What Capacitor Series Resistance Is and How It Appears in Standard Hardware
The series resistance of capacitor (ESR) is internal resistance causing voltage drop, heat, and weaker filtering in standard hardware. Learn how it impacts circuits.
The series resistance of a capacitor — called equivalent series resistance, or ESR — is the internal resistance that appears in series with an ideal capacitor. Every real capacitor carries it. This parasitic appears in standard hardware as voltage drop, heat, and weaker filtering; a single ohm of this resistance can cost one volt of headroom under load. This is not a defect; it is an unavoidable trait of construction.
The series resistance of a capacitor matters most in high-frequency circuits, where low impedance magnifies losses. The adverse effects of the series resistance of a capacitor include switching ripple and wasted power inside the part. The series resistance of a capacitor shifts with frequency and temperature, so the datasheet gives only one snapshot. Measuring impedance across operating conditions and treating a high series resistance of a capacitor as a diagnostic clue helps engineers find warm, unstable supplies.
Key Takeaways
- Every real capacitor contains ESR, equivalent series resistance. This internal resistance causes voltage loss, heat, weaker filtering.
- Capacitor ESR changes with frequency, temperature, age. Always compare readings under identical test conditions. A single datasheet value cannot cover all cases.
- High ESR creates output ripple, warm capacitor cases, unstable voltage. Watch for these warning signs. These symptoms point to supply problems.
- A rising ESR value often signals a failing capacitor. Replace the part above the datasheet limit. A new low-ESR capacitor restores stable power.
- Measure ESR with a meter, LCR bridge, impedance analyzer. Low ESR parts reduce heat, restore stable voltage. Choose replacement parts within datasheet limits.
Defining the Series Resistance of Capacitor
Ideal Capacitor vs. Real Capacitor
An ideal capacitor stores energy with zero loss. Its equivalent series resistance (ESR) is zero, and its inductance is zero. It behaves as a purely capacitive component at every frequency. A real capacitor cannot match that model. Every physical part has internal resistance from leads, electrodes, and dielectric material. The dielectric, plate material, electrolytic solution, and terminal leads all contribute at a particular frequency. In circuit analysis, the capacitor's impedance is written as Z = R + jX, where R is the real-valued resistance and X is the reactance. The series resistance of capacitor is exactly that real part. Engineers call it the in-phase AC resistance because it dissipates energy instead of storing it.
That resistance comes from identifiable sources. Metal foils, internal tabs, and terminals contribute electrode and termination resistance. Wet aluminum electrolytic capacitors add electrolyte resistance, whose conductivity shifts with temperature. Dielectric loss also dissipates energy. The capacitor's series resistance is the sum of these losses.
| Physical source | Contribution |
|---|---|
| Electrode and termination resistance | Metal foils, internal tabs, electrodes, and terminals add resistance in the current path. |
| Electrolyte resistance | In wet aluminum electrolytic capacitors, ionic resistance can dominate ESR and varies with temperature. |
| Dielectric loss | Energy loss inside the dielectric adds to the dissipation factor. |
In a non-electrolytic capacitor and electrolytic capacitors with solid electrolyte, metallic resistance of leads and electrodes plus dielectric losses cause the ESR. Aluminum and tantalum electrolytic capacitors with non-solid electrolyte have much higher ESR values, up to several ohms; electrolytics of higher capacitance show lower ESR.
Capacitor ESR vs. ESL
A real capacitor includes another parasitic: equivalent series inductance, or ESL. The series resistance of capacitor causes resistive loss, while ESL shifts behavior at high frequency. Comparing capacitor ESR vs. ESL means separating these two effects. This equivalent series resistance is not a fixed datasheet point. Both parasitic elements sit in series with the ideal capacitance, but they act differently. At low frequency, the impedance is capacitive. Near self-resonance, capacitive and inductive reactances cancel, so the effective ESR and impedance reach their minimum, and the part becomes a pure resistor. Above self-resonance, ESL dominates, so the component turns inductive. For example, a capacitor used in a power supply carries ripple current through this resistance, producing waste heat.
