HEAT-1
THERMOMETRY
This is the science of temperature and its measurement.
TEMPERATURE
The temperature of a body is a number which expresses its degree of hotness or coldness on some chosen scale.
It is measure of how hot or cold the body is.
THERMOMETERS
A thermometer is an instrument designed to measure the temperature of a body.
Thermometers use some measurable property of a substance (thermometric property) which is sensitive to temperature.
Thermometric property
Is that property in which quantity value of a thermometer varies linearly and continuously with temperature
The thermometric property is also called physical property of a thermometer.
Examples of thermometric properties (physical properties) of a thermometer are:
  1. Length of liquid column in a glass tube
  2. Volume of a gas at constant pressure
  3. Pressure of a gas at constant volume
  4. Electrical resistance of a platinum wire
  5. Electromotive force of a thermo-couple
QUALITIES OF A THERMOMETRIC PROPERTY
A thermometric property must have:
  1. A marked degree of expansion for a small temperature rise
  2. A uniform expansion rate
  3. Good thermo conductivity
  4. High boiling point and low freezing point (if it is liquid)
TEMPERATURE SCALES
  1. CELSIUS SCALE
This is a temperature scale in which the fixed points are the temperatures at standard pressure of ice in equilibrium with water (0WX2VVPp9bBjQZiQYgsMmKy3ldQPfsYm8X UgxtP45mo4XeAGPuKCbVA3yfcCfOpPdujVgLsDhzlXsvSG OJ7tEjextb ItxJ1DcMeXE0an49kDyhIXKpV8epfTF 7gIdBdDNhwQ) and water in equilibrium with steam (100WX2VVPp9bBjQZiQYgsMmKy3ldQPfsYm8X UgxtP45mo4XeAGPuKCbVA3yfcCfOpPdujVgLsDhzlXsvSG OJ7tEjextb ItxJ1DcMeXE0an49kDyhIXKpV8epfTF 7gIdBdDNhwQ)
The scale between these two temperatures is divided into 100 equal parts and each part is called a degree.
The temperature on this scale is expressed in degree Celsius (WX2VVPp9bBjQZiQYgsMmKy3ldQPfsYm8X UgxtP45mo4XeAGPuKCbVA3yfcCfOpPdujVgLsDhzlXsvSG OJ7tEjextb ItxJ1DcMeXE0an49kDyhIXKpV8epfTF 7gIdBdDNhwQ)
  1. FAHRENHEIT SCALE
This is a temperature Scale in which the temperature of boiling water is taken as 212XPp2WjzB Ym0lYENI6IbQXofZUIDxrG9IIs52eTPp0lkteRa RyOk40woYdspu33MUAJdUvGaKBDD70 BkgJ NfWisSLoMltquLAKR4rcOVJs915eOs9DvIbH Li63 Ftm4o2A and the temperature of pure melting ice is taken as 32XPp2WjzB Ym0lYENI6IbQXofZUIDxrG9IIs52eTPp0lkteRa RyOk40woYdspu33MUAJdUvGaKBDD70 BkgJ NfWisSLoMltquLAKR4rcOVJs915eOs9DvIbH Li63 Ftm4o2A
The interval between these two reference temperatures is divided into 180 equal parts and each part is called degree Fahrenheit (XPp2WjzB Ym0lYENI6IbQXofZUIDxrG9IIs52eTPp0lkteRa RyOk40woYdspu33MUAJdUvGaKBDD70 BkgJ NfWisSLoMltquLAKR4rcOVJs915eOs9DvIbH Li63 Ftm4o2A)
To convert this scale into degree centigrade (WX2VVPp9bBjQZiQYgsMmKy3ldQPfsYm8X UgxtP45mo4XeAGPuKCbVA3yfcCfOpPdujVgLsDhzlXsvSG OJ7tEjextb ItxJ1DcMeXE0an49kDyhIXKpV8epfTF 7gIdBdDNhwQ), the formula is:
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  1. THERMODYNAMIC TEMPERATURE SCALE
This is the standard temperature scale adopted for scientific measurement.
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Thermodynamic temperature is denoted by the symbol T and is expressed in Kelvin, K.
The lowest possible temperature which can be measured by this scale is assigned the value zero (OK) called absolute zero
It is the lowest temperature theoretically attainable at which the random motion of molecules and atoms in a substance is at minimum.
The temperature of a substance cannot be lowered further by decreasing the random motion.
Thermodynamic temperature is also called absolute temperature. The degree centigrade is equal in magnitude to temperature in Kelvin i.e a change of temperature in WX2VVPp9bBjQZiQYgsMmKy3ldQPfsYm8X UgxtP45mo4XeAGPuKCbVA3yfcCfOpPdujVgLsDhzlXsvSG OJ7tEjextb ItxJ1DcMeXE0an49kDyhIXKpV8epfTF 7gIdBdDNhwQ is equal to a change of temperature in Kelvin.
