Sensors and Actuators

Chapter 7
Temperature, Optical, Chemical, and Environmental Sensors

Bachelor Program in Mechatronics Engineering
Sensors and Actuators   •   Bachelor

Temperature, Optical, Chemical, and Environmental Sensors

Introduction

Sensors convert physical, chemical, or biological quantities into signals that can be measured, processed, and used for control. In mechatronic systems, temperature, light, gas concentration, humidity, and biological variables influence safety, energy consumption, product quality, and machine performance. These sensors are often exposed to contamination, vibration, electromagnetic interference, changing ambient conditions, and chemically aggressive environments. Consequently, sensor selection is not based only on nominal accuracy. The engineer must also consider selectivity, response time, calibration stability, installation, signal conditioning, maintenance, and failure modes.

This chapter examines thermocouples, resistance temperature detectors (RTDs), thermistors, infrared detectors, photodiodes, fiber-optic sensors, humidity and gas sensors, electrochemical sensors, and biosensors. Although their physical principles differ, the design questions are similar: What quantity is actually being measured? How does the sensor respond? What unwanted variables influence the output? How quickly must the measurement be available? How will contamination and aging be detected?

Learning objectives

By the end of this chapter, the reader should be able to:

  1. Explain the operating principles of major temperature, optical, chemical, and environmental sensors.
  2. Select an appropriate sensor using range, sensitivity, accuracy, response time, selectivity, and environmental constraints.
  3. Apply basic sensor equations and signal-conditioning methods.
  4. Explain the effects of contamination, drift, hysteresis, self-heating, emissivity, and cross-sensitivity.
  5. Design a practical measurement chain including calibration, filtering, diagnostics, and safe installation.
  6. Evaluate an integrated sensing solution for a realistic mechatronic application.

1. Sensor performance concepts

1.1 Sensitivity, range, resolution, and accuracy

Sensitivity is the change in output per unit change in measurand. For a sensor with output y and input x, local sensitivity is

a = dy/dx

where a is sensitivity, dy is a small output change, and dx is a small input change. The equation is a local approximation and is most useful when the sensor characteristic is approximately linear over the operating interval.

Accuracy describes closeness to the accepted value, whereas precision describes repeatability. Resolution is the smallest input change that can be distinguished, including the effects of sensor noise and electronics. A high-resolution instrument can still be inaccurate if it has an uncorrected calibration error.

A useful first-order model is

y = y0 + Sx + e

where y0 is the offset, S is sensitivity, and e represents error and noise. Real sensors may require nonlinear calibration, temperature compensation, or a dynamic model.

1.2 Dynamic response

Many sensors behave approximately as first-order systems. If the input changes suddenly, the output can be represented by

y(t) = yf + [y(0) − yf]e^(−t/τ)

where yf is the final output, y(0) is the initial output, and τ is the time constant. At t = τ, the output has completed approximately 63.2% of its total change; at about 4.6 time constants it has reached 99%. The model assumes linear behavior, constant parameters, and a single dominant time constant. A protective sheath, stagnant fluid, or poor thermal contact can increase τ.

There is always a trade-off between protection and speed. A thick metal thermowell protects a sensor but increases thermal inertia. A membrane may provide chemical selectivity but slow diffusion.

1.3 Selectivity and interference

Selectivity is the ability to respond predominantly to the target quantity. It is not the same as absolute specificity. Gas sensors, for example, may respond to several gases with different sensitivities. Interference can be reduced by selective membranes, catalysts, optical wavelengths, temperature compensation, reference channels, signal-processing models, and periodic calibration.

Contamination may create a bias rather than random noise. Dust on an optical detector reduces received light; condensation changes infrared transmission; oil on a humidity sensor can block water diffusion; and fouling on an electrochemical electrode changes reaction kinetics. A maintenance plan should therefore include inspection, cleaning rules, recalibration intervals, and plausibility checks.

2. Temperature sensors

Temperature sensing is central to motor protection, battery management, process control, refrigeration, additive manufacturing, and human-machine safety. The major choices are thermocouples, RTDs, thermistors, and non-contact infrared sensors.

2.1 Thermocouples

A thermocouple consists of two dissimilar conductors joined at a measuring junction. The Seebeck effect produces a thermoelectric voltage related to the temperature difference between the measurement junction and the reference junction. In general,

V = ∫[Tref to Tmeas] SAB(T)dT

where V is thermoelectric voltage, SAB(T) is the temperature-dependent Seebeck coefficient of conductor pair A–B, and Tmeas and Tref are measurement and reference temperatures. The integral is required because sensitivity is not perfectly constant.