Total capacitor impedance in an AC circuit is Z = sqrt(ESR² + (XL - XC)²). At self-resonance, XL = XC, so Z = ESR. The dissipation factor is DF = tan δ = ESR / XC, and Q = 1 / tan δ. The capacitor ESR depends on operating frequency and temperature, so a single number cannot describe every situation. High capacitor ESR increases loss, ripple, and heating. Low capacitor ESR improves ripple-current handling, stabilizes output voltage, and extends component life. When capacitor ESR rises, filtering quality falls.
An ESR value from a datasheet describes only one frequency and temperature point. The ESR and impedance of a real part shift with frequency, temperature, and age. Always compare datasheet values under identical test conditions. A rising internal resistance is a reliable warning sign of failing hardware.
How Capacitor ESR Appears in Standard Hardware
Ripple, Heating, and Filtering Loss
Output ripple voltage under load is a direct result of capacitor ESR. In a switch-mode power supply, high equivalent series resistance causes increased output voltage ripple. This elevated ripple appears as voltage fluctuations at the output, which can degrade the performance and reliability of the powered electronic circuits. For electrolytic capacitors in a switch-mode power supply, ESR becomes the dominant factor in determining output voltage ripple. When calculating the minimum capacitance needed to mitigate ripple, the ESR is so predominant that the capacitance value can be ignored, and only the ESR is used in the calculation.
If Iripple ≈ 0.5 A at 500 kHz and we target ΔVESR ≤ 10 mV, the total ESR should be ≤ 20 mΩ: ESR ≤ ΔVESR / Iripple = 0.01 / 0.5 = 0.02 Ω
A buck converter output ripple calculation treats the ESR contribution separately from the capacitance-dependent part. In one example design, the two are assumed to contribute equally, giving 16.5 mV for the ESR-induced portion. The capacitance-based ripple calculation assumes an ideal capacitor, so the actual output voltage ripple will be higher in practice because real capacitors introduce parasitic ESL and ESR. Capacitor ESR is therefore a direct source of additional output ripple.
Self-heating follows the power loss formula P = I²rms × ESR. The temperature rise is proportional to the ESR, so a higher ESR produces more heat. The dissipated power causes the capacitor to warm up.
| Parameter | Value/Relationship |
|---|---|
| Self-heating formula | ΔT = I²rms × ESR |
| Power loss formula | P = I²rms × ESR |
| Test capacitor | CL21B223KCFNNNF |
| Ripple current | 100 mA at 100 kHz |
| Temperature rise | 5–10 °C |
| Extreme cumulative energy dissipation | Several hundred milliwatts |
| Maximum operating temperature | 125 °C |
The equivalent series resistance of the CL21B223KCFNNNF arises from dielectric material loss and electrode metal resistance. At low frequencies, dielectric loss dominates; at high frequencies near or above self-resonance, electrode resistance becomes primary. Typical ESR values range from tens of milliohms at low frequencies to hundreds of milliohms at high frequencies. ESR generates heat when the component carries AC or ripple current. It also contributes to voltage ripple and affects high-frequency impedance.
Decoupling and LDO Stability
Reduced decoupling and filtering effectiveness is another practical consequence. A high-esr capacitor cannot shunt high-frequency noise to ground effectively, so supply rails carry more noise into sensitive loads. Low esr parts improve ripple-current handling and stabilize output voltage. The LDO closed-loop system has two main poles: the internal pole formed by the error amplifier and pass transistor, and the external pole associated with the output capacitor's esr. The ESR of the output capacitor affects the stability of the LDO control loop. A minimum ESR of 1 Ω or less is recommended to ensure stability. The output capacitor also influences transient response: a larger output capacitor can improve the LDO's response to rapid load-current changes, but it may increase start-up time. Good-quality ceramic capacitors can be used if they meet the LDO datasheet's minimum capacitance and maximum ESR specifications; X5R or X7R dielectrics are recommended because of their good temperature stability and low voltage coefficient.
Nova Technology Company (HK) Limited, a HiSilicon-designated (authorized) solutions partner, supports chip-level power supply design, decoupling, and signal integrity work for system integration teams.
