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Heat Sink Measurements
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15 December 2007
I ran a series of quick tests on five heatsinks for TO220
tab-mount transistors today. The heat source is a Caddock MP930 film resistor,
packaged in a TO220 style mount. The MP930 used has a nominal value of 10 Ω, 1%
and is rated at 30 watts when mounted on an appropriate heat sink. The MP930's
data sheet may be found
here.
I applied DC power across the resistor with an HP 6205C
dual DC power supply, paralleling the two outputs to obtain additional current.
The voltage across the test resistor is measured with an HP 3468A digital
multimeter. The MP930 test resistor measured 9.990 Ω using the HP 3468A in
4-wire resistance mode. Power is computed as E2/R, and I assumed the
MP930's resistance remained constant over the test temperature range. (This is a
reasonable assumption as the MP930's worst-case temperature coefficient is +80
PPM/°C. For a 100 °C temperature increase, the total resistance change is 0.8%.)
I monitored the temperature of the device and heat sink
with a Fluke 62 infrared thermometer, and recorded the highest temperature
reading. The maximum temperature reading was found on the MP930's surface, near
the mounting hole. The data is plotted using Origin 7.5 and the data fitted with
a linear curve fit to extract the thermal resistance. |
A simple, but accurate, model of temperature and heat flow in this analysis is
illustrated below. (For the original document, click
here.) |
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The thermal model is analogous to a series resistor circuit;
power dissipated maps into current, thermal resistance of the various elements
of the assembly map into resistance and temperature maps into voltage.
In the illustration, Ta, Ts, Tc and Tj are:
Ta—Ambient (air) temperature
Ts—Heat sink temperature
Tc—Case temperature (the TO220 device's outer surface in our test arrangement)
Tj—Junction temperature, i.e., the temperature of the semiconductor junction, or
in this case, the thin film resistive element, inside the case.
The three thermal resistances are:
Rjc—resistance from junction to case
Rcs—resistance from case to heat sink
Rsa—resistance from heat sink to ambient
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Rjc is 4.17 °C/watt (note the units; thermal resistance is
most conveniently stated as degrees per watt) according to the MP930's data
sheet. Rcs is a function of the size of the device,
the type of thermal compound used between the device and the heat sink and the
thickness of the compound layer. For the TO220 device and the thermal compound I
used (Dow Corning No. 4 silicone), I estimate Rcs is between 1 and 2 °C/watt.
If we use a heat sink with Rsa of, say, 12.7 °C/watt and
if we apply 3.162 volts across the MP930, and if the ambient temperature is 70
°F, we may compute the various temperatures. 70°F corresponds to 21.1 °C.
First, the power dissipated in the MP930 is (3.162)2/10
= 1.0 watts.
The temperature drops are thus:
- Drop from junction to case: 1.0 watts * 4.17 °C/watt =
4.17 °C.
- Drop from case to heatsink: 1.0 watts * 1.5 °C/watt =
1.5 °C (taking the midpoint of the estimated Rcs
- Drop from heatsink to ambient: 1.0 watts * 12..7
°C/watt = 12.7 °C.
We may now compute the various temperatures:
- Ambient temperature, we have said is 21.1 °C
- Heatsink temperature is 21.1 + 12.7 °C or 33.8 °C
- Case temperature is 33.8 + 1.5 °C or 35.3 °C
- Internal junction temperature is 35.3 + 4.17 °C = 39.5
°C, or 103 °F
If we needed, for example, the heat sink rating needed to
keep the junction temperature at 120 °C, with an ambient temperature of 100 °F
(approx 38°C) and with 10 watts power dissipation, we would use the approach
outlined above, but solving for Rsa.
Tcase = 120 °C - 10.0 watts * 4.17 °C/watt = 78.3 °C at
case
Theatsink = 78.3 °C - 10 watts * 1.5 °C/watt = 63.3 °C at heat sink
Rsa = (63.3 °C - 38 °C) / 10 watts = 2.53 °C/watt
Thus, our target requirements dictate a heat sink with a
thermal resistance of approximately 2.5 °C/watt. This is a large heat sink, by
the way. We might consider relaxing the junction temperature limit (the MP930 is
rated to 150 °C, after all) and also using a higher quality thermal compound to
get by with a smaller heat sink.
The figure below shows the five heat sinks tested. In addition, I ran a test
without any heat sink.
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| Photo Key |
Manufacturer |
Part No. |
Measured
Rsa ° [1] |
Mfgr Specified Rsa |
| B |
Futurlec |
TO220S008A |
12.7 °C/watt |
not specified |
| none |
none |
none |
30.3 °C/watt |
|
| A |
AAVID |
576802b04100 |
26.6 °C/watt |
27.3 °C/watt |
| C |
Futurlec |
TO218S049B |
7.0 °C/watt |
not specified |
| D [2] |
Comair/Rotron |
411626B02500 |
6.8 °C/watt |
4.2 °C/watt |
| D [3] |
same |
same |
5.4 °C/watt |
4.2 °C/watt |
| E |
AAVID |
551002B00000G |
11.7 °C/watt |
12.4 °C/watt |
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[1] Because of the uncertainty of the case-to-heatsink thermal resistance, the
measured Rsa values above represent the series combination of Rsa and Rcs. This
is because the infrared thermometer measured the outside case temperature, not
the heat sink temperature. You may wish to therefore subtract the Rcs's "guessimate"
of 1.5 °C/watt, from these values.[2] With Dow
Corning No. 4 silicon grease between MP930 and heat sink.