A thermocouple does not directly measure an absolute temperature; it measures a difference. Modern instruments use cold-junction compensation to measure the reference-junction temperature and infer the measuring-junction temperature from standardized calibration tables or polynomial approximations. Common types include Type K for broad industrial use, Type J for moderate-temperature applications, and Type T for low-temperature work. The permissible range and accuracy depend on wire materials, insulation, sheath construction, and standards.

Advantages include low cost, ruggedness, small thermal mass, and operation at high temperatures. Limitations include low output voltage, nonlinear response, reference-junction requirements, drift from oxidation or contamination, and susceptibility to electrical noise. Extension wires must match the thermocouple type or use suitable compensating cable.

2.2 Resistance temperature detectors

An RTD uses the predictable change in resistance of a metal, commonly platinum. Over a moderate range, a linear approximation is

R(T) = R0[1 + α(T − T0)]

where R(T) is resistance at temperature T, R0 is resistance at reference temperature T0, and α is the temperature coefficient in °C⁻¹. For platinum, T0 is commonly 0 °C and α is approximately 0.00385 °C⁻¹ for the widely used IEC platinum standard. At wider ranges, a standard polynomial such as the Callendar–Van Dusen relationship is required rather than the linear approximation.

For a Pt100 sensor, R0 = 100 Ω. At 100 °C using the linear approximation,

R = 100[1 + 0.00385(100 − 0)] = 138.5 Ω

This value is an approximation; certified calculations should use the applicable standard polynomial.

RTDs provide good accuracy, stability, and near-linearity. Two-wire connections include lead resistance in the measurement. Three-wire circuits compensate approximately for equal lead resistances, while four-wire circuits measure the sensing resistance with minimal lead-error influence. Constant-current excitation is common, but excitation causes self-heating. The power dissipated is

P = I²R

where P is heating power, I is excitation current, and R is sensor resistance. The current should be low enough that the resulting temperature rise is acceptable.

2.3 Thermistors

Thermistors are semiconductor resistors with a large temperature coefficient. Negative-temperature-coefficient (NTC) thermistors decrease in resistance as temperature increases. A common model is

R(T) = R0 exp[B(1/T − 1/T0)]

where temperatures T and T0 are absolute temperatures in kelvin, R0 is resistance at T0, and B is the material constant in kelvin. Kelvin must be used in this equation.

Thermistors are inexpensive and highly sensitive over a limited range. Their strong nonlinearity requires a lookup table, polynomial, or linearization circuit. Self-heating can be significant because thermistors often have high resistance and are operated with measurable voltage. They are common in battery packs, HVAC equipment, laboratory instruments, and electronic temperature compensation.

2.4 Comparing contact temperature sensors

SensorMain strengthMain limitationTypical use
ThermocoupleWide range and ruggednessLow output; reference compensationFurnaces, engines, process equipment
RTDAccuracy and long-term stabilityMore expensive; slower in protective probesProcess control, precision measurement
NTC thermistorHigh sensitivity and low costStrong nonlinearity and self-heatingConsumer equipment, batteries
Infrared detectorNon-contact measurementEmissivity, obstruction, and ambient effectsMoving, hot, or inaccessible targets

3. Optical sensors

Optical sensors measure radiation intensity, wavelength, phase, polarization, or time of flight. They are valuable where electrical isolation, high speed, small size, or non-contact measurement is required.

3.1 Infrared temperature detectors

Every object above absolute zero emits thermal radiation. A simplified radiative relation is

P = εσA(T⁴ − Tsur⁴)

where P is net radiative power, ε is emissivity, σ is the Stefan–Boltzmann constant, A is viewed area, T is target absolute temperature, and Tsur is surrounding absolute temperature. This idealized expression assumes diffuse surfaces and a defined radiative exchange geometry. Real infrared thermometers use wavelength bands, optics, detector characteristics, atmospheric corrections, and emissivity settings.

Emissivity is especially important. A matte painted surface generally has higher emissivity than polished metal. If the instrument is configured for an emissivity that differs from the target, the inferred temperature may be substantially wrong. Reflected radiation from hot surroundings can also be interpreted as target radiation. Steam, dust, smoke, windows, and condensation may attenuate or alter the signal.

Infrared detectors include thermopiles, pyroelectric detectors, and semiconductor photodetectors. A pyroelectric detector responds primarily to changes in radiation, making modulation or target motion useful. A thermopile can measure steady radiation and is often used in non-contact thermometers.

