There is often confusion about the benefit of a body that is slow to heat up. Some think that the slower transfer of heat means that the heat sink is more efficient. Others contend that the faster the heat gets to the surface of the flashlight, the more effective it is.
The truth is that the name of the game is to keep the LED below the temperature where it breaks down. If the surface of the flashlight is slow to heat then it's because the transfer of heat is slow. It is reasonable to also expect that it's slow to transfer the heat away from the LED.
The slower heat is removed from the LED, the more the temperature rises in the LED.
It is my opinion that the slower the flashlight body heats, the poorer the heat management.
Daniel
In many cases, especially a well designed flashlight, your opinion would be completely wrong.
I will put it into electrical terms as most people understand it better:
- Thermal resistance = electrical resistance
- Thermal capacity (or mass) = electrical capacitance
- Temperature differential = voltage differential
- Temperature = absolute voltage
Any element in a thermal system has both thermal resistance and thermal capacitance.
Let's say you try to dump 2 watts of energy into a small capacitor through a defined resistance. The capacitor will quickly rise in voltage. As the resistance is define, the voltage whatever it may be, will also go up quickly. Now if you have a big capacitor, the voltage on the cap will go up slowly as will the voltage on the other side of the resistor (I fixed power).
Now let's say I attached a 2W dissipating LED directly to a big copper block (or aluminum) ... just a big block. The high thermal mass of the block means that the block will be very slow to rise in temperature. At the same time, the high heat transfer capabilities of the material will work to keep the temperature of the block somewhat homogenous though obviously there will be a differential. After some period of time, the block of metal will hit equilibrium with the heat going into it and the heat being transferred out of it. With the exception of a small differential through the block (it has a high conductivity), the LED temp never gets much higher than the surface temperature.
So let's take a copper (or aluminum) block that is 1/8 the volume (and 1/4 the surface area). The block will heat up much faster until it reaches equilibrium. However, because it has 1/4 the surface area, that equilibrium temperature at the surface w.r.t. room temperature is now 4 times higher. The thermal resistance between the surface of this smaller block and the LED may be 1/2, but since the conductivity of the materials is so high, it make little difference in terms of a thermal differential. Hence in this scenario, the increase in LED temperature will be 4x.
The only thing you can surmise from a hot bodied flashlight is that what is inside is even hotter.
A flashlight body with no fins will heat up much faster (and get much hotter overall), then one with a ton of fins with the end result being a hotter LED during all the operation.
If you "could" make a graphite bodied flashlight (graphite conducts fantastic in the alignment of the strands), then the outside would be hot quicker and the LED would potentially be cooler in equilibrium. However, with very little thermal mass, if you had brief "turbo" modes, during the turbo mode, the LED would be much hotter than an aluminum or copper body that could absorb (like a capacitor) the thermal energy spike.
Thermally enhanced plastics would get hot quicker than aluminum or copper as well, however, due to their low thermal mass and higher thermal resistance, the LED will absolutely be hotter both in transient and equilibrium conditions.
Where a slowly heating body would be a concern would be with materials with a high ratio of thermal mass to thermal resistance. The obvious one is non thermally enhanced plastic bodies. All that happens there is the LED gets really hot, then the interior gets really hot, which make the differential across the plastic body enough to transfer the heat being generated.
The other case is less obvious, titanium flashlights. Titanium on a volume basis has a similar thermal mass to aluminum. On the other hand it is a poor thermal conductor, about 1/7 that of aluminum. Because of that there will be a greater thermal gradient across the material for equivalent energy transfer. On the other hand the thermal mass is high so it will take time before the exterior heats up. It is not an indication of poor thermal management per se, just poor material choice.
Semiman