Inrush Current Limiters In Switching Power
Supplies
The problem of current surges in switch-mode power supplies
is caused by the large lter capacitors used to smooth the
ripple in the rectied 60 Hz current prior to being chopped
at a high frequency. The diagram above illustrates a circuit
commonly used in switching power supplies.
In the circuit above the maximum current at turn-on is the
peak line voltage divided by the value of R; for 120 V, it is
approximately 120 x √2/RI. Ideally, during turn-on RI should
be very large, and after the supply is operating, should be
reduced to zero. The NTC thermistor is ideally suited for this
application. It limits surge current by functioning as a power
resistor which drops from a high cold resistance to a low
hot resistance when heated by the current owing through
it. Some of the factors to consider when designing NTC
thermistor as an inrush current limiter are:
• Maximum permissible surge current at turn-on
• Matching the thermistor to the size of the lter
capacitors
• Maximum value of steady state current
• Maximum ambient temperature
• Expected life of the power supply
Maximum Surge Current
The main purpose of limiting inrush current is to prevent
components in series with the input to the DC/DC convertor
from being damaged. Typically, inrush protection prevents
nuisance blowing of fuses or breakers as well as welding of
switch contacts. Since most thermistor materials are very
nearly ohmic at any given temperature, the minimum no-load
resistance of the thermistor is calculated by dividing the peak
input voltage by the maximum permissible surge current in
the power supply (Vpeak/Imax surge).
Energy Surge at Turn-On
At the moment the circuit is energized, the lter caps in a
switcher appear like a short circuit which, in a relatively
short period of time, will store an amount of energy equal
to 1/2CV2. All of the charge that the lter capacitors store
must flow through the thermistor. The net effect of this large
current surge is to increase the temperature of the thermistor
very rapidly during the period the capacitors are charging.
The amount of energy generated in the thermistor during
this capacitor-charging period is dependent on the voltage
waveform of the source charging the capacitors. However,
a good approximation for the energy generated by the
thermistor during this period is 1/2CV2 (energy stored in the
lter capacitor). The ability of the NTC thermistor to handle
this energy surge is largely a function of the mass of the
device. This logic can be seen in the energy balance equation
for a thermistor being self-heated:
~
DC/DC
Converter
Typical Power Supply Circuit
Input Energy = Energy Stored + Energy Dissipated
or in differential form:
Pdt = HdT + δ(T – TA)dt
where:
P = Power generated in the NTC
t = Time
H = Heat capacity of the thermistor
T = Temperature of the thermistor body
δ = Dissipation constant
TA = Ambient temperature
During the short time that the capacitors are charging
(usually less than 0.1 second), very little energy is
dissipated. Most of the input energy is stored as heat in
the thermistor body. In the table of standard inrush
limiters there is listed a recommended value of maximum
capacitance at 120 V and 240 V. This rating is not
intended to dene the absolute capabilities of the
thermistors; instead, it is an experimentally determined
value beyond which there may be some reduction in the
life of the inrush current limiter.
Maximum Steady-State Current
The maximum steady-state current rating of a thermistor
is mainly determined by the acceptable life of the nal
products for which the thermistor becomes a
component. In the steady-state condition, the energy
balance in the differential equation already given reduces
to the following heat balance formula:
Power = I2R = δ(T – TA)
As more current ows through the device, its
steady-state operating temperature will increase and its
resistance will decrease. The maximum current rating
correlates to a maximum allowable temperature.
In the table of standard inrush current limiters is a list of
values for resistance under load for each unit, as well as
a recommended maximum steady-state current. These
ratings are based upon standard PC board heat sinking,
with no air ow, at an ambient temperature of 77° (25°C).
However, most power supplies have some air ow, which
further enhances the safety margin that is already built
into the maximum current rating. To derate the
maximum steady state current for operation at elevated
ambient temperatures, use the following equation:
Iderated = √(1.1425–0.0057 x TA) x Imax @ 77°F (25°C)