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NECESSARY CONDITIONS FOR THE TEMPERATURE SCALE TO BE ESTABLISHED
In order to establish a temperature scale one requires;
(1) SOME PHYSICAL PROPERTY OF A MATERIAL
The physical property of a material should vary linearly and continuously with temperature.
Examples
  1. The length of liquid column in a glass tube varies linearly and continuously with temperature.
Length temperature Image?w=87&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
Image?w=58&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
= k + 0 Image?w=87&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
Image?w=93&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
Compare y = + Image?w=68&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
This is a linear relationship
  1. The volume of a gas at constant
    pressure varies linearly and continuously with temperature.
Volume temperature Image?w=93&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
Image?w=56&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw V T
    • V = K T + 0
    Image?w=102&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
    Compare y = + Image?w=73&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
    This is a linear relationship
    1. The pressure of a gas at constant volume varies linearly and continuously with temperature
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    Image?w=53&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw P T
      • P = K T + 0
      Image?w=102&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Compare y = + Image?w=73&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      This is a linear relationship
      (2) FIXED POINTS
      A fixed point is a temperature that can be accurately reproduced to enable it to be used as a basis of a temperature scale.
      It is a single temperature at which it can confidently be expected that a particular physical event ( e.g the melting of ice under specific conditions) always takes place.
      The three fixed points are:
      1. Ice point
      Is the temperature at which pure ice can exist in equilibrium with water pure at standard atmospheric pressure (i.e. at 760mmHg).
      1. Steam Point
      Is the temperature at which pure water can exist in equilibrium with its vapor at standard atmospheric pressure.
      1. Triple point
      Is that unique temperature at which vapor, liquid and solid phases of a substance exist in equilibrium.
      The triple point is particularly useful, since there is only one pressure at which all three phases (solid, Liquid and gas) can be in equilibrium with each other.
      Example, For water the triple point is 273.16K and it occurs at a pressure of 611.2Pa
      DISAGREEMENT BETWEEN SCALES
      Different materials do not expand in quite the same way over a wide range of temperatures.
      Thermometric properties do not keep in step as the temperature changes.
      Consequently, if we calibrate different kinds of thermometers by using ice point and steam point as the reference marks they will not agree precisely (accurately).
      Different results are obtained when different kinds of thermometers are used to measure the same temperature except at the calibrated fixed point.
      THE TEMPERATURE SCALE EQUATION
      When there is a change of temperature, the physical property of a material also changes.
      Since the physical property of a material varies linearly and continuously with temperature then we have:
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      Let X be physical property of a material
      Let X0 be physical property of a material at ice point (0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM)
      Temperature
      Physical Property
      0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM
      X0
      100IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM
      X100
      Image?w=28&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
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      CASE 1
      When the temperature changes from 0307nFJ CG20vXnAmYzG34zSRj4OD3aFt Sh6hepiImC52h8Qp0mBB21kyQtGo7v6 YmhkNvq5sgebwjzXx OYrHIwme3bt37ht3olBCT7mK2qkD6VxKmcakiUjQs9EInwLCUAZA to 100307nFJ CG20vXnAmYzG34zSRj4OD3aFt Sh6hepiImC52h8Qp0mBB21kyQtGo7v6 YmhkNvq5sgebwjzXx OYrHIwme3bt37ht3olBCT7mK2qkD6VxKmcakiUjQs9EInwLCUAZA
      Change in temperature = 100 – 0 Image?w=54&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      = 100IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM
      Change in property = Image?w=64&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      But change in temperature PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos change in thermometric property
      100Image?w=105&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw ( )
      100 = K( ) …………………………….(1) Image?w=178&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Where K = constant of proportionality
      CASE 2
      When the temperature changes from 0Image?w=66&h=27&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Change in temperature = Ugk6esMo GMbR AmebpeMdbatzgjfMjNdzmWtl9gun3SUY3Xl9aEUxENXSHrJp0kR0LM6GF93B0JBkC VdwXJhvFIhl9 66O7FORS8rKa1jZKIhNkXDktje0dDVdwRYrFjGJTNQ
      = PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc
      Change of the thermometric property = Image?w=56&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      But change in temperature PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos change in thermometric property
      Image?w=107&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw )
      Image?w=160&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw = ……………………………..(2)
      Where k = constant of proportionality
      Dividing JCImC8eDj7xFMSoVDtGiTs2LC1QiaLNjq0d5NqjbX3aXPmT9BX Tx WUlb 5k0mjOHuoQPWtPD4 JhvLYJHi1HPAdoxKAsItflk9WcEoGTdBKReic5FmHMYWm3F0DmuvV8BFWkM
      Image?w=181&h=35&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw =
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      RELATIONSHIP BETWEEN PHYSICAL PROPERTY OF A MATERIAL AND TRIPLE POINT
      Consider a physical property P of a material which varies linearly and continuously with temperature.