Best practice includes measuring a known reference, controlling the field of view, avoiding shiny surfaces where possible, selecting an appropriate spectral band, and checking whether the target completely fills the measurement spot.

3.2 Photodiodes

A photodiode converts incident optical power into photocurrent. In a useful operating range,

Iph = R_λ Popt

where Iph is photocurrent, R_λ is responsivity in A/W at wavelength λ, and Popt is incident optical power. Responsivity depends on wavelength, bias, temperature, and device construction.

In photovoltaic mode the diode operates near zero bias, giving low noise but limited speed. In photoconductive mode reverse bias reduces junction capacitance and increases speed, but dark current and noise may increase. A transimpedance amplifier converts photocurrent to voltage:

Vout = −Iph Rf

where Rf is feedback resistance. The amplifier must be selected for input capacitance, bandwidth, stability, and leakage-current effects.

Photodiodes are used in encoders, optical switches, barcode readers, pulse oximeters, and fiber communication receivers. Ambient light can saturate the detector; modulation and synchronous detection help distinguish the desired source from background illumination.

3.3 Fiber-optic sensors

Optical fibers transmit light through a core surrounded by lower-refractive-index cladding. Sensors may be intrinsic, where the measurand affects light inside the fiber, or extrinsic, where the fiber carries light to and from an external sensing element. Measurement principles include intensity attenuation, wavelength shift, interferometry, and fiber Bragg gratings.

A fiber Bragg grating reflects a narrow wavelength band. Strain and temperature shift its Bragg wavelength according to

λB = 2neffΛ

where λB is Bragg wavelength, neff is effective refractive index, and Λ is grating period. Changes in strain or temperature alter neff and/or Λ. A reference grating or separate temperature measurement is needed when strain and temperature both vary.

Fiber sensors provide electrical isolation, immunity to electromagnetic interference, and suitability for high-voltage or explosive environments. Their limitations include interrogation-system cost, bending losses, connector contamination, and cross-sensitivity.

4. Humidity and gas sensors

4.1 Humidity measurement

Relative humidity is defined as

RH = 100 × pv/psat(T)

where pv is actual water-vapor partial pressure and psat(T) is saturation vapor pressure at temperature T. Relative humidity is therefore temperature-dependent even when the amount of water vapor remains constant.

Capacitive humidity sensors use a moisture-sensitive dielectric whose permittivity changes with absorbed water. Resistive sensors measure a humidity-dependent resistance. Thermal-conductivity sensors infer gas composition from heat transfer and can be used for absolute humidity or gas mixtures under controlled conditions.

Condensation, dust, oil, chemical vapors, and rapid temperature changes can cause hysteresis or inaccurate readings. A humidity sensor should be located where air exchange represents the process, while avoiding direct water droplets and localized heat sources. Dew-point calculations require temperature compensation because a warm sensor exposed to cooler moist air may temporarily report misleading relative humidity.

4.2 Gas sensors

Important gas-sensing technologies include metal-oxide semiconductor (MOS), catalytic bead, nondispersive infrared (NDIR), photoionization detector (PID), and electrochemical sensors.

MOS sensors change resistance when gases react with an oxide surface. They are relatively inexpensive but often require a heater and show strong cross-sensitivity to humidity, temperature, and multiple gases. Catalytic bead sensors oxidize combustible gases on a heated catalyst and are useful for flammability monitoring, but oxygen concentration and catalyst poisoning affect the response.

NDIR sensors measure gas absorption at characteristic infrared wavelengths. A simplified transmission relationship is the Beer–Lambert law:

I = I0 exp(−αcL)

where I0 is incident intensity, I is transmitted intensity, α is absorption coefficient, c is concentration, and L is optical path length. The model assumes a defined wavelength, homogeneous gas, and negligible scattering. Reference channels help compensate for lamp aging, dust, and optical fouling.

PIDs use ultraviolet radiation to ionize compounds with suitable ionization potentials. They are sensitive to many volatile organic compounds but do not identify every gas uniquely. Sensor selection must therefore reflect the actual hazard and required selectivity.

5. Electrochemical sensors and biosensors

5.1 Electrochemical measurement

Electrochemical sensors use electrodes and an electrolyte to convert chemical activity into voltage or current. Potentiometric sensors measure a potential difference under approximately zero current. Amperometric sensors hold a controlled electrode potential and measure reaction current. Conductometric sensors measure changes in ionic conductivity.

