KVoltage (Effects of applying voltage to life):
Miniature and large sized aluminum electrolytic capacitors for popular
applications, such as surface mount types, radial lead types, snap-in types
and block types, have little voltage effect on their life. Other factors like
temperature and ripple current determine the life in comparison with voltage,
as long as the capacitors are used at voltages and temperatures within the
specifications prescribed in the catalog. Consequently, KVoltage = 1 is used
for these capacitors. 350V and higher screw-mount terminal types of
capacitors for custom-made power electronics applications allow the lifetime
to extend by applying low voltage, relating to the characteristics of their
aluminum oxide layer. For Kvoltage values of the screw-monut products,
please contact our company or sales agents.
KRipple (Effects of ripple current to life):
Aluminum electrolytic capacitors have higher tanδ than any other types of
capacitors; therefore, the ripple current gives aluminum electrolytic
capacitors higher internal heat. Be sure to check the rated ripple current
which is specified in the catalog for assuring the life. The ripple current
through the capacitor produces heat by dissipating power from the
capacitor. This leads to temperature increase. Internal heating produced
by ripple current can be expressed by:
W = (IRipple)2 * RESR + V * I Leakage
Where:
W = Internal power los
IRipple = R.M.S. Ripple current
RESR = Internal resistance (ESR) at ripple frequency
V = Applied voltage
ILeakage = Leakage current
Leakage current may be 5 to 10 times higher than the values measured
at 20℃, but compared with IRipple, the leakage current value is very small
and negligible. Thus, the above equation can be simplified:
W = (IRipple)2 * RESR
The following equation gives the internal heat rise; it's heat rise to stable
condition. (It is necessary to input several factors):
(IRipple)2 * RESR = β * A * △T
Where:
β = Heat transfer constant
A = Surface area of can case
A = (π/4) * D * (D + 4L)
Where:
D = Can case diameter
L = Can case length
△T = An increase in core temperature by internal heating
due to ripple current
(△T = Core temperature - Ambient temperature)
From the above equation, internal temperature rise (△T) produced by
ripple current is given by:
△T = (IRipple)2 * RESR / (β * A)
When the ripple frequency is 120Hz, RESR at 120Hz is expressed by
RESR = tanδ / (ω * C)
△T = (IRipple)2 * tanδ / (β * A * ω * C)
Where:
tanδ = 120Hz value
ω = 2π * f = 2π * 120Hz
C = 120Hz capacitance value
As above equation, △T varies with frequency of ripple, frequency and
temperature dependent ESR and application on dependent β (even ripple
current is constant). We really recommend that customers measure △T
with a thermocouple at the actual operating conditions of the application
in lieu of using the above equation. (Another approximation of △T will
be stated later.) As mentioned in the paragraph of Ktemp, aluminum
electrolytic capacitors will slowly increase in tanδ and ESR during their
service life. The application without ripple current has no influence on
the life of the capacitor even though the ESR will increase during life.
In other words, the application with ripple current makes △T increase;
furthermore, a △T increase results in ESR increase. The ESR increase
then makes △T increase. It is a chain reaction. Theoretically, the
ripple current acceleration term (KRipple) cannot be simply expressed like
the ambient temperature acceleration term (KTemp). Practically, the
ripple current acceleration term (KRipple) can be approximately
expressed by an equation using a △T initially measured. The following
table shows the ripple current acceleration term (KRipple) for each
capacitor design group. Note that a △T over a certain maximum limit
may over-heat the capacitor, though the lifetime estimation will not give
you practical lifetime. For instance, the following shows a guide limit of
△T at each ambient temperature for 105℃ maximum rated products.
Ambient temperature TX (℃) |
85 |
105 |
Guide limit of △T (℃) |
15 |
5 |
Core temperature (Tx + △T) |
100 |
110 |
Approximation of △T
Estimation of the lifetime requires two temperature measurements;
first obtain △T by actually measuring the core temperature, inserting
the thermocouple inside the operating capacitor and secondary, the
ambient temperature. A more convenient way to get the △T is to
convert the surface temperature of the capacitor case and the ambient
temperature by using a coefficient specified for each case diameter as
tu
following:
△T = KC * (TS - TX)
Where:
KC = Coefficient from table below
TS = Surface temperature (℃) of capacitor can case
TX = Ambient termperature (℃)
No air flow conditions
Diameter (mm) |
Φ5 to Φ8 |
Φ10 |
Φ12.5 |
Φ16 |
Φ18 |
Φ22 |
Φ25 |
KC |
1.10 |
1.15 |
1.20 |
1.25 |
1.30 |
1.35 |
1.40 |
Diameter (mm) |
Φ30 |
Φ35 |
Φ40 |
Φ50 |
Φ63.5 |
Φ76 |
Φ89 |
Φ100 |
KC |
1.50 |
1.65 |
1.75 |
1.90 |
2.20 |
2.50 |
2.80 |
3.10 |
Also, you can roughly estimate a △T by using the following equation
without measurement.
△T = △TO * (IX / IO)2
Where:
△TO = 5℃ for 105℃ maximum rated capacitors
IO = Rated ripple current (ARMS); If its frequency is different
from operating ripple current IX, it needs converting
by using a frequency multiplier prescribed in the
catalog.
IX = Operating ripple current (ARMS) actually flowing into a
capacitor
Like switching power supplies, if the operating ripple current consists
of commercial frequency element and switching frequency element(s),
an internal power loss is expressed by the following equation:
W = (If1)2 * ESRf1 + (If2)2 * ESRf2 + --------- + (Ifn)2 * ESRfn
Where:
W = Internal power loss
If1 ---- Ifn = Ripple currents at every frequencies f1 ---- fn
ESRf1 ---- ESRfn = ESR's at every frequencies f1 ---- fn