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Tolerance, Accuracy and Error

No component is perfect. A resistor marked 100 Ω may actually be 102 Ω. A capacitor rated at 100 nF might measure anywhere from 80 nF to 120 nF. Your multimeter shows 5.00 V, but the real voltage might be 4.97 V. Understanding tolerance, accuracy and error is what separates a circuit that always works from one that works on your bench but fails for a customer, in the cold, or after six months. This lesson explains the concepts, the numbers, and how to work with them.

What you will learn: Component tolerance and how it is specified, the difference between accuracy and precision, measurement resolution and error types, how to calculate percentage error, temperature coefficient and how it affects components over temperature, and how to apply worst-case thinking to circuit design.

What is tolerance?

Tolerance is the allowed deviation of a component's actual value from its stated (nominal) value. A 100 Ω resistor with ±5% tolerance may have any actual resistance between 95 Ω and 105 Ω and still be within specification. The manufacturer guarantees it will be in that range; they make no promise beyond that.

Tolerance is not a defect or a sign of poor quality — it is an engineering choice that balances cost against precision. Tighter tolerances require tighter manufacturing processes and cost more. For many applications, 5% or 10% tolerance is perfectly adequate. For filter networks, oscillator tuning circuits, and measurement equipment, 1% or better may be essential.

Example: A 1 kΩ resistor with ±10% tolerance:
Minimum value: 1000 − (1000 × 0.10) = 1000 − 100 = 900 Ω
Maximum value: 1000 + (1000 × 0.10) = 1000 + 100 = 1100 Ω

Resistor tolerance grades

Through-hole resistors indicate their tolerance with a colour band. In a four-band resistor, the fourth band is the tolerance band:

Tolerance band colourToleranceTypical use
Brown±1%Precision circuits, filters, measurement
Red±2%Precision circuits
Gold±5%General purpose (most common)
Silver±10%Non-critical applications
None (no band)±20%Very non-critical; rarely seen now

Five-band and six-band resistors are used for 1% and tighter tolerances. They use an extra digit band for the resistance value. Six-band resistors add a sixth band for temperature coefficient.

Precision 1% resistors are available in the E96 series, which has 96 values per decade (compared to 12 for the E12 series used for 10% parts). The finer spacing of E96 values means you can hit almost any target resistance using a single component.

Four-band resistor colour code diagram with the fourth (tolerance) band highlighted and gold (±5%), silver (±10%) and brown (±1%) bands labelled

The tolerance band is always the last band on a four-band resistor — separated from the value bands by a slightly larger gap. Gold (±5%) is the most common; brown (±1%) identifies a precision part.

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Capacitor tolerance codes

Capacitors use letter codes for tolerance, particularly on small ceramic and film capacitors where there is no room for a colour band:

Letter codeTolerance
B±0.1 pF (absolute, for small capacitors)
C±0.25 pF (absolute)
D±0.5 pF (absolute)
F±1%
G±2%
J±5%
K±10%
M±20%
Z−20% / +80% (electrolytic capacitors)

Note that electrolytic capacitors often have asymmetric tolerance (e.g. −20% / +80% or −10% / +50%). The nominal capacitance can vary significantly; for decoupling and filtering applications this is usually acceptable, but for tuned circuits you need tighter tolerance types such as ceramic NP0/C0G or film capacitors.

Accuracy vs precision

These two words are often used interchangeably in everyday language, but in metrology (the science of measurement) they have distinct meanings:

  • Accuracy is how close a measured or stated value is to the true value. A highly accurate component has a value very close to its marked value.
  • Precision is how consistent or repeatable a value is. A precise instrument gives the same reading every time, even if that reading is not the true value.