For a reversible ion-selective electrode, the Nernst relationship is

E = E⁰ + (RT/zF) ln a

where E is electrode potential, E⁰ is a reference constant, R is the gas constant, T is absolute temperature, z is ion charge, F is Faraday’s constant, and a is ion activity. Concentration may replace activity only when activity coefficients are adequately controlled or approximated. The relationship assumes equilibrium and a stable reference electrode.

Amperometric current depends on electrochemical reaction rate and mass transport. Membranes and diffusion barriers can improve selectivity and define response time, but they also reduce signal magnitude and slow response. Electrodes may foul, dry out, polarize, or suffer from electrolyte evaporation.

5.2 Biosensors

A biosensor combines a biological recognition element with a transducer. Recognition elements include enzymes, antibodies, nucleic acids, receptors, and whole cells. The transducer may be electrochemical, optical, thermal, or piezoelectric.

A glucose enzyme electrode, for example, uses an enzyme such as glucose oxidase to recognize glucose and produces an electrochemical signal through a reaction product or mediator. The biological element supplies selectivity, but temperature, pH, oxygen concentration, interfering compounds, immobilization quality, and enzyme aging affect the result.

Biosensors require careful control of sample handling. A sensor may be analytically accurate in a clean buffer but unreliable in blood, wastewater, or food because proteins and particulates foul the surface. Disposable membranes, anti-fouling coatings, blank measurements, and matrix-matched calibration are practical responses.

6. Signal conditioning, calibration, and diagnostics

A sensor is part of a measurement chain: sensing element, excitation, analog conditioning, analog-to-digital conversion, software, communication, and decision logic. Common conditioning functions include amplification, filtering, linearization, isolation, cold-junction compensation, bridge completion, and open-circuit detection.

Filtering must be matched to the process. A low-pass filter suppresses high-frequency noise but delays the signal. For a first-order digital exponential filter,

yk = βxk + (1 − β)yk−1

where xk is the current sample, yk is the filtered output, and β lies between 0 and 1. Larger β responds faster but smooths less. Filtering should never conceal a dangerous rapid rise in temperature or gas concentration.

Calibration establishes the relation between indicated output and a reference. A two-point linear calibration can be written as

x = x1 + (y − y1)(x2 − x1)/(y2 − y1)

where (x1,y1) and (x2,y2) are two reference points and y is the measured output. This is appropriate only when the sensor is sufficiently linear over the interval. Multi-point calibration or a lookup table is preferable for thermistors, infrared instruments, and many chemical sensors.

Diagnostics should identify open circuits, short circuits, implausible rates of change, saturation, disagreement between redundant sensors, and calibration expiration. Safety-related systems should use independent measurement paths where a single sensor failure could create unacceptable risk.

7. Selection framework for mechatronic systems

A systematic selection process is more reliable than choosing a sensor from nominal accuracy alone.

  1. Define the measurand and measurement location. Specify temperature, pressure, composition, optical geometry, and expected transients.
  2. Establish the required range, uncertainty, resolution, response time, and allowable loading.
  3. Identify environmental conditions: vibration, shock, humidity, dust, chemicals, radiation, electromagnetic fields, and hazardous-area classification.
  4. Evaluate selectivity and interference. Ask which substances, surfaces, temperatures, or light sources can produce a false signal.
  5. Select the interface: voltage, current loop, resistance, frequency, digital bus, or optical interrogator.
  6. Plan calibration, cleaning, replacement, and verification.
  7. Analyze failure modes and define alarms and safe states.
  8. Confirm applicable standards and documentation.

Industrial installations may require conformity with electrical safety, electromagnetic compatibility, hazardous-location, machinery, and functional-safety requirements. Gas and biosensor applications may also involve occupational exposure limits, medical-device rules, or laboratory quality systems. The exact requirements depend on jurisdiction and application; standards should be consulted rather than assumed.

8. Illustrative case: monitoring a lithium-ion battery module

Background

A battery module in an autonomous mobile robot contains multiple cells, a liquid-cooling plate, and a battery-management controller. Excessive cell temperature accelerates degradation and can contribute to thermal runaway. The module also operates near electric motors that generate electromagnetic noise.

Problem

The design team initially proposes one inexpensive NTC thermistor on the cooling plate. Analysis shows that the plate temperature may lag the hottest cell, and one sensor cannot identify a disconnected or locally damaged measurement path.

Analysis

The required system must detect slow thermal rise for charge control and rapid abnormal rise for protection. It must tolerate vibration, electrical noise, and limited space. A thermocouple offers a wide range but requires additional cold-junction compensation. An RTD offers stability but may be physically larger and more expensive. NTC thermistors offer high sensitivity and compact packaging, but self-heating and nonlinear conversion must be managed.

