Dielectric absorption

Dielectric absorption is the name given to the effect by which a capacitor, that has been charged for a long time, discharges only incompletely when briefly discharged. Although an ideal capacitor would remain at zero volts after being discharged, real capacitors will develop a small voltage from time-delayed dipole discharging,[1] a phenomenon that is also called dielectric relaxation, "soakage", or "battery action". For some dielectrics, such as many polymer films, the resulting voltage may be less than 1–2% of the original voltage, but it can be as much as 15% for electrolytic capacitors. The voltage at the terminals generated by the dielectric absorption may possibly cause problems in the function of an electronic circuit or can be a safety risk to personnel. In order to prevent shocks, most very large capacitors are shipped with shorting wires that need to be removed before they are used and/or permanently connected bleeder resistors. When disconnected at one or both ends, DC high-voltage cables can also "recharge themselves" to dangerous voltages.

Theory
The random orientations of molecular dipoles in a dielectric are aligned under the influence of an electric field by applying a voltage to the electrodes.
Circuit model for explaining a time-delayed voltage build-up by parallel RC-timers

Charging a capacitor (due to a voltage between the capacitor plates) causes an electric field to be applied to the dielectric between the electrodes. This field exerts a torque on the molecular dipoles, causing the directions of the dipole moments to align with the field direction. This change in the molecular dipoles is called oriented polarization and also causes heat to be generated, resulting in dielectric losses (see dissipation factor). The time of the dipoles orientation does not follow the electric field synchronously, but is delayed by a time constant that depends on the material. This delay corresponds to a hysteresis response of the polarization to the external field.

When the capacitor is discharging, the strength of the electric field is decreasing and the common orientation of the molecular dipoles is returning to an undirected state in a process of relaxation. Due to the hysteresis, at the zero point of the electric field, a material-dependent number of molecular dipoles are still polarized along the field direction without a measurable voltage appearing at the terminals of the capacitor. This is like an electrical version of magnetic remanence. The oriented dipoles will be discharged spontaneously over time and the voltage at the electrodes of the capacitor will decay exponentially.[2] The complete discharge time of all dipoles can be days to weeks depending on the material. This "reloaded" voltage can be retained for months, even in electrolytic capacitors, caused by the high insulation resistance in common modern capacitor dielectrics. The discharge of a capacitor and the subsequent reloading can be repeated several times.

Measurement

Dielectric absorption is a property which has been long known. Its value can be measured in accordance with the IEC/EN 60384-1 standard. The capacitor shall be charged at the DC voltage rating for 60 minutes. Then the capacitor shall be disconnected from the power source and shall be discharged for 10 s. The voltage regained on the capacitor terminals (recovery voltage) within 15 minutes is the dielectric absorption voltage. The size of the dielectric absorption voltage is specified in relation to the applied voltage in percent and depends on the dielectric material used. It is specified by many manufacturers in the data sheets.[3][4][5][6][7]

Type of capacitor Dielectric absorption
Air and vacuum capacitorsNot measurable
Class-1 ceramic capacitors, NP00.6%
Class-2 ceramic capacitors, X7R0.6 to 1.0%[7]
Class-2 ceramic capacitors, Z5U2.0 to 2.5%[7]
Polypropylene film capacitors (PP)0.05 to 0.1%
Polyester film capacitors (PET)0.2 to 0.5%
Polyphenylene sulfide film capacitors (PPS)0.05 to 0.1%
Polyethylene naphthalate film capacitors (PEN)1.0 to 1.2%
Tantalum electrolytic capacitors with solid electrolyte2 to 3 %,[8] 10 %[9]
Aluminium electrolytic capacitors with non-solid electrolyte10 to 15%[10]
Double-layer capacitordata not available

