What Is an RTD and How Does It Work?

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Temperature Measurement
What Is an RTD?

An RTD (Resistance Temperature Detector) measures temperature through the predictable change in electrical resistance of a metal as it heats up.

A transmitter converts this resistance change into a standard 4-20 mA signal for the control system.

This guide covers the working principle, construction types, wiring configurations, key parameters, and how to select the right RTD for your application.

Pt100 and Pt1000 Wire-Wound vs Thin-Film 2, 3 and 4-Wire IEC 60751 Standard

The sensor works on a simple principle: the electrical resistance of a pure metal increases linearly with temperature. Platinum is the preferred material because it is chemically stable, highly pure, and produces a well-defined, reproducible resistance-temperature relationship defined by IEC 60751.

RTD Working Principle: How Resistance Changes with Temperature

Hello! Today we are covering this sensor in detail: what it is, how it works, how it is constructed, and how to choose the right one for industrial temperature measurement. It is one of the most accurate and stable temperature sensors available, and understanding the RTD is fundamental to any instrumentation engineer's knowledge base.

Every metal contains a lattice of positively charged atoms. When current flows, electrons move through this lattice. At higher temperatures, the atoms vibrate more intensely and collide more frequently with passing electrons, increasing the opposition to current flow. This opposition is called resistance.

Three properties make this measurement accurate: a predictable temperature coefficient of resistance (TCR), a stable linear response, and low self-heating error. Click any term to expand.

Temperature Coefficient of Resistance (TCR or α): The fractional change in resistance per degree Celsius, referenced to 0°C. For IEC 60751 platinum RTDs, α = 0.00385 Ω/Ω/°C. This means for every 1°C rise, the resistance increases by 0.385% of its value at 0°C. A Pt100 increases from 100 Ω at 0°C to 138.5 Ω at 100°C. This relationship is described by the Callendar-Van Dusen equation and tabulated in IEC 60751.
Linear Response: Platinum resistance increases nearly linearly with temperature across the industrial measurement range (minus 200°C to 600°C). The small non-linearity is corrected by the Callendar-Van Dusen coefficients embedded in the transmitter or DCS input card software. The user sees a linear, directly displayed temperature value. This linearity makes this sensor far easier to use than a thermocouple, which has a non-linear millivolt output that varies by type.
Self-Heating Error: The excitation current required to measure the sensing element resistance also dissipates power in the sensing element (P = I² × R). This raises the element temperature above the process temperature, introducing a positive measurement error. For a Pt100 with 1 mA excitation current: P = (0.001)² × 100 = 0.1 mW. In a good installation with adequate heat transfer to the process fluid, this error is less than 0.1°C. In stagnant gas or vacuum installations, self-heating can be significant and the excitation current should be reduced.
0.00385
TCR (α) of IEC 60751 platinum RTDs in Ω/Ω/°C (the international standard)
100 Ω
Pt100 resistance at 0°C (ice point). Pt1000 = 1000 Ω. Resistance increases with temperature.
±0.1°C
Typical accuracy of a Class B Pt100 RTD at 0°C per IEC 60751
1 mA
Typical excitation current supplied by a transmitter to measure RTD resistance
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RTD Construction: Wire-Wound vs Thin-Film

The sensing element is made by forming a length of pure platinum wire or film into a defined geometry on a substrate. The two main construction types are wire-wound and thin-film. Each has distinct advantages for different applications.

FeatureWire-Wound RTDThin-Film RTD
ConstructionFine platinum wire coiled around a ceramic or glass mandrel and potted in protective powderThin platinum layer deposited on a ceramic substrate by sputtering, then laser-trimmed to exact resistance
Temperature rangeMinus 200°C to 850°CMinus 50°C to 500°C (standard); specialist types to 600°C
AccuracyHighest: Class AA and Class A tolerances achievableGood: Class B standard; Class A available in premium types
Vibration resistancePoor: wire can deform under vibration, changing resistanceExcellent: the thin film is bonded directly to the substrate
Response timeSlower: larger thermal massFaster: smaller element with lower thermal mass
CostHigherLower: suitable for high-volume applications
Typical useLaboratory, calibration standards, high-accuracy process measurements above 300°CIndustrial process control, HVAC, food processing, pharmaceutical

RTD Resistance Formula

The Callendar-Van Dusen equation gives the exact resistance at any temperature. For most industrial purposes above 0°C, the linear approximation is accurate to within 0.4% up to 400°C.

RTD Linear Approximation (0°C to 400°C)
R(T) = R₀ × (1 + α × T)
R(T): resistance at temperature T (Ω)
R₀: nominal resistance at 0°C (100 Ω for Pt100, 1000 Ω for Pt1000)
α: temperature coefficient = 0.00385 Ω/Ω/°C (IEC 60751)
T: temperature in °C

Pt100 at 200°C: R = 100 × (1 + 0.00385 × 200) = 100 × 1.77 = 177.0 Ω
Pt1000 at 200°C: R = 1000 × (1 + 0.00385 × 200) = 1770.0 Ω

The transmitter stores the Callendar-Van Dusen coefficients and applies the non-linear correction automatically. The engineer enters only the sensor type and range.

See the Pt100 calibration guide for the resistance-to-temperature table used during calibration.

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RTD Wiring Configurations: 2-Wire, 3-Wire and 4-Wire

Lead wire resistance adds to the measured resistance and causes a positive temperature error. The wiring configuration determines how much of this error is compensated. See the sensor connections guide for full wiring diagrams for each configuration.

2-Wire RTD

Simplest wiring. The transmitter measures lead wire resistance plus sensing element. Lead error cannot be separated.nnot be separated. A 1 Ω lead causes approximately 2.6°C error in a Pt100.