      Let P Trip be physical property of a material at triple point temperature T Trip
      Since change in temperature PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos change in thermometric property we have
      T Trip PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos P Trip
      FarcLQfhDNGDvcqQb8NJf3sfLF0AhKHfYlM3m6Fxk1sLmnOt9mYHp6k6VuDMgVTXFNDxHd5zVBAwmLtYJbZvWc5OoXIupX9 EyKBr5pp5BWdKlJo0NdAtTl71IuEmhOzM1lWwbM T Trip = k P Trip ………………………………….(1)
      Where K = constant of proportionality
      Let PT be physical property of a material at a temperature T (in Kelvin)
      Similarly T PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos PT
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      Dividing JCImC8eDj7xFMSoVDtGiTs2LC1QiaLNjq0d5NqjbX3aXPmT9BX Tx WUlb 5k0mjOHuoQPWtPD4 JhvLYJHi1HPAdoxKAsItflk9WcEoGTdBKReic5FmHMYWm3F0DmuvV8BFWkM
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      Equation (3) above can also be written as:
      T = 2 0i 4Ns4bf4PhX6C WnW4jfDXzpX8XNlvPey 0rbUZN5QLlBDe9tCg5f7r GewIubOU4DyIxnFx7YzKc7CBJNDKj02nYulPZxUoyA0 Qgub65VWT28SK8mD6bNc5XVe58CQXvM x T Trip
      For water T Trip = 273.16K
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      TYPES OF THERMOMETERS
      There are so many types of thermometers but they all have common fact that they depend on some physical property of a material which changes with temperature.
      Some important thermometers are: – (i) Liquid in glass thermometers
      1. Gas thermometers
      2. Platinum resistance thermometers
      3. Thermocouple thermometers
      4. Radiation thermometers (Pyrometers)
      (i)LIQUID IN GLASS THERMOMETERS
      One of the most familiar thermometer uses mercury as a thermometric liquid
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      In this type of thermometer the length of mercury in a glass tube is the thermometric property of a material when the temperature changes.
      This means that in the temperature scale equation, H06AfGQ58m8rP89AhTWWP1GzUx U4ZDd8iu 9 Yuyookrzrn A A PbbjO5sk03uAyL2BaAsa U5lXsp1ji5GqYxiFZOtj6 B7v4l4qOt W8eLmzGNneYCb0 I9IVLKI1E74OEY becomes length NxpUrFI8yGH8vTIcw7SvAuLTtjugSxoLNLmBqUIAlc25Uj7mPoeV0AyWjoUVA4BWZDssTZADRlprVATBn3eNWmrFpWmdETASmL8Hvxrgxvcfayv7OahDjYy64m8rBMHbt7lakCo
      The temperature PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc of the thermometer in terms of length NxpUrFI8yGH8vTIcw7SvAuLTtjugSxoLNLmBqUIAlc25Uj7mPoeV0AyWjoUVA4BWZDssTZADRlprVATBn3eNWmrFpWmdETASmL8Hvxrgxvcfayv7OahDjYy64m8rBMHbt7lakCo of mercury is given by:
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      When, BakoPWArPpHqlMr GnrcPLEudKHevQh4RNiugWHlG NwLhSuS SYCY77rZXRA6AbhVq4XwsTbJzf8UtJakBQfn2zo VMm6Xa5Do5NYRYEpLzr8nKmH7moZRIuqns3L0jz8jWcIM = length of mercury at ice point
      Image?w=46&h=28&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw length of mercury at steam point
      Image?w=51&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw Length of mercury at the unknown temperature MgLlAXaV9H NwfZX 70ib6hkFq5oCGOAwQilQ F1qIqZjAyXQ43eDhoZWarlL03OmmBKodJSCWls6Z0600LioMn B5CAb6rgrCOUcM P0d7Ot7W IyH5SqNo2a OLxg6ftqystg
      ADVANTAGES OF USING MERCURY IN THE LIQUID GLASS THERMOMETER
      The use of mercury has the following advantages.
      1. Its boiling point 357IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM and its freezing point is – 36IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM
      Therefore it can be used over a wide range of temperature.
      1. Its expansion is nearly uniform over the ordinary range of temperatures.
      This makes the calibration of the thermometer easier.