Design considerations and safety

The voltage at the terminals generated by the dielectric absorption may possibly cause problems in the function of an electronic circuit. For sensitive analog circuits such as sample and hold circuits, integrators, charge amplifiers or high-quality audio circuits, Class-1 ceramic or polypropylene capacitors instead of Class-2 ceramic capacitors, polyester film capacitors or electrolytic capacitors are used.[11] For most electronic circuits, particularly filtering applications, the small dielectric absorption voltage has no influence on the proper electrical function of the circuit. For aluminum electrolytic capacitors with non-solid electrolyte which are not built into a circuit, the dielectric absorption voltage generated can be a personnel safety risk.[12] The voltage can be quite substantial, for example 50 V for 400 V electrolytic capacitors, and can cause damages to semiconductor devices, or cause sparks during installation in the circuit. Larger aluminum electrolytic capacitors and high-voltage power capacitors are transported and delivered short-circuited to dissipate this unwanted and possibly dangerous energy.

Another effect of dielectric absorption is sometimes described as "soakage". This manifests as a component of leakage current and it contributes to the loss factor of the capacitor. This effect has been known of only recently: it is now a proportionately greater part of leakage current due to the significantly improved properties of modern capacitors.[9]

No figures are available from manufacturers for double-layer capacitors.

History

Dielectric absorption was first discovered in Leyden jars and telegraph cables, and it was already a well-known phenomenon in the late 19th century. Once known as "electric absorption", satisfactory explanations of its physical mechanism was lacking at that time. A description appeared in James Clerk Maxwell's 1873 book A Treatise on Electricity and Magnetism, in which he derived its physical model, but it was only applicable to an inhomogeneous dielectric material with multiple layers.[13][14]

See also

References
  1. "Modeling Dielectric Absorption in Capacitors, by Ken Kundert" (PDF).
  2. "Elliot sound products, 2.1 - Dielectric Absorption".
  3. WIMA, Characteristics of Metallized film capacitors in Comparison with Other Dielectrics "WIMA". Archived from the original on 2012-11-05. Retrieved 2012-12-14.
  4. "Film Capacitors, TDK Epcos, General technical information" (PDF). Archived from the original (PDF) on 2012-02-01. Retrieved 2012-01-23.
  5. AVX, Dielectric Comparison Chart
  6. "Holystone, Capacitor Dielectric Comparison, Technical Note 3" (PDF). Archived from the original (PDF) on 2012-02-01. Retrieved 2012-01-23.
  7. https://www.wima.de/de/service/knowledge-base/grundlagen-der-kondensatorentechnologie/ knowledge base of the capacitor manufacturer WIMA (german), Retrieved 2020-11-21.
  8. "Kemet, Polymer Tantalum Chip Capacitors" (PDF). Archived from the original (PDF) on 2014-11-23. Retrieved 2012-01-23.
  9. R. W. Franklin, AVX, Analysis of Solid Tantalum Capacitor Leakage Current, PDF, PDF
  10. CDE, Aluminum Electrolytic Capacitor Application Guide, PDF
  11. National Semiconductors, Understand Capacitor Soakage to Optimize Analog Systems Archived 2010-01-23 at the Wayback Machine
  12. What's all this Trapped Charge and Dielectric Compression stuff anyhow?
  13. Maxwell, James (1873). "Chapter X. Conduction in Dielectrics". A Treatise on Electricity and Magnetism. Clarendon Press. p. 376. In a condenser of this kind, first charged in any way, next discharged through a wire of small resistance, and then insulated, no new electrification will appear. In most actual condensers, however, we find that after discharge and insulation a new charge is gradually developed, of the same kind as the original charge, but inferior in intensity. This is called the residual charge. To account for it we must admit that the constitution of the dielectric medium is different from that which we have just described. We shall find, however, that a medium formed of a conglomeration of small pieces of different simple media would possess this property.
  14. H. A. Rowland (1878). "Note on the Theory of Electric Absorption". American Journal of Mathematics. 1 (1): 53–58. doi:10.2307/2369434. JSTOR 2369434.

Further reading
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