Capacitor ESR Changes With Frequency and Temperature
Capacitor ESR is not a constant. It shifts with frequency, temperature, and age. Engineers must compare measured values under the same operating conditions. A reading taken at one frequency tells nothing about behavior at another.
Frequency-Dependent Behavior
The series resistance of capacitor falls as frequency rises in aluminum electrolytic parts. Ohmic losses in the aluminum oxide layer decrease at higher frequencies. The 120 Hz point serves as the standard measurement frequency for aluminum electrolytics under IEC 60384-4. Many datasheet values are specified there. The 100 kHz point is common for low-resistance electrolytics and meter measurements.
Above 100 kHz, capacitor ESR behaves differently by technology. Aluminum electrolytic ESR increases with frequency, which raises losses and lowers efficiency. Ceramic MLCC parts keep ESR in the milliohm range. Designers often pair electrolytics with ceramics for high-frequency filtering.
Below self-resonance, the impedance falls as frequency rises. At self-resonance, impedance reaches its minimum and equals ESR. Above self-resonance, impedance rises because parasitic inductance dominates. This resistance also increases from skin effect and proximity effects. This impedance shift makes capacitor ESR especially problematic in high-frequency circuits.
Temperature and Aging Effects
Low temperature raises capacitor ESR sharply in aluminum electrolytics. Between 25°C and -55°C, electrolyte resistivity can increase by a factor of about 100. At the low-temperature limit, this resistance can be more than ten times its normal value. A capacitor rated at -20°C operated at -40°C can more than double its resistance.
Heat and age drive this resistance upward over time. Electrolyte evaporation is the primary cause. Capacitor life approximately halves for every 10°C rise above the rated temperature. Ripple current heats the capacitor core and speeds electrolyte loss. This ripple current stress creates a feedback loop: a higher resistance causes more heating, which raises it further. Electrolytics in switch-mode power supplies handle continuous ripple current. Typical failure timelines run 5–10 years in consumer electronics. A single ESR value cannot describe every situation. Always check the datasheet for acceptable limits and compare measurements at the same frequency and temperature as the datasheet specification.
Good Capacitor ESR Values and Measurement
Typical ESR Ranges by Technology
A good capacitor esr value depends on the family. Standard aluminum electrolytics run 7–30 Ω at low frequency and 2–7 Ω at high frequency. Low-ESR aluminum parts drop to 1–5 Ω and 0.3–1.6 Ω. Solid aluminum sits at 0.2–0.5 Ω. Sanyo OS-CON reaches 0.04–0.07 Ω and 0.03–0.06 Ω.
| Capacitor family | Typical ESR |
|---|---|
| Standard aluminum | 7–30 Ω (low freq), 2–7 Ω (high freq) |
| Low-ESR aluminum | 1–5 Ω (low freq), 0.3–1.6 Ω (high freq) |
| Solid aluminum | 0.2–0.5 Ω |
| Sanyo OS-CON | 0.04–0.07 Ω, 0.03–0.06 Ω |
For 100 µF/10–16 V parts at 100 kHz and 20°C, typical values are 800 mΩ for standard aluminum, 360 mΩ for low-ESR aluminum, 400 mΩ for solid aluminum, and 25 mΩ for Sanyo OS-CON. A 1000 µF electrolytic shows 0.05 Ω at 10 V and rises to 0.7 Ω at 450 V. Low-ESR secondary capacitors in power supplies usually stay well below 1 Ω when healthy.
As a rough guide: a 1000µF/25V electrolytic should have ESR below 0.1Ω. If your reading is more than 2-3x the typical value for that capacitance/voltage, the capacitor is degraded and should be replaced.
Datasheets and Measurement Tools
A datasheet may state ESR directly, list impedance at 100 kHz, give tan δ, or quote a ripple-current rating. The rated ripple current and ripple current rating hint at ESR capability. Compare any specified esr at the same frequency and temperature, because the maximum esr limit shifts with both. Smaller cases carry higher ESR for the same capacitance.
A handheld esr meter sends a short current pulse or a low-voltage AC signal near 100 kHz, so semiconductor junctions stay off and in-circuit checks work. An LCR meter with four-wire Kelvin leads removes contact resistance; use series mode for low-impedance parts. An impedance analyzer sweeps frequency and shows the full curve. Discharge the capacitor first, zero the probes, then compare the reading against the datasheet.