[3] With AAVID Thermalcote II heat sink compound between
MP930 and heat sink. |
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The plot below shows the temperature versus power
data for the six tests. Also shown, but difficult to see at the reduced scale
version, are linear fits to the measured data. The slope of linear fit ΔT/ΔP
(with T in °C, of course) provides Rsa for each measured heat sink. |
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17 December 2007
I received a tube of AAVID Thermalcote II heat sink
compound today and re-ran the Rotron / Comair heat sink test with it. The
results are quite impressive. For a given maximum temperature, using Thermalcote
II permits about 25% greater power dissipation.
I've had the tube of DC No. 4 for at least 35 years, so
it's not surprising that better heat sink joint compounds have been developed
and, I believe, DC No. 4 was intended more for electrical insulation and water
displacement properties than for a heat sink compound. |
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20 December 2007
I purchased several surplus heat sinks from All
Electronics
http://www.allelectronics.com/ intended for Pentium-type integrated circuit
cooling with the thought of using them to cool TO-220 case type power MOSFET
transistors and TO-220 style power resistors. The particular heat sink is
described as:
AVC # AV-112C80FBL03. 12 Vdc,
0.1A, 60 mm ball bearing fan attached to an aluminum heatsink. Overall
dimensions: 3.14" x 2.50" x 2.48" high. Bottom, mating, surface of heatsink is
3.04" x 1.85" Mating surface is prepped with a 0.8" square of thermal
compound. Fan has three 8" leads with 3-pin female connector (0.1" spacing).
UL, CSA, CE, TUV.
CAT# CF-286
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I removed the mounting clip and drilled and tapped
several 4-40 mounting holes in the heat sink's bottom surface. (Of course, if
you drill & tap the bottom surface, remove the fan assembly first!) The photo
below shows the heat sink with two Caddock MR930 resistors and two BUZ11 power
MOSFETs installed. I used AAVID's Thermalcote II compound between the tabs and
heat sink surface. BUZ11's connect the drain to the tab, so the heat sink
is also part of the drain circuit and the drains are in parallel.
The fan power connections are, by the way, positive to
red, negative to black (12 volts). The white lead is an open-collector
tachometer sensor, providing a speed-related pulse width for fan failure
detection.
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Here's the heat sink connected to a breadboard constant current driver circuit.
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The heat sink is quite effective, as seen in the plot below. The first test used
a single Caddock MP930 10 ohm resistor, whilst the second test is the as-built
prototype constant current circuit. The circuit shares the current approximately
equally between the two MOSFET/sense resistor pairs (within a couple percent).
The heat sink appears to be more efficient in the second test for a couple
reasons. Most importantly, the heat sources are spread over a larger area. Also,
my data measures the case temperature, not the heat sink surface temperature and
the BUZ11's have a better thermal structure than the MP930 resistors. In the
dual FET case, the sense resistors (0.1 ohm) dissipate a small percentage of the
total power, typically a couple percent, depending on the current setting.
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23 December 2007
One question that I've assumed an answer to is what is the
case-to-heat sink thermal resistance, RθCS
The commonly quoted value for a TO-220 metal tab transistor, employing decent
quality thermal compound, is 0.5 °C/watt.
To measure
RθCS I added two Fluke 80PK-1 Type K bead thermocouple temperature
sensors to an IRF510 MOSFET transistor mounted on the Comair/Rotron 411626B02500
heatsink used in my earlier studies. One attaches to the top of the IRF510's tab
to measure case temperature and the second attaches to the heat sink near the
IRF510, as shown below. The thermocouples are read with a Fluke 189 digital
voltmeter on temperature scale, using a Fluke 80AK Type K to DMM adapter.
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IRF510 with two thermocouple temperature sensors. One is
attached to the heat sink and the other to the IRF510's tab to measure the
case temperature.
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These connections are likely not perfect, but are close enough for our purposes.
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Temperature Degrees C |
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Watts |
Case |
Heat Sink |
RθCS |
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0.0 |
22.8 |
23.1 |
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2.6 |
36.2 |
34.8 |
0.53 |
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natural convection |
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4.2 |
46.2 |
45.1 |
0.25 |
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natural convection |
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5.1 |
51.5 |
50.0 |
0.29 |
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natural convection |
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7.5 |
68.2 |
64.8 |
0.45 |
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natural convection |
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10.0 |
81.7 |
77.2 |
0.45 |
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natural convection |
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12.5 |
94.3 |
89.1 |
0.42 |
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natural convection |
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20.0 |
47.6 |
38.9 |
0.43 |
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with fan |
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40.0 |
72.9 |
56.4 |
0.41 |
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with fan |
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50.0 |
85.4 |
63.2 |
0.45 |
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with fan |
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Mean |
0.41 |
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Based on these measurements, the standard quoted 0.5
°C/watt is conservative. Since the measured data involves subtracting two
temperatures that are not that far apart at low power, the higher power readings
are more trustworthy than those at lower power levels.
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I also compared the thermocouple case and heat sink
temperatures with simultaneous readings using a Fluke 62 IR thermometer. In all
cases, the IR thermometer readings were between the case and heat sink
temperatures measured by thermocouple. It appears, therefore, that the IR spot
size is sufficiently large that an averaging effect is present. Fluke specifies
the 62 IR thermometer as ±1.5°C over the
temperature range in question. The 62's spot size ratio is 10:1, i.e., at
10 inches distance, the spot size is 1 inch. The 80PK-1 thermocouple bead probe
has a typical error of ±1.5°C over the temperature range in question.
These error bands are large compared with the difference
between the case and heatsink temperatures, which again suggests some caution
should be exercised in using the measured 0.41 °C/watt value. |
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