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What happens when a heatsink is put on top of a package? Well, you'd expect
the junction temperature to drop because we've suddenly got a lot more
surface exposed to the air. But life isn't always as simple as that! Here's
a little simulation which shows how there can sometimes be some quite
unexpected effects even in seemingly simple situations.
Figure 1 - General Configuration
The calculation is based on a 208L PQFP similar (but not identical)
to the package used in the JEDEC JC15.1 Still Air Round Robin. The board
is a low conductivity test board (JEDEC Standard JESD15_3) and it is mounted
in a horizontal configuration.
Figure 2 - Results: PQFP; No Heatsink; Power = 1W;
Natural Convection
With the power set to 1W, we get the results shown in Figure 2 with
a junction temperature Tj of 60.2 C (or (Theta)ja = 40.2 C/W).
Now, what happens if I add a nice big heatsink - in this case, an extruded
Aluminum heatsink with 10 fins? Figure 3 shows that, as you'd expect,
Tj drops to 42.3C ((Theta)ja = 22.3C/W). Obviously all that
extra surface area is really helping.
Figure 3 - Results: PQFP; 10 Fin Extruded Heatsink;
Power = 1W; Natural Convection
But now lets look a little more closely at what's happening inside the
component. We know that, for this type of package without a heatsink,
the majority of the heat passes through to the board through the leads
(see, for example, Application Note #102).
In fact, for this package in this configuration without a heatsink,
the proportion is about 65%. With the heatsink on top, we would
expect to see a much greater proportion go through the top and thus less
through the leads. But, if we use FLOTHERM mean flow regions to determine
the heat flux through the leads, we find that the proportion has only
dropped to about 58% (Figure 4) - not a very great effect.
Figure 4 - Comparison of Results
Let's look at it in a different way. Given the power flux through the
leads, and the temperature of the die and the board, we can calculate
an effective thermal resistance for the conduction path from the die to
the board - let's call it (Theta)jb. Without a heatsink, the junction
to board thermal resistance is about 100C/W. With the heatsink in place,
the junction to board thermal resistance drops to 58C/W. How is the heatsink
changing the thermal characteristics of the component?
Figure 5 - Results: PQFP; 10 Fin Extruded Heatsink;
Power = 1W;
Natural Convection Close up of the Temperatures in the Package
Look a little more closely at the temperature contours within the package
when the heatsink is on top. Figure 5 is a close-up of the package which
shows that, at the center of the package, the temperature gradient drives
heat from the die into the heatsink. However, towards the edge of the
package, the temperature gradient is reversed and heat is conducted from
the heatsink base into the package itself and from there through the lead
frame into board. In effect, the heatsink base provides a conduction path
parallel to the lead frame thus reducing the junction to board thermal
resistance.
Figure 6 - Results: PQFP; Heat Spreader on Top; Power
= 1W; Natural Convection
Finally, let's try something radical. Let's cut off all of the fins
from the heatsink and simply attach the heatsink base to the top of the
package! A conventional analysis using a databook value for (Theta)jc
and Heatsink Thermal resistance would suggest that we'd get slightly poorer
performance than the bare package (we are adding a little thermal resistance
to the top but leaving the exposed area unchanged). However, when we run
the calculations, we find that the performance is considerably better
than the bare package, and very little worse than the case with the heatsink
(Tj = 44.9 C or (Theta)ja = 24.9C/W).
Moral: don't always take heatsinks for granted!!!
Credit where credit's due: I am indebted to Tiao Zhou of SGS Thomson
for suggesting this little study - something that I'd never even thought
about!
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