Approach and solution

The design uses several bonded NTC thermistors distributed across the module, with one sensor near the cell group most likely to become hot. Each channel uses a low excitation current and a calibrated lookup table. The controller checks for open-circuit resistance, short-circuit resistance, disagreement between adjacent sensors, and an implausibly rapid temperature change. A redundant sensor technology, such as a small digital temperature sensor or RTD on a reference location, is used during validation rather than relying solely on software filtering.

The sensors are electrically separated from high-current paths, wiring is routed to reduce induced noise, and the thermal interface is specified so that adhesive thickness is controlled. Calibration is performed at several temperatures, including the expected operating range. The protection strategy has two levels: controlled derating for a sustained high temperature and immediate shutdown for a validated rapid rise or sensor disagreement.

Outcome

The distributed arrangement detects spatial gradients that a single plate sensor would miss. Low excitation reduces self-heating, while plausibility checks reveal wiring faults. The system is not made safe merely by adding sensors: enclosure venting, cell balancing, charging limits, and an independent protection path remain necessary.

Learning points

The case demonstrates that sensor choice is a system-design decision. Spatial placement, thermal coupling, failure detection, response time, calibration, and consequences of error are as important as nominal accuracy.

9. Contemporary developments and professional practice

Modern sensors increasingly combine local processing, digital calibration, self-test, and network connectivity. Multispectral infrared systems can distinguish temperature from emissivity effects more effectively than single-band instruments. Fiber-optic arrays provide distributed monitoring in structures and high-voltage equipment. Machine-learning models can classify gas mixtures or compensate for drift, but they require representative training data and must not replace physical safeguards without validation.

Sensor data should be traceable: record calibration date, sensor identity, environmental conditions, firmware version, and maintenance history. Cybersecurity matters when sensors are connected to industrial networks. Authentication, controlled updates, access management, and plausibility monitoring reduce the risk that corrupted data will cause unsafe actuation. In safety-critical systems, a black-box prediction should not be the sole basis for an emergency decision unless its performance, limits, and failure behavior have been rigorously established.

Chapter Summary

Temperature sensors exploit thermoelectric voltage, resistance change, or semiconductor behavior. Thermocouples are rugged and wide-ranging but require reference-junction compensation. RTDs offer stable, accurate resistance measurement, while thermistors provide high sensitivity at the cost of nonlinearity and self-heating. Infrared sensors enable non-contact measurement but depend strongly on emissivity, field of view, and optical conditions.

Photodiodes convert optical power to current, and fiber-optic sensors provide electrical isolation and immunity to electromagnetic interference. Humidity sensors respond to water content through dielectric, resistive, or thermal effects. Gas sensors include MOS, catalytic, NDIR, PID, and electrochemical technologies, each with different selectivity and interference behavior. Electrochemical sensors use potential, current, or conductivity; biosensors add biological recognition elements but require control of fouling, matrix effects, and biological stability.

Successful deployment requires more than selecting a sensing principle. The engineer must manage response time, contamination, calibration, environmental effects, signal conditioning, diagnostics, safety, and lifecycle maintenance. Distributed and redundant sensing, reference channels, physical safeguards, and documented calibration improve reliability.

Key Terms

Sensitivity: Change in sensor output per unit change in measurand.

Accuracy: Closeness of a measurement to an accepted reference value.

Resolution: Smallest distinguishable change in the measured quantity.

Time constant: Time for a first-order response to reach approximately 63.2% of its final change.

Thermocouple: Temperature sensor based on thermoelectric voltage from dissimilar conductors.

Cold-junction compensation: Correction for the reference-junction temperature of a thermocouple.

RTD: Resistance temperature detector using a temperature-dependent metal resistance.

Thermistor: Semiconductor resistor with a large temperature coefficient.

Emissivity: Ratio describing a surface’s thermal radiation relative to an ideal blackbody.

Photodiode: Semiconductor device that converts incident light into photocurrent.

Responsivity: Photocurrent produced per unit incident optical power.

Fiber Bragg grating: Periodic fiber structure that reflects a wavelength dependent on grating properties.

Relative humidity: Water-vapor partial pressure expressed as a percentage of saturation pressure.

Cross-sensitivity: Response to quantities other than the target measurand.

NDIR sensor: Gas sensor using wavelength-specific infrared absorption.