Symptoms of High-ESR Capacitors in Real Hardware
Rising internal resistance shows up in the output waveform, the case temperature, and the stability of the supply.
| Symptom | Consequence |
|---|---|
| Excessive voltage ripple | Filtering loses effectiveness, so AC ripple reaches the load |
| Overheating | Power dissipated inside the part raises its temperature |
| Unstable output voltage | Supply output fluctuates under constant load |
| Power supply will not start | Failed part prevents the PSU from powering on |
Excessive Ripple and Warm Capacitors
Output ripple is the first visible sign. When capacitor esr climbs, the capacitor can no longer smooth voltage fluctuations. A buck converter output may show a sawtooth-like waveform that should be nearly flat. The power loss equation P = I²rms × ESR explains the heating. Ripple current in capacitor esr generates heat.
Murata sets a self-heating limit for ceramic capacitors. At 25°C ambient, its body temperature rise should stay below 20°C. A sustained rise above that limit indicates excessive ripple current. The higher esr creates a feedback loop: more heat evaporates electrolyte, and electrolyte loss raises resistance further. Each additional ripple current heats the core and accelerates electrolyte loss.
Unstable Supplies and Early Failure
Unstable output voltage is the next symptom. A high-esr capacitor cannot hold the rail steady during load steps. The supply may sag, oscillate, or fail to start. Low esr types hold the rail firm and support stable regulation. In LDO circuits, the output capacitor esr can shift the control-loop phase margin and cause oscillation.
The datasheet gives safe operating boundaries. Check the ripple-current rating in the datasheet; this value defines safe ripple current at a reference frequency. The ripple current rating tells how much AC current the part can tolerate. Power supplies that handle continuous ripple current stress the output part. If the esr value exceeds the datasheet limit, replace the part. A low esr replacement restores filtering. A high-esr capacitor that remains installed will overheat and fail.
An impedance analyzer can identify the problem. Measure the part at the same frequency used in the datasheet. The capacitor esr rises with age. Treat that esr climb as an early warning and replace the component before the power supply fails.
Every real capacitor carries ESR, an unavoidable parasitic resistance in series with the ideal capacitance. Its practical consequences are consistent: voltage drop under load, internal heating, weaker filtering, and possible instability in supplies and regulators. This is why capacitor ESR matters in nearly every hardware design.
Capacitor ESR also varies with frequency, temperature, and age. Comparisons only hold under identical conditions. Check the datasheet, measure impedance when possible, and treat a rising capacitor ESR as a likely cause of common hardware failures.
FAQ
What exactly is capacitor ESR?
Capacitor ESR is the real-valued resistance in series with the ideal capacitance. It comes from electrode resistance, electrolyte resistance, termination resistance, and dielectric loss. This esr dissipates energy as heat instead of storing it. Every real capacitor has it, and it directly affects filtering and voltage stability.
How do I know if an ESR value is too high?
Compare the reading against the datasheet limit at the same frequency and temperature. A 1000 µF/25 V electrolytic should stay below 0.1 Ω. If the measured value is two to three times the typical figure for that capacitance and voltage, the capacitor is degraded and should be replaced.
Does ESR matter at low frequencies?
Yes, but less than at high frequencies. Standard aluminum electrolytics show 7–30 Ω at low frequency. At 120 Hz, ESR still causes ripple and heating. However, impedance falls as frequency rises, so the same part performs better at higher frequencies until self-resonance.
How do I measure capacitor ESR?
Use an ESR meter for quick in-circuit checks near 100 kHz. An LCR meter with four-wire Kelvin leads removes contact resistance. An impedance analyzer sweeps frequency for the full curve. Always discharge the capacitor first, then compare the reading against the datasheet at the specified test conditions.
Can I replace a high-ESR capacitor with a low ESR type?
Yes, and you often should. A low esr replacement restores filtering and reduces heating. Check the datasheet for minimum capacitance and maximum ESR limits, especially in LDO circuits. Ceramic capacitors with X5R or X7R dielectrics work well if they meet the regulator's stability requirements.







