RF Test & Measurement

Bolometer

/buh-lom-ih-ter/
A thermal RF power sensor that absorbs electromagnetic energy and measures the resulting temperature rise to determine incident power. The DC substitution technique (replacing RF heating with equivalent DC power in a balanced bridge) provides NIST-traceable accuracy of ±0.1-1%. Types: thermistor (NTC bead in Wheatstone bridge, -20 to +10 dBm), thermocouple (direct EMF, -30 to +20 dBm), and diode detector (for comparison). Bolometers serve as the primary absolute power standard for national metrology institutes.
Accuracy: ±0.1-1%
Range: -20 to +10 dBm
Standard: NIST-traceable

Understanding Bolometers

The bolometer is the simplest and most fundamental RF power sensor: it converts electromagnetic energy to heat and measures the temperature change. This simplicity is its strength. Unlike diode detectors, which respond to the RF voltage waveform and can give inaccurate readings for complex modulated signals, a bolometer responds to total absorbed power through thermodynamics: every joule of RF energy produces the same heating regardless of frequency, modulation, or waveform shape. This waveform-independent response makes bolometers the ultimate reference for power measurement calibration.

In a thermistor bolometer, a tiny NTC (negative temperature coefficient) bead is mounted inside a coaxial structure designed to absorb all incident RF power. The bead is one arm of a self-balancing Wheatstone bridge. With no RF applied, DC power heats the bead to a stable operating temperature. When RF power is absorbed, the bead temperature rises, its resistance drops, and the bridge feedback reduces DC power to maintain balance. The change in DC power precisely equals the absorbed RF power. This DC substitution principle traces the measurement to DC voltage and current, the most precisely measurable electrical quantities.

Bolometer Measurement Equations

DC substitution principle:
PRF = PDC,initial − PDC,final
PDC = V2/R = I2R

Thermistor sensitivity:
α = (1/R)(dR/dT) ≈ -4%/°C (NTC)
ΔR = R × α × ΔT
ΔT = P / (Gth)
Gth = thermal conductance

Thermocouple EMF:
V = S × ΔT (Seebeck effect)
S ≈ 250 μV/°C (thin-film)

Effective efficiency:
ηe = Psubstituted/Pincident
Accounts for mismatch + mount losses
Typical: 0.95-0.99 (95-99%)

RF Power Sensor Comparison

Sensor TypeRange (dBm)AccuracyResponseWaveformUse Case
Thermistor-20 to +10±0.1-1%msTrue averageCalibration std
Thermocouple-30 to +20±3-5%msTrue averageGeneral RF
Diode (CW)-70 to -20±2-3%μsSq-law onlyLow power CW
Diode (wide)-60 to +20±3-5%μs-nsCorrected avgModulated signals
Calorimeter+20 to +50±0.5%s-minTrue averageHigh power std
Common Questions

Frequently Asked Questions

How does a bolometer measure RF power?

An NTC thermistor bead absorbs RF energy, heating up and changing resistance in a self-balancing Wheatstone bridge. The bridge feedback reduces DC bias power to re-balance. P_RF = P_DC_initial − P_DC_final. This DC substitution traces measurement to DC voltage/current standards, providing ±0.1-1% accuracy. Response is waveform-independent since it measures total absorbed heat.

Why are bolometers used as power standards?

They respond to total absorbed power through thermodynamics, regardless of frequency, waveform, or modulation. DC substitution provides NIST-traceable accuracy by comparing RF heating to precisely measurable DC heating. National labs (NIST, PTB, NPL) maintain microcalorimeter primary standards. Calibration chain uncertainty from NIST to production: 2-5% (0.1-0.2 dB).

What are the different RF power sensor types?

Thermistor: highest accuracy (±1%), limited range (-20 to +10 dBm), slow (ms). Thermocouple: broader range (-30 to +20 dBm), true average, moderate accuracy (±3-5%). Diode: widest range (-70 to +20 dBm), fastest (ns), but accuracy degrades for complex modulated signals above square-law region (-20 dBm). Calorimeter: high power (+20 to +50 dBm), slowest.

RF Metrology

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