 this circuit can
be constructed in a number of ways. It is essential that the
LM317 have at least some heat sinking. In normal operation, the
average LED current of a Luxeon III will be about 1 amp, peaking to 2
amps or so at 100% positive modulation. Under these conditions,
the LM317 will have to dissipate about 2 watts of heat while R1 will be
dissipating around 1 watt.
Even though this is a fairly small amount of heat, it is important that
this circuit
NOT be mounted on the same heat sink
as the Luxeon! A quick check of the Luxeon's specifications will
show you that is it warms up, its efficiency drops, so it is best not
to add another device that will warm it up. As shown in these
pictures, the LM317 is mounted separately from the Luxeon's heat sink -
preferably off to the side so that convection will not be likely to
cause one heat sink to heat the other.
It worth noting that it is also a good idea
not to excessively
heat sink the LM317. A good example of this is shown in the
bottom circuit of
Figure 2 where the LM317 is simply soldered
to a piece of copper circuit board material. This provides
adequate heat sinking for normal operation where the LM317 is
dissipating about 2 watts. If, however, a fault develops and,
say, a full 12 volts is placed across the LED drive, this will cause
the current to exceed the 2.25-2.5 amp threshold. When this
happens, the voltage drop across the LM317 necessarily increases and
this will dramatically increase the amount of heat being dissipated by
the LM317. In this state, the current will start to drop as the
LM317 gets hot, soon reducing the current to well below the 2.25-2.5
amp threshold. It is under these conditions that a very large
heat sink is less-desirable as it would prevent the LM317 from heating
up and reducing the operating current.
Operational use:
As mentioned before, there must be enough voltage headroom in the power
supply voltage and modulator circuit to accommodate the added voltage
drop of this protection circuit. In the modulators that I have
build, power MOSFETs are used along with 1 ohm current-sense resistors,
adding as much as 2.5 volts of additional drop - but these run will
drive the LED to over 2 amps with an 11.5 volt supply - the voltage of
a discharged lead-acid battery.
Under normal conditions, this circuit is completely transparent:
Other than an addition I*R voltage drop across the sense resistor,
there are no effects at all. When the current exceeds the preset
threshold, however, the LED drive is clipped at that level and could
cause some distortion.
A quick look at the schematic will also reveal that I have placed it in
the "high" side of the LED supply. This was done in the event
that the "low" side of the LED (which, in my case, goes to the
modulator) gets shorted to ground: A high-side current limiter
will still protect the LED in this case.
Note that because this circuit sits inline, there is no real voltage
limit to it aside the voltage differential that would occur under fault
conditions when the LM317 is current-limiting. What this means is
that if you were to run a string, say, 5 Luxeons in series from a
24-36 volt supply, you could: This circuit would happily protect
them all.
Other types of circuits:
Figure 3:
Close-up view of a red Luxeon III emitter. Note the
fine-gauge bond wire that connects to the conductors on top of the
die: It is this wire that fuses if too much current is
run into the LED.
Click on the image for a larger version.

|
When I was deciding how to protect the Luxeon, I was considering other
types of circuits such as comparators driving MOSFETs or other
transistor-based limiter. While these would work - and some have
the advantage of having lower voltage drops - none of them were as
simple as the LM317-based circuit shown here and some of them require
their own supply voltage to operate. This circuit has the
advantage of being cheap, simple, and it need only be placed in series
with the current flow, not needing a ground or voltage reference.
There is also the obvious question as to why not use a fuse? If
you look closely at a Luxeon III emitter (see Figure 3)
you'll note that it already has a fuse disguised as a bond wire
connecting one of the terminals to the center of the emitter die.
If you use an external fuse, it must be one of a lower rating and
faster than that bond wire. Clearly, this rules out slow-blow
fuses as well as thermistor-type PTC fuses. It is also worth
noting that there is quite a difference between the "hold" current of a
fuse and the current at which it will blow quickly, and a current at
which the fuse will fail over a longer period of time - not to mention
a fairly wide range of variability of fuses of the same ratings - even
those from the same manufacturer. Finally, if one uses fuses, it
is imperative that spares be kept onhand.
Final comments:
Despite the voltage drop which is something that can be worked around
in most circuits, usually through a minor change, the described
protection circuit works very well to keep peace of mind - and it could
prevent the sudden, expensive end of testing should some sort of fault
or accident occur that might open up the LED.
Return
to the KA7OEI Optical communications Index page.
If you have questions or comments concerning the contents
of this
page, feel free to contact me using the information at this URL.
This page and contents copyright
2007-2008. Last update: 20081023