Potentiometric sensor: Electrochemical sensor measuring equilibrium potential.

Amperometric sensor: Electrochemical sensor measuring current at controlled potential.

Biosensor: Sensor combining biological recognition with a physical transducer.

Self-heating: Temperature or measurement error caused by sensor excitation power.

Calibration: Establishment of a relationship between sensor output and reference quantity.

Review Questions

Short Answer Questions

  1. Why does a thermocouple require cold-junction compensation?
  2. State two advantages and two limitations of RTDs.
  3. What is emissivity, and why does it matter in infrared temperature measurement?
  4. Distinguish potentiometric and amperometric electrochemical sensors.
  5. Explain why contamination can produce a systematic sensor error.

Long Answer Questions

  1. Compare thermocouples, RTDs, and NTC thermistors for industrial temperature control, including range, accuracy, response time, conditioning, and failure modes.
  2. Explain the operation of photodiodes and fiber Bragg grating sensors and discuss their applications in mechatronics.
  3. Compare MOS, NDIR, PID, catalytic, and electrochemical gas sensors with respect to selectivity, response time, maintenance, and environmental sensitivity.
  4. Develop a calibration and diagnostic strategy for a humidity or temperature measurement subsystem.
  5. Explain the main design challenges of biosensors in real samples and propose methods for controlling fouling and matrix effects.

Analytical / Application Questions

  1. A process requires non-contact measurement of a polished metal surface in an area containing hot equipment and dust. Select an infrared measurement strategy and identify the corrections and validation tests required.
  2. A gas monitor shows a slow concentration increase after a filter becomes visibly dirty. Determine whether the likely error is contamination, cross-sensitivity, sensor aging, or a real process change, and design a diagnostic experiment.
  3. Design a temperature-monitoring architecture for a battery module in which a single sensor failure must not prevent protective shutdown. Justify sensor type, placement, excitation, calibration, filtering, and voting or plausibility logic.

Multiple Choice Questions with Answers

Question 1

Which temperature sensor directly produces a voltage related primarily to the temperature difference between two junctions?

A. RTD

B. Thermocouple

C. NTC thermistor

D. Capacitive humidity sensor

Correct Answer: B. Thermocouple

Question 2

For a Pt100 RTD, using the linear approximation with α = 0.00385 °C⁻¹, what is the resistance at 100 °C?

A. 100.0 Ω

B. 103.85 Ω

C. 138.5 Ω

D. 385.0 Ω

Correct Answer: C. 138.5 Ω

Question 3

In the equation R(T) = R0 exp[B(1/T − 1/T0)], temperatures must be expressed in:

A. Degrees Celsius only

B. Degrees Fahrenheit only

C. Kelvin

D. Percent relative humidity

Correct Answer: C. Kelvin

Question 4

Which factor is especially important when using an infrared thermometer on a shiny metal surface?

A. Emissivity

B. Lead resistance

C. Cold-junction voltage

D. Electrolyte concentration

Correct Answer: A. Emissivity

Question 5

A photodiode with responsivity 0.5 A/W receives 2 mW of optical power. What photocurrent is predicted by the linear model?

A. 0.001 A

B. 0.0015 A

C. 0.01 A

D. 1 A

Correct Answer: A. 0.001 A

Question 6

Which gas-sensing method is based most directly on wavelength-specific infrared absorption?

A. NDIR

B. Catalytic bead

C. Potentiometric ion electrode

D. Thermistor

Correct Answer: A. NDIR

Question 7

Relative humidity is defined using the ratio of water-vapor partial pressure to:

A. Atmospheric pressure at sea level

B. Saturation vapor pressure at the same temperature

C. Gas constant times temperature

D. Oxygen partial pressure

Correct Answer: B. Saturation vapor pressure at the same temperature

Question 8

Which electrochemical sensor measures current while an electrode potential is controlled?

A. Potentiometric sensor

B. Amperometric sensor

C. Conductometric sensor

D. Thermocouple

Correct Answer: B. Amperometric sensor

Question 9

At one time constant in an ideal first-order sensor response, approximately what fraction of the final change has occurred?

A. 10.0%

B. 37.0%

C. 63.2%

D. 99.9%

Correct Answer: C. 63.2%

Question 10

Which design measure most directly reduces the effect of ambient light on a photodiode measurement?

A. Increasing thermocouple wire length

B. Using optical modulation and synchronous detection

C. Increasing RTD lead resistance

D. Removing all calibration points

Correct Answer: B. Using optical modulation and synchronous detection

Sensors and Actuators
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