| Thermally Conductive Microwave Materials |
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| Written by Russ Hornung, Mike Smith and Chet Guiles | |||
| Thursday, 01 May 2008 14:20 | |||
Increasing the thermal conductivity of the base materials improves thermal management in RF designs.Looking
at the thermal issues which are impacting microwave design in today’s
marketplace, we see several drivers that will continue to require
better and more effective thermal management in the near future. Some
of these factors are relevant to all electronics packaging, such as
increased watt density on smaller package footprints, but others are of
particular importance to the microwave and RF industries. Among the
more important considerations for the microwave engineer are:
When
the heat generated by an active device mounted on a PCB cannot be
dissipated, then the temperature of the device rises. With all the
drivers pointing toward more power and smaller board surface area, the
watt density becomes such that temperatures can easily exceed the
qualificated temperature for many of the individual components. Since
reliability of components follows a first order Arrhenius equation, a
10ËšC increases in temperature doubles failure rate, so even 1ËšC
temperature increase matters. Figure 1 shows data
presented by Eli Reese of TriQuint, and presented at IWPC in November
2005, relating junction temperature to mean time-to-failure. The key to
reducing junction temperature is to increase the rate at which heat can
be removed from the device and from the working area of the PCB
immediately adjacent to the device.
The
cost of device failure can be significant since device failure accounts
for as much as 70 to 90% of equipment downtime, and in the case of
tower-mounted electronics, the cost can run several thousand dollars
for a simple repair that results in a short downtime. In bad weather
this can extend to a full day and cost as much as $25,000. Between
actual repair costs and potential lost revenue the implications of this
trend towards increased operating temperatures of PCBs is substantial.
The industry is looking seriously at solutions that can provide a
cost-effective way to mitigate the risk of failure. Heat
is generated every time an active device is in operation. Heat itself
does not become a problem until there is an increase in temperature
above a critical point (typically 105 to 120ËšF). In simple terms, the
whole business of managing heat in a PCB assembly is about preventing
the junction temperature from getting high enough to “fry” the active
devices. Heat is moved by one of three basic modes:
conduction, convection or radiation. In a PCB assembly all three are in
effect to one degree or another. The most effective is direct
conduction, where a warmer body is in direct contact with a cooler one,
and the heat moves from the hot to cold material (Figure 2).
The rate at which heat is carried from one to the other depends on the
thermal gradient, the coefficient of heat transfer of both materials,
the quality of the interface and to a lesser extent, the heat capacity
of the cooler body – that is its ability to absorb heat.
Convection
is the transfer of heat from a hot body to a cooler gas or liquid,
which carries the heat away. Convection may be aided by forcing the
cooling gas or liquid to flow past the warm body, removing the heat
more quickly. Radiation is the removal of heat from a body by the
emission of energy in the form of electromagnetic radiation, which may
be in the infrared (heat) or even visible (light) parts of the
spectrum, depending on the temperature of the radiating body. Corollary
to consideration of the thermal conductivity (Tc) of laminate substrate
materials is also the fact that the heat transfer coefficient in the
perpendicular direction (through the PCB) is different from that in the
plane of the board. Unfortunately most modeling software assumes
isotropy, which may result in over or underestimation of the heat
removal. Traditionally, a number of approaches have
been put forward to reduce temperature in PCBs by removal of heat from
active devices. The IWPC has been actively involved in assessment and
discussion of the various thermal management techniques, which include
the following:
While
all of these methods (note the predominance of the more efficient
conductive approach) are effective to varying degrees in the reduction
of junction temperatures, many of them have attributes that make them
less than ideal for use in microwave or RF circuit boards. Thermal vias
(a clusters of plated-through holes located beneath an active device)
are effective in removing heat because of the high thermal conductivity
of copper (370-400 W/m-K) but the plated through holes near the signal
traces can affect signal integrity, and a large number of plated
through holes can affect the mechanical strength of the PCB itself. Heat
sinks and heat spreaders are heavy and expensive (a 3mm copper plate
can add as much as $25 to a single PCB) and devices such as thermal
coins that require cutouts result in increased fabrication complexity
and assembly costs. More sophisticated approaches such as forced
convection are costly, and may themselves be subject to risk of
electromechanical failure. An attractive alternative
to total reliance on the traditional approaches of thermal management
is to build the underlying PCB with a dielectric material that is
inherently more thermally conductive. Conventional PCB materials having
a thermal conductivity of 0.2 to 0.25 W/m-K, and filled products range
from 0.4 to 0.6 W/m-K do not provide enough heat removal and heat
spreading capacity to do the job alone. There are
new materials entering the market that have a 6.15 Dk and are suitable
for use as microwave substrate materials. These materials can provide
thermal conductivity (Tc) of 1.1 W/m-K perpendicular to the plane of
the board, and 1.4 W/m-K in-plane. This is more than double the best
thermal conductivity currently available in a standard microwave PCB
substrate materials, and high enough to allow designers to reduce
dependency on more costly approaches. What benefit does increased thermal conductivity of microwave PCB substrates offer to the PCB designer?
The design objectives for the development of these thermally conductive materials included:
The
specific target products were to produced as 6.15 and 3.50 Dk materials
to meet the predominant industry demand for RF amplifier designs. Table 1 compares the key properties of two standard and two thermally enhanced conductive materials.
The
unique chemistry of the engineered laminate material includes a
significantly reduced TCEr (thermal coefficient of dielectric constant)
as seen in Figure 3. This translates into a more stable signal within any range of temperature fluctuation.
The improvements of this thermally enhanced material include:
To illustrate the impact of
thermal conductivity both in the perpendicular direction, as indicated
by reduced temperatures measured at the active device, and in-plane, as
determined by the degree of heat spreading, a sample circuit based on
an RF power field effect transistor was developed and thermograms
obtained using thermally conductive laminate and a standard material
with a thermal conductivity of 0.46. The results
were significant both in terms of the heat reduction at the top surface
and the spreading of the heat in the plane of the board. The resulting
thermograms dramatically illustrate the effect of increased thermal
conductivity. The maximum temperature reached at constant wattage was
82ËšC for the conventional material, 73ËšC for the thermally enhanced
material, a reduction of 10% and more importantly, a reduction of 9ËšC
that could be the difference between life and death for sensitive
junctions. (Figures 4a and 4b).
Summary
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