Insulation Resistance, DCL Leakage Current and Breakdown Voltage
- Posted by doEEEt Media Group
- On February 22, 2023
- 0
This article explains some basic parameters of capacitors – insulation resistance, DCL leakage current, and breakdown voltage / withstanding voltage.
An important feature of a capacitor apart from its capacitance is:
- Its ability to keep the charge for some time without self-discharging due to its internal leakage (conductivity) mechanisms. Either IR Insulation Resistance or DCL leakage current electrical parameters characterize this. These reciprocal parameters describe the same capacitor stage, so it does not matter which parameters are used. Electrostatic capacitors such as paper, organic film, or ceramic capacitors are usually characterized by IR values, while electrolytic capacitors (aluminum, tantalum) with low IR values use DCL leakage current specification.
- Withstand a voltage before it breakdown. This is defined by its maximum Operating Rated Voltage and Breakdown Voltage. Rated voltage is a common parameter found in catalogs, and it practically means that manufacturers guarantee the specified electrical parameters and reliability are maintained up to this voltage. The maximum rated voltage can be categorized by AC/DC operation or maximum allowed operating temperature (so-called Category Voltage – will discuss this in next lectures)
Figure 1. Schematic of the Insulation Resistance IR in a capacitor.
The dielectric of a capacitor has a large area and a short length. Even if the material is a good isolator there always flows a certain current between the charged electrodes (the current increases exponentially with the temperature). This leakage can be described as a parallel resistance with a high value, an Insulation Resistance (Figure 1.). We use the abbreviation IR in the following.
Measurement of the IR and Leakage Current
At an IR determination, one measures the DC leakage current through the capacitor. The measuring circuit, however, always contains a certain series of resistance.
Hence we need to take into consideration the charging time. The circuit diagram and charging curve for a capacitor is shown in Figure 2.
The charging current to the capacitor is shown in Figure 3. (circuit diagram as in Figure 2.). If the capacitor is ideal the current would rapidly attain the limiting value corresponding to the IR. The ideal current curve is designated IC-ideal. But because the polarization in the dielectric requires a finite time for dipoles to reorient the real charging current follows the curve IC-polarization.
Figure 2. The charging curve for a capacitor in a resistive circuit
Figure 3. Ideal and real charging current in a capacitor
To attain the actual IR we would need to wait for a very long time. In practice, we content ourselves with a specified IR value corresponding to a measuring current at the time tmeasure in Figure 4. Here we have marked a specified current value which on the measuring devices is graded in the corresponding IR value. A common time for IR readings is in IEC specifications 1 minute. The MIL specifications often call for 2 minutes or more. Considerably shorter times are applied at incoming and production inspections. Information in this book is based on the 1-minute value if nothing else is stated. Additionally, the IR concerns the ”room temperature condition” (RT), approximately 23 °C. The IR decreases with an increase in part temperature and may, at the maximum temperature, be several ten powers lower than at RT.
Figure 4. Time limitations at IR measurements
The IR of capacitors of a specific type and voltage rating decreases proportionally to the growth in capacitance (i.e., the increasing area). And vice versa. A reduced capacitance by a correspondingly lessened area will increase the IR. However, up to a specific maximum value of capacitance, the IR actually is so high that it’s actually the outer construction and the molding or conformal coating that determines measured values. Up to this point, one specifies the IR in M. Above this breakpoint the specifications call for the constant product of IR x C (in seconds). This product also is designated the time constant (see next section).
For electrolytic capacitors with their relatively low IR rather the leakage current is specified.
See also the follow-up article with more details on Leakage Current Characteristics of Capacitors
The time constant
If we leave a charged capacitor with open connections the charge successively will leak from one electrode to the other through the internal insulation resistance. Eventually, the voltage will drop to zero. Because of the very high IR of the electrostatic capacitor (nonelectrolytic) a complete discharging will take an extremely long time. A more comprehensible measure of the discharge speed is the time constant. It is defined as the time for the initial voltage E to drop to the value 1/e by E (Figure 5.). With reference to Figure 1. and figure 2. we can define as the product IR x C. This quantity is deduced as Ω x As/V = Vs/V = s(econds). Periodically one sees the expression ohm-farad (ΩF) or the somewhat awkward megohm-microfarads (MΩF). Instead of using the expression IR x C it’s customary to mention only the RC product of the capacitor. Then R is understood as IR, i.e. IR x C = RC = τ .
τ = RC (s) or (ΩF) ………….[1]
Figure 5. Illustration of the time constant
The material’s dielectric strength is determined by the breakdown voltage and is expressed in kV/cm. As time, temperature, and other factors determine the breakdown voltage, this is reflected in conditions for measurements of the dielectric withstanding voltage, DWV. They are performed at a specified temperature, material thickness, frequency and shape of test voltage curve, and connection method. DWV usually is determined as an average value of a set of samples due to the effects of material variations etc.
