ABC of CLR
EPCI online handbook on C,L,R Passive Components
Chapter C: Capacitors
EPCI licenced content by:
 EPCI European Passive Components Institute experts original articles
 CLR Passive Components Handbook by P-O.Fagerholt*
*used under EPCI copyright from CTI Corporation, USA
WET ALUMINUM ELECTROLYTICS
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C 3.3 WET ALUMINUM ELECTROLYTICS
C 3.3.1 Introduction
Wet aluminum (Al) electrolytic capacitors continuously generate hydrogen gas under operation and while stored with even a small residual charge. That hydrogen must be able to diffuse and exit the package or it will rupture. Thus conventional wet Al electrolytics must not be hermetic sealed. The diffusion takes place through the non-hermetic lid that usually has a rubber packing in the pressure seal against the can edge.
Larger size cans are also supplied with a safety vent that provides for relief in the instance of very critical gas generation. There are also special, high reliability hermetic Al electrolytic available on the market based on improvements of electrolytes and gas absorbing compounds.
In catalog sheets for different electrolytic types it’s usual to show impedance versus frequency at different temperatures. The axes are given a logarithmic scale and look in principle like the one in following figure where the ESR at several temperatures can also be read.
Figure C3-24. Impedance versus frequency at two temperatures T1 and T2 .
The capacitance stability versus time and temperature is comparatively poor. Tolerances must be adjusted, from ±20 for the best professional types to –20/ +80% for some commercial makes. Rated voltages exist from 3 to above 500 V DC.
The maximum permissible reverse voltage is:
• 0.5 V for VR ≤ 7 V.
• 1 V for VR > 7 V.
The reverse voltage figures apply up to the rated temperature. Then a proper derating is recommended. Losses often are large and strongly temperature and frequency dependent. Figure C3-24 shows how the impedance versus frequency curve at increasing frequencies approaches and finally reaches the ESR contribution at temperature dependent levels. This occurs somewhere between 1 to 100 kHz, depending on capacitance size and temperature.
Recent examples of new solid-polymer or hybrid electrolytes with improved electrical conductivity present on the market. Nevertheless, the conventional wet Al electrolytic capacitors are one of the lowest cost capacitor technologies on the market and still under high volume use or in higher voltage applications where there is no polymer/hybrid electrolyte alternatives.
Examples of some typical applications of wet Al electrolytics are as follows: smoothing, filtering in Switched Mode Power Supplies (SMPS; low ESR necessary), coupling/decoupling , energy storage, timing and delay circuits with large time constants.
C 3.3.2 Properties
Capacitance versus temperature
Figure C3-25. Typical curve range for capacitance versus temperature T for wet Al electrolytics.
Figure C3-25 shows a strong capacitance deviation at lower temperatures. It is caused by the increasing resistivity of the electrolyte. Note that the temperature ranges vary and with that the temperature dependence of corresponding electrolytes also varies. Some types can withstand –55/+150 °C, others only –25/+85. Most common temperature ranges are –40/+85 and -40/+105 °C.
Capacitance versus frequency
Figure C3-26. Typical curve range for capacitance versus frequency of wet Al electrolytics.
Note in Figure C3-26 how the low voltage – high capacitance, characterized by large foil surfaces and finer etching, demonstrates a higher frequency dependence while the opposite decreases this dependence.
Tan δ versus temperature
Figure C3-27. Typical curve range for normalized Tand versus Temperature for wet Al electrolytics.
Figure C3-27 shows the normalized Tan δ value, i.e., the multiplier for Tan δ compared with the reference value at 20 °C. Thus, according to the curve, in worst case Tan δ55°C is approximately 50 times larger than Tan δ+20°C.
ESR versus temperature
According to the formula Tan δ = ESR x ωCs which means that at a fixed frequency the ESR versus temperature curve will have the same appearance as the one of Tan δ (Figure C3-28).
Figure C3-28. Normalized ESR range versus temperature T in wet Al electrolytics. Reference value at 25°C.
ESR versus frequency
In Figure C3-29 the ESR versus frequency is shown as a ratio between the 100 Hz value and the ones at other frequencies (a multiplier of the reference value). It applies at room ambient temperatures and above and will differ slightly at lower temperatures. The strong slope of the curve range at lower frequencies depends mainly on the oxide losses.
Figure C3-29. Typical curve range for normalized ESR versus frequency for wet Al electrolytics. Reference at 100 Hz.
Just for caparison a typical curve also for solid Al is shown.
ESR and ripple currents
In filter applications the capacitors will conduct considerable AC currents caused by superimposed ripple. The ripple current creates heat in the capacitor ESR. Therefore a maximum ripple current IR-max is specified at reference conditions: 100 or 120 Hz and at some higher temperature, for example 85 °C or the upper category temperature Tuc (Figure C3-25). With reference data in the data sheets as a starting-point it is then possible to convert these values to operational condition values.
The maximum ripple current is specified to create a generated average core temperature rise of 10 °C above the allowable maximum ambient temperature. This margin, however, varies strongly with can size and manufacturer. With respect to proper derating this margin should not be utilized. When the ripple current frequency rises, the ripple current capability increases. That depends on a corresponding decrease of the ESR (Figure C3-29) that has a negative TC, mainly caused by the electrolyte, and this will consequently lead to a decreasing ESR when the temperature rises (for example, at higher ripple currents) (Figure C3-28). If we, for example, specify an IR-max at 100 Hz and permit 1.4 x IR-max at 10 kHz this is possible just because ESR10kHz ≈ ½ESR100Hz. For (1.4 x IR-max )2 x ½ ESR100Hz ≈ 2 x ½ x (IR-max )2 x ESR100Hz = (IR-max)2 x ESR100Hz. But, please, check the manufacturer’s data sheets. There are differences between both styles and manufacturers.
