The structure function shown in Figure
4 is a thermal resistance / capacitance map along the heat
flow path in an IC package. The x axis is the thermal resistance,
left-hand side: chip, right-hand side: ambience. The y axis
is proportional to the squared cross-sectional area of the heat
flow path.
Irregularities of the heat removing (as faulty
die attach etc) can be easily determined and localized with the
help of this diagram. Thermal quality of the packages can be determined
easy.
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Figure 4: The differential
"structure function" of an IC package |
In Figure 5 one can see
the so called cumulative (or integral) structure function,
where the x-axis is the cumulative thermal resistance - starting from the chip, the y-axis is the cumulative heat
capacitance.
The structure function is theoretically derived
from the one-dimensional heat-flow equation. (One-dimensional here
means essentially one dimensional, including cylindrical
and spherical propagation, too.) In practice, it can be easily constructed
from the Cauer-type model network shown in Figure
2. The thermal resistance between the n-th element of
the model network and the heat source is
and the cumulative thermal capacitance is
where Ri and Ci denote the element values of the i-th
stage of the Cauer-type model network. It can be proved, that the
derivative of Kn,
the differential structure function
is proportional to the square of the cross-sectional
area of the conducting path.
The k(r) differential structure function has some interesting features. For
example, its integral is characteristic for the heat capacitance
of a given section of the heat conduction path. More precisely,
the total heat capacitance between two points of the structure characterized
by parameters r1 and r2 is
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Figure 5: Cumulative
structure function of the heat-flow path. The left-hand side
corresponds to the chip, the right-hand side to the ambience. |
The physical distance between points of the structure
characterized by parameters r1 and r2 is
where l and c denote the thermal conductivity and the specific
heat per unit volume of the material. (For further features and
for the analytical form of the structure function in special cases
refer to e.g. [8].) Values of k for
different materials are given in Table 2
Material |
k [W2 sec /
K2] |
Silicon |
2.58·108 ·A2 |
Iron |
2.65·108 ·A2 |
Kovar |
0.70·108 ·A2 |
Al2O3 |
0.95·108 ·A2 |
|
Table 2 k values
for different materials. A denotes the cross-sectional
area. |
As it can be seen in Figure 5,
the structure function tends to infinity, corresponding to the fact,
that the "universe" as a general thermal environment has
an infinite thermal capacitance. The distance between the origin
and the location of this singularity of the structure function is
exactly the thermal resistance between the heat source (in our case
the test chip) and the ambience (which is 45 K/W in Figure
5).
The features characterized by relations (d) and (e) suggest, that the structure function is
a good tool to identify geometrical dimensions of the heat conduction
path if the material is known. The structure function can also be
used to guess the type of the material of the heat conduction path
in the knowledge of its geometrical dimensions, but in any case,
the total chip-to-ambience thermal resistance of the structure can
be identified with its help, see our simple case
studies.
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