Corona voltage
A practical and important limit for the breakdown voltage is the corona voltage, i.e., where the corona starts appearing. Corona is initial electrical discharges in gases which then are ionized. The ionized products in the air or in carbon-rich environments, typical in all microcavities or voids in the dielectrics as well as in large cavities within the component package, consist of ozone and nitrous fumes. Most organic dielectrics are directly affected by degradation. If the gaseous products have been created within a hermetically-sealed package as their concentration increases, they will degrade the behavior of organic dielectrics. Remember that AC peak voltages just above the corona voltage every half-cycle give a new contribution to the corona products. Additionally, there is a heat release from the corona phenomenon, further accelerating the chemical decomposition.
On the whole, there is a certain smallest field strength
needed in the cavity to start ionization. Moreover, the ionization gap length comes into play. But even if the field strength according to the formula C1-6 should be considerably higher in one part of a mixed dielectric AC, voltages below 250 V R.M.S. are harmless also in the most unfavorable case. On one condition: No incoming transients that otherwise might start an ionization course of events should be allowed. Hence we ought to create safe margins based on our knowledge of occurring transients. If unsure, one should use capacitors where the voltage is distributed over elements connected in series.
Transients and anomalies in the dielectric are a dangerous combination.
Figure 6. A partially mixed dielectric consisting of a layered composite of the organic dielectric and of the gases in the void
The following example will demonstrate the danger. For the sake of simplicity, the measurements and dielectric constants are chosen as in Figure C6. From general formula we obtain εr1 x E1 = εr2 x E2; 1 x E1 = 3 x E2; E1 = 3E2. Here we unintentionally have an electric field strength three times the rated one. ”Safe” rated AC voltages just below 250 V or incoming transients certainly will start the corona in such a void.
In high-voltage ceramic capacitors intended for high-reliability systems, a testing and screening technique detect voids and delaminations by evoking partial discharges (corona). The method uses preferentially AC
voltages just above the corona inception voltage (CIV) and can detect voids exceeding EIA-469 size requirements.
Test voltage
The test voltage is a practical guarantee value of the capacitor. It is positioned well below the corona voltage and is applied for a specific limited time, e.g., 2 seconds at production control and 1 minute at type tests and incoming inspection. Common test voltages maybe 1.5 x VR, 2 x VR, etc.
Capacitor Breakdown Types
There are two basic types of capacitor breakdowns:
(I) Electrical breakdown
During electrical breakdown, the electrical field, usually related to the excessive voltage applied, exceeds the dielectric material’s electrical strength, resulting in complete disruption and low resistance / short circuit failure mode. The responsible conductivity mechanism is mostly the tunneling of electrons or holes accelerated by an electrical field over the critical value. An avalanche effect may then lead to destruction and catastrophic failure – a short circuit of the capacitor.
Critical specification parameters are Rated AC/DC Voltage, Category Voltage (maximum voltage at defined temperature).
(II) Thermal breakdown
During thermal breakdown electrical field is lower than a critical value (applied voltage lower than rated voltage), but the excessive current is flowing through the capacitor – either as high ripple current, transient current, or in reverse mode (polarized capacitors). Joule heating is caused by passing recent increases in local temperature inside of the capacitor structure up to thermal damage and disruption of its materials.
Critical specification parameters are Maximum ripple current/voltage, Maximum power rating, Maximum dV/dt or dI/dt transient or minimum series resistance of the circuit.
Electrical Breakdown Test
Capacitor, electrical breakdown value, may not be such an exact parameter as one could expect. The critical parameter is the applied electrical field on the dielectric, but apart from the ambient temperature, the state of the dielectric / energy dissipation may also depend on time and history (inner temperature due to past events, moisture, etc).
For electrical breakdown, we can consider the following test procedures that, in some capacitor technologies, may give different breakdown voltage values:
1] Static Breakdown
On the external power supply, we set up a maximum current limitation and then increase the voltage from the rated voltage by small increments to minimize transient current until breakdown occurs. This can be done manually, but it is better to do this by a more sophisticated programmable power supply or even automatic breakdown measurement systems that preciously detect the BDV voltage by change of dI/dt.
2] Dynamic Breakdown
During dynamic breakdown high power, the pulse is applied to the capacitor through a low series resistance. Caution: the circuit has to reflect the maximum transient voltage/current limitation conditions not to cause a thermal breakdown.
The test sequence is usually automated in that we apply a certain amount of pulses at a desired voltage (such as 1.1xVr) and then if the capacitor survives we move to one step higher voltage ( for example 1.2xVr) until the breakdown of the capacitor. … again this can be fully automated using programmable power supplies.
3] Self-healing Suppressed Dynamic Breakdown
This test is identical to the dynamic breakdown as above, just the change is that we will replace the samples after each voltage step. This is relevant for capacitor technologies with self-healing as we want to suppress capacitors’ ruggedization by a self-healing process in the previous load step. Target is to get the impression of its BDV robustness when an uneven spike happens in real operation (without any conditioning by aging).
Differences between the BDV induced by the above methods depend on the capacitor technology. There would be practically no difference on air/vacuum capacitors, little on electrostatic capacitors, and more remarkable on electrolytic capacitors with self-healing where obviously the Static BDV > Dynamic BDV > Dynamic Breakdown without history.
Resource: Passive components Blog
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