Leakage current versus temperature
Figure C3-30. Normalized typical curve range for DCL versus temperature for Al electrolytics. Reference DCL at 25 °C.
Also the important parameter leakage current varies with the environmental conditions. When temperature increases from the lower to the upper limit of the temperature range, leakage current rises approximately two orders of magnitude (Figure C3-30). Next figure shows the ratio of DCL versus applied DC voltage and DCL at 100% VR.
Leakage current versus DC voltage
Figure C3-31. Normalized typical curve range for DC Leakage versus DC voltage for wet Al electrolytics.
C 3.3.3 Heat generation
Figure C3-32. Thermal dissipation in a large Al electrolytic with internal heat generation.
Aluminum electrolytics also are manufactured with high CV products in correspondingly large cans. If they are loaded with a superimposed ripple voltage heat generation from the power ESR x IAC2 might be troublesome. The rise of temperature will be largest in the center of the winding, i.e. the capacitor Hot Spot, and must not exceed certain values. Therefore a maximum AC current value is specified at 100 or 120 Hz and sometimes also at 20, 40 or 100 kHz. Furthermore it’s usual to state the maximum ESR at these frequencies. A schematic of the heat generation principle is shown in Figure C3-32. The components of ESR are shown in Figure C3-33.
Figure C3-33. Schematic of ESR components
• Rox = resistance in the dielectric oxide layer.
• Re = resistance in the electrolyte and paper separator.
• Rlead = resistance in electrical conduction paths.
Above all it’s the dielectric oxide losses that are frequency dependent and cause the general appearance of the ESR curve shown in Figure C3-29. In more detail the frequency dependence can be illustrated as in Figure C3-34 where one can note how the oxide losses, on the whole, end above 1.5 kHz.
Figure C3-34. Frequency dependence of the oxide losses in Al electrolytics.
There are for high-reliability styles information about their thermal capacitance and resistance. If we know the can and ambient temperatures then the Hot Spot temperature of the capacitor can be calculated more thoroughly. A less accurate but more simple calculation says that Thsp – Ty » Ty – Ta⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅⋅[C3-1]
• Thsp = Hot Spot temperature.
• Ty = surface temperature of the can.
• Ta = ambient temperature (Figure C3-35).
C 3.3.4 Life calculation
The Life (L0) for a wet Al electrolytic is stated in the catalog sheets as the number of hours at the maximum temperature, Tuc. If, for example, the stated L0 = 2000 h @ 85 °C, we get the Life at 35°C by means of the formula as
Thus the formula says that Life is doubled for a temperature decrease ∆T = 10 °C. We repeat that the formula is just a rule of thumb (Arrhenius relationship) and no accurate calculation.
C 3.3.5 Mounting
Large can electrolytics with a safety vent preferably should be mounted in an upright or horizontal position, thus preventing electrolytic liquids from obstructing any gas diffusion.
C 3.3.6 Cleaning solvents
Penetrating contaminations, especially from halogenbased washing agents, sooner or later may lead to a short circuit. Exposed to an electric field they will be converted electrochemically to free chlorides that will cause corrosion, a subsequent increase in leakage current and finally a short circuit. Because destruction takes place only when the capacitor is electrically operated, failures unfortunately occur only in the field and after some time. In order to avoid a suction effect during the washing one shall make sure that the component has a lower temperature than that of the washing bath.
Table C3-5. Examples of cleaning solvents.
C 3.3.7 Failure modes
The most common failure is drying escape of the electrolyte. Drying first manifests itself as a high ESR. For it’s not only hydrogen gas that diffuses through the sealings to the lid of the aluminum electrolytic. The electrolytic liquid also diffuses through the non-hermetic lid. One leading manufacturer has solved this problem to a great extent by utilizing rubberized laminated paper washers instead of conventional rubber seals. However, diffusion and hydrogen development will take their tribute. Gradually the electrolyte dries up and left will be only a kind of resistor.
Experiences indicate that an electrolyte loss of 20% increases the ESR approximately 100%! The wet Al electrolytic capacitor is the one component type that has the most distinct life limitation. Beyond a certain time the capacitor ceases to be a capacitor. At tests performed at the maximum temperature one may get an idea of the diffusion rate and thus the life by weighing the part and calculating the electrolyte loss during the test. Wet Al electrolytics in chip design had some problems when they first were introduced on the market. There were examples of how certain types lost half of the electrolyte supply during the soldering process.
Now these problems certainly are overcome, but make sure the manufacturer is in command of the difficult manufacturing process of chip sealing. Open circuits caused by fatigue fractures in internal contact strips between winding and terminals during vibration/bump are not too unusual. Chloride contamination of foils from clammy hands or penetrating cleaning agents can cause high leakage currents and finally short circuiting.
Table C 3-6. WET AL ELECTROLYTICS, POLARIZED
Table C 3-6, ctd. WET AL ELECTROLYTICS, POLARIZED
ABC of CLR: Chapter C Capacitors
WET ALUMINUM ELECTROLYTICS
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Concepts and Measurements
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