Use only with very short cables (under 2 m) or with a Pt1000 where the relative lead error is smaller.

3-Wire RTD

The most common industrial configuration. A third wire allows the transmitter to measure one lead and subtract it from both sides of the bridge.

Requires all three wires to be identical. Standard for industrial Pt100 installations with cable runs up to 50 m.

4-Wire RTD

Two wires carry excitation current; two separate wires measure voltage across the element only. Lead resistance is completely eliminated regardless of cable length.

Used for laboratory reference standards and measurements requiring accuracy better than 0.1°C. See the platinum RTD advantages guide.

Transmitter in Head (Head-Mount)

A compact transmitter mounted in the sensor connection head. The short element-to-transmitter distance eliminates lead resistance. The transmitter outputs 4-20 mA over the loop cable.

The preferred configuration for new installations, removing the need for special extension cable. See the temperature transmitter guide.

Resistance and Temperature Calculator

Resistance and Temperature Calculator
Calculate resistance from temperature or temperature from measured resistance
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Sensor Material Types and Temperature Ranges

MaterialNominal R at 0°CRangeTCR (α)Application
Platinum (Pt)100 Ω (Pt100) or 1000 Ω (Pt1000)Minus 200°C to 850°C0.00385 Ω/Ω/°CAll industrial and laboratory applications. Most accurate and stable.
Nickel (Ni)100 Ω or 120 ΩMinus 60°C to 250°C0.00617 Ω/Ω/°CHVAC, refrigeration, lower cost applications where full platinum accuracy is not needed
Copper (Cu)10 ΩMinus 200°C to 260°C0.00427 Ω/Ω/°CMotor winding temperature monitoring; linear but less stable than platinum
Nickel-Iron (Ni-Fe)604 ΩMinus 100°C to 200°C0.00518 Ω/Ω/°CBridge circuits and specific military applications
Platinum is the material of choice for this sensor because it is chemically inert (does not react with most process fluids), can be manufactured in very high purity (99.999%), has a highly reproducible resistance-temperature relationship, and is stable at high temperatures. The IEC 60751 standard defines the exact resistance-temperature table for platinum RTDs with α = 0.00385. See the thermocouple vs RTD guide for when to use a thermocouple instead.

IEC 60751 Accuracy Classes per IEC 60751

IEC 60751 defines four accuracy classes for platinum RTDs. The class applies to the sensing element only, not to the complete measurement chain including the transmitter and lead wires.

ClassTolerance at 0°CTolerance FormulaTypical Use
AA±0.1°C±(0.1 + 0.0017 × |T|)Laboratory reference standards, primary calibration
A±0.15°C±(0.15 + 0.002 × |T|)High accuracy process measurement, precision calibration
B±0.3°C±(0.3 + 0.005 × |T|)Standard industrial process control (most common)
C±0.6°C±(0.6 + 0.01 × |T|)General purpose, non-critical temperature indication

Class B is the default for most industrial Pt100 and Pt1000 sensors. At 100°C, Class B tolerance = ±0.8°C. Specify Class A for critical measurements.

See the temperature transmitter calibration guide for the full verification procedure.

Watch: What Is an RTD and How Does It Work?

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RTD Sensor Questions

What does RTD stand for and how does it measure temperature?
RTD stands for Resistance Temperature Detector. It measures temperature by detecting the change in electrical resistance of a metal (usually platinum). A small excitation current is passed through the sensor and the resulting resistance is measured.
What is the difference between Pt100 and Pt1000 RTDs?
Both are platinum RTDs with TCR 0.00385 Ω/Ω/°C. Pt100 = 100 Ω at 0°C, Pt1000 = 1000 Ω. The Pt1000 is ten times more sensitive and less affected by lead resistance.
Why is a 3-wire connection preferred for industrial installations?
The 3-wire transmitter measures one lead resistance and subtracts it from both sides of the bridge, compensating for lead error. A 2-wire RTD includes lead resistance in the reading causing a positive temperature error.
What temperature range does a platinum RTD cover?
Wire-wound Pt100 sensors cover minus 200°C to 850°C per IEC 60751. Thin-film Pt100 sensors are typically rated to 500°C or 600°C. For temperatures above 600°C, a thermocouple is the appropriate sensor choice.
How is an RTD different from a thermocouple?
An RTD measures resistance changes and needs an excitation current. A thermocouple generates a millivolt signal and needs no excitation. RTDs are more accurate; thermocouples cover higher temperatures and respond faster. See the thermocouple vs RTD guide.

External References

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What We Learn Today

  • An RTD (Resistance Temperature Detector) measures temperature through the predictable increase in electrical resistance of a metal as temperature rises
  • Platinum is the standard RTD material: Pt100 (100 Ω at 0°C) and Pt1000 (1000 Ω at 0°C) follow IEC 60751 with TCR = 0.00385 Ω/Ω/°C
  • Wire-wound RTDs offer higher accuracy and wider range (to 850°C); thin-film types offer faster response, better vibration resistance, and lower cost
  • The 3-wire configuration compensates for lead resistance and is the industrial standard. The 4-wire configuration eliminates lead error completely for highest accuracy.
  • IEC 60751 accuracy classes: AA (±0.1°C), A (±0.15°C), B (±0.3°C), C (±0.6°C), all measured at 0°C
  • Platinum RTDs are more accurate and stable than thermocouples. Thermocouples cover higher temperatures and respond faster. Choose based on the application requirements.
“This temperature sensor is not a complex device. It is a length of pure platinum wire that gets slightly harder to push electrons through as it gets warmer. Everything else, accuracy, stability, repeatability, follows from that simple and predictable relationship.”

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