The classic analogy uses a target:

  • Accurate and precise: all shots clustered tightly near the bullseye
  • Precise but not accurate: all shots clustered tightly, but far from the bullseye (systematic error)
  • Accurate but not precise: shots scattered randomly, but centred around the bullseye on average (random error)
  • Neither accurate nor precise: shots scattered randomly and off-centre

In electronics, a resistor with excellent precision but poor accuracy would produce the same value in every unit, but that value might be well off the marked nominal. A high-quality 1% resistor is both accurate (close to nominal) and precise (consistent unit to unit).

Four-panel target diagram showing: top-left — accurate and precise (tight cluster on bullseye); top-right — precise but not accurate (tight cluster off-centre); bottom-left — accurate but not precise (scattered around bullseye); bottom-right — neither accurate nor precise (scattered and off-centre)

The four combinations of accuracy and precision. A well-calibrated, tight-tolerance component is both — it hits near the true value consistently. Systematic error shifts the cluster off-centre; random error spreads it out.

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Resolution

Resolution is the smallest change an instrument can detect or display. A digital multimeter that reads to 0.001 V has a resolution of 1 mV. It cannot tell the difference between 4.9991 V and 4.9994 V — both will display as 4.999 V.

Resolution is not the same as accuracy. A meter might have 0.001 V resolution but only ±0.5% accuracy. Its displayed reading of 5.000 V could represent a true voltage anywhere from 4.975 V to 5.025 V. The fine resolution gives you confidence about changes, not about the absolute value.

Types of error

Measurement errors fall into two broad categories:

Systematic error (bias)

An error that consistently pushes the measurement in one direction. Examples: a miscalibrated meter that always reads 2% high; a thermometer that always reads 1°C above true temperature; a component that was stored incorrectly and aged to a shifted value. Systematic errors cannot be reduced by averaging multiple measurements — they affect every reading equally.

Random error

An error that varies unpredictably from measurement to measurement. Examples: electrical noise on a sensitive measurement; thermal fluctuations in a component's value; quantisation noise in a digital instrument. Random errors can be reduced by averaging multiple measurements — the errors partly cancel.

Calculating percentage error

Percentage error tells you how far a measured or actual value is from the expected value, expressed as a proportion of the expected value:

Percentage error = ((Measured − True) / True) × 100%

Example: A resistor is marked 470 Ω. You measure it at 483 Ω.
Percentage error = ((483 − 470) / 470) × 100% = (13 / 470) × 100% ≈ +2.8%
This is within the ±5% tolerance band, so the resistor is in spec.
Example: A frequency counter reads 14.225 MHz. The actual frequency (referenced to a GPS-disciplined oscillator) is 14.220 MHz.
Percentage error = ((14.225 − 14.220) / 14.220) × 100% = (0.005 / 14.220) × 100% ≈ +0.035%
= 350 ppm

Temperature coefficient

Most component values change with temperature. The temperature coefficient describes how much the value changes per degree Celsius of temperature change. It is typically abbreviated TC or TCR (Temperature Coefficient of Resistance) for resistors.

A positive temperature coefficient (PTC) means the value increases with temperature. A negative temperature coefficient (NTC) means it decreases.

Component / TypeTypical temperature coefficient
Carbon composition resistor−500 to −200 ppm/°C (large, unpredictable)
Carbon film resistor−200 to −100 ppm/°C
Metal film resistor (standard)±100 ppm/°C
Metal film resistor (precision)±10 to ±25 ppm/°C
Wirewound resistor±20 to ±50 ppm/°C
Ceramic capacitor (X5R, X7R)±15% change over rated temperature range
Ceramic capacitor (NP0/C0G)<30 ppm/°C — very stable
Electrolytic capacitorHighly variable; can change >20% from −40°C to +85°C
Crystal oscillator (AT-cut)±2 to ±5 ppm over industrial temperature range
TCXO (temperature-compensated XO)±0.5 to ±2.5 ppm

Parts per million (ppm)

Parts per million is a convenient way to express very small relative changes. 1 ppm means 0.0001%, or 1 in 1 000 000. It is particularly common for expressing:

  • Crystal and oscillator frequency accuracy: a 10 MHz crystal rated at ±5 ppm can be anywhere from 9.99995 MHz to 10.00005 MHz — a range of just 100 Hz across 10 MHz.
  • Resistor temperature coefficients: a 10 kΩ resistor with a TC of 100 ppm/°C changes by 100 kΩ/°C × 100/1 000 000 = 1 Ω/°C. Over a 50°C temperature change, it shifts by 50 Ω — still less than 1% of its nominal value.
  • Reference voltage stability: a precision voltage reference rated at 5 ppm/°C drifts by just 5 μV per degree Celsius for a 1 V reference.
Conversion: ppm ↔ percentage
1 ppm = 0.0001%
100 ppm = 0.01%
10 000 ppm = 1%

A 25 ppm/°C temperature coefficient over a 40°C range:
Change = 25 × 40 = 1000 ppm = 0.1%

Worst-case analysis

Worst-case analysis is the habit of checking whether your circuit still works correctly when all component tolerances stack up in the most unfavourable direction simultaneously. In a well-designed circuit, the worst-case combination of tolerances still produces acceptable results.

The steps are:

  1. Identify which parameters matter for circuit performance (e.g. output voltage, resonant frequency, gain).
  2. Determine how each component tolerance affects those parameters.
  3. Choose the component values that push the output in the worst direction (all low, all high, or some combination).
  4. Calculate the output for this worst case and check it is still within the acceptable range.
Example: A voltage divider uses two 10 kΩ ±5% resistors from a 5 V supply. The expected output is 2.5 V.
Worst case high: R1 = 9.5 kΩ, R2 = 10.5 kΩ
Vout = 5 × (10.5 / (9.5 + 10.5)) = 5 × 10.5/20 = 2.625 V
Worst case low: R1 = 10.5 kΩ, R2 = 9.5 kΩ;
Vout = 5 × (9.5 / (10.5 + 9.5)) = 5 × 9.5/20 = 2.375 V
So the worst-case output range is 2.375 V to 2.625 V (±5% of 2.5 V). If that is acceptable for your application, 5% resistors are fine. If you need ±1%, use 1% parts.

In ham radio, worst-case thinking matters whenever you are designing frequency-selective circuits (filters, matching networks), reference oscillators, power supply regulators, or measurement bridges. It also comes up when specifying component power ratings — always size resistors and capacitors for the worst-case operating conditions, not the typical ones.

Frequently Asked Questions

Does 1% tolerance mean the component is always close to 1% of nominal?

A 1% tolerance guarantees the value is within ±1% of nominal — it may be exactly on value, slightly off, or at the 1% limit. Most components from quality manufacturers cluster near the centre of the tolerance band, but you cannot rely on that for design purposes. Design to the full ±1% range. The only way to guarantee a tighter actual value is to measure the component before use or buy 0.1% or better parts.

Why do crystals have ppm accuracy ratings rather than percentage?

Because the accuracy is so fine that percentage becomes unwieldy. A crystal rated at ±5 ppm is accurate to ±0.0005%. At 14 MHz, that is a worst-case error of ±70 Hz — small enough that it would almost always read as 0.00% if expressed as a percentage, but significant enough to matter for SSB and digital modes. Parts per million is simply the more practical unit at this level of precision.

Why does capacitance change so much with temperature in ceramic capacitors?

Because most ceramic dielectrics are ferroelectric materials whose permittivity (dielectric constant) changes with temperature, electric field and mechanical stress. Class II ceramics (X5R, X7R, Y5V) are chosen for high capacitance per volume, but they sacrifice stability. Class I ceramics (NP0/C0G) use a different dielectric formulation that is much more stable, but they cannot achieve as high a capacitance per unit volume. For tuned RF circuits and reference networks, always use NP0/C0G capacitors.

Test Your Knowledge

Answer the questions below to check your understanding of this lesson. Every answer can be found in the lesson above.

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