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How does a thermocouple work as a temperature measurement device?

Short Answer

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Question: Explain the working principle of a thermocouple as a temperature measurement device. Answer: A thermocouple works based on the Seebeck effect, which generates a voltage proportional to the temperature difference between a sensing and reference junction, both formed by connecting two different metal wires. The generated voltage is measured at the reference junction, which is kept at a known and constant temperature. The temperature at the sensing junction is then calculated using thermocouple characteristics, which involve thermocouple tables or mathematical algorithms, enabling accurate temperature measurement at the desired location.

Step by step solution

01

Thermocouple Materials and Components

A thermocouple is made of two wires made of different metals, typically alloys such as chromel-alumel, iron-constantan, or copper-constantan, connected at one end to form a junction. This junction, usually called the sensing junction, is placed at the location where temperature needs to be measured. The other ends of the wires are connected to a measuring device, and this junction is called the reference junction.
02

The Seebeck Effect

The thermocouple works based on the Seebeck effect, which states that when two different conductors are connected at two different junctions, and one junction is kept at a higher temperature than the other junction, a voltage is generated proportional to the difference between the temperatures of the two junctions. It's important to note that the voltage generated is a function of the temperature difference between the sensing junction and the reference junction.
03

Measuring the Voltage

At the reference junction, the voltage generated by the Seebeck effect is measured using a voltmeter or a microprocessor-based system. The reference junction is usually kept at a known and constant temperature, such as 0°C by using an ice bath.
04

Converting Voltage to Temperature

As the voltage generated is a function of the temperature difference between the sensing and reference junctions, and we have the value of the reference junction temperature, we can determine the temperature at the sensing junction. The voltage-temperature relationship is known as the thermocouple characteristic, and it's unique for each thermocouple type. Thermocouple tables or mathematical algorithms are used to convert the measured voltage into the temperature of the sensing junction, thus deriving the temperature at the desired location. In summary, a thermocouple uses the Seebeck effect to generate a voltage based on the temperature difference between the sensing junction and the reference junction. By measuring this voltage, the temperature at the sensing junction can be calculated using the thermocouple characteristics, allowing for accurate temperature measurement.

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Most popular questions from this chapter

How do we achieve very low temperatures with gas refrigeration cycles?

Refrigerant-134a enters the compressor of a refrigerator as superheated vapor at \(0.20 \mathrm{MPa}\) and \(-5^{\circ} \mathrm{C}\) at a rate of \(0.07 \mathrm{kg} / \mathrm{s},\) and it leaves at \(1.2 \mathrm{MPa}\) and \(70^{\circ} \mathrm{C}\). The refrigerant is cooled in the condenser to \(44^{\circ} \mathrm{C}\) and \(1.15 \mathrm{MPa}\), and it is throttled to 0.21 MPa. Disregarding any heat transfer and pressure drops in the connecting lines between the components, show the cycle on a \(T\) -s diagram with respect to saturation lines, and determine ( \(a\) ) the rate of heat removal from the refrigerated space and the power input to the compressor, \((b)\) the isentropic efficiency of the compressor, and \((c)\) the \(C O P\) of the refrigerator.

A refrigerator operates on the ideal vapor compression refrigeration cycle with \(\mathrm{R}-134 \mathrm{a}\) as the working fluid between the pressure limits of 120 and 800 kPa. If the rate of heat removal from the refrigerated space is \(32 \mathrm{kJ} / \mathrm{s}\), the mass flow rate of the refrigerant is \((a) 0.19 \mathrm{kg} / \mathrm{s}\) \((b) 0.15 \mathrm{kg} / \mathrm{s}\) \((c) 0.23 \mathrm{kg} / \mathrm{s}\) \((d) 0.28 \mathrm{kg} / \mathrm{s}\) \((e) 0.81 \mathrm{kg} / \mathrm{s}\)

A heat pump that operates on the ideal vaporcompression cycle with refrigerant-134a is used to heat a house. The mass flow rate of the refrigerant is \(0.25 \mathrm{kg} / \mathrm{s}\) The condenser and evaporator pressures are 1400 and \(320 \mathrm{kPa}\) respectively. Show the cycle on a \(T\) -s diagram with respect to saturation lines, and determine ( \(a\) ) the rate of heat supply to the house, \((b)\) the volume flow rate of the refrigerant at the compressor inlet, and \((c)\) the COP of this heat pump.

It is proposed to use a solar-powered thermoelectric system installed on the roof to cool residential buildings. The system consists of a thermoelectric refrigerator that is powered by a thermoelectric power generator whose top surface is a solar collector. Discuss the feasibility and the cost of such a system, and determine if the proposed system installed on one side of the roof can meet a significant portion of the cooling requirements of a typical house in your area.

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