      1. It can be easily seen through glass because it is opaque and shining liquid.
      2. It does not wet glass 27oH97RPb0DU4JZLSeFRBaihyeb0aKgQ5nGOMGlRIPJBzaonMC8jPcMmc6K8aDaZnEG1G8ikaSZ 9G4U6nCfqI7CUGoNRbFjdOQ8HkxsyZinQw Ao8p6s4tHNwdEtai1Bmnr1YY no mercury remains on the sides of the glass tube when the mercury level falls.
      3. It has low specific heat capacity. Therefore it does not absorb much heat from the body whose temperature is to be measured.
      DISADVANTAGE OF USING MERCURY IN THE LIQUID IN GLASS THERMOMETERS
      It cannot be used to measure very low as well as very high temperatures.
      (ii) GAS THERMOMETERS
      In most accurate work, temperatures are measured by gas thermometers.
      There are two types of gas thermometers:
      1. Constant volume gas thermometer
      2. Constant pressure gas thermometer
      JOLLY’S CONSTANT VOLUME GAS / AIR THERMOMETER
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      B1 is a glass bulb containing dry air
      B2 is a glass tube containing mercury
      B1 is connected to B2 by means of a capillary tube E bent twice at right angles
      B3 is a glass tube containing mercury which is open the atmosphere at its upper end.
      There is a fixed mark ―O‖ on the glass tube B2
      The volume of air in B1 is maintained constant by raising or lowering the glass tube B3 until the mercury in B2 is at the fixed mark ―O‖.
      OPERATION
      When the thermometer is in use the bulb NQmfI6SiYBYTJh5lvrRexHJzVEw88eQrN1zdIMmKAub0vqAoKhtVzU3k1m4EpTvvLYiifzgTaCJNj5IbsjiYvr8mU JMqQvVSH5r JIm5npxsHKxl0c5kr9FUmTmyPuxlNrrBmo is placed inside the enclosure whose temperature is required.
      Keeping the volume of air in B1 constant by raising or lowering the glass tube B3, the pressure of air in B1 at ice point (0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM), steam point (100IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM) and at the unknown temperature Image?w=34&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw) are determined.
      If P denote pressure of a gas/air at constant volume, then one can talk of pressure at 0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM,
      100 and as P0, P100 and WfnaBrvXXlUH99YEL0dIcGGQRcWdAygWoPcl5h120CmGFQ8gPzoYLunwq3YI69skivT8IbnJMzStk2eSDkel3AxnrLcqxCRLSy Io3xZfRTLOYC1yKZTGAif6ijpUg6pmczPa0Y respectively Image?w=69&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Now, the unknown temperature PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc is given by:
      WbrfdGjiooAIIttoJ2fhjz6BDjZyEdNHDpOCeAqAPzDEnp0 603CCCshstGFx6iVSdLKW82pGsKSqNnmb3UiyZlUWLkcYbmeG KMMjT2KUzixc5lM6l8YfSLf3zlIErKn35Kx0c
      Gas thermometer is an ideal thermometer because the increase in volume or pressure of a gas with temperature is independent of the nature of the gas.
      27oH97RPb0DU4JZLSeFRBaihyeb0aKgQ5nGOMGlRIPJBzaonMC8jPcMmc6K8aDaZnEG1G8ikaSZ 9G4U6nCfqI7CUGoNRbFjdOQ8HkxsyZinQw Ao8p6s4tHNwdEtai1Bmnr1YY All gases have the same coefficient of volume or pressure expansion.
      ADVANTAGES OF USING GAS THERMOMETER
      The gas thermometer has the following advantages:
      1. It is more sensitive than liquid in glass thermometer because the expansion of gases is many times greater than that of any liquid.
      2. The expansion of the gas is uniform and regular.
      3. Gas scale temperatures degree with absolute scale of temperature.
      4. It can be used to measure very low as well as very high temperatures.
      Example
      Hydrogen gas thermometer can measure temperature from – 200IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM to 500IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM
      DISADVANTAGES OF USING GAS THERMOMETERS
      The gas thermometer has the following disadvantages: –
      1. Its use is inconvenient due to its very large size.
      2. The air in the capillary tube is not at the temperature being measured.
      3. It cannot be used to measure the temperature of a liquid available in small quantity.
      4. It is not a direct reading thermometer. ie require skill
      SOURCES OF ERRORS WHEN USING GAS THERMOMETERS
      1. The bulb expands
      2. Air is not an ideal gas
      (iii)The air in the capillary tube is not at the temperature being measured
      PLATINUM RESISTANCE THERMOMETER
      The Platinum resistance thermometer is based on the principle that the electrical resistance of a pure metal increases with increasing in temperature and vice versa.
      Experiments show that the resistance of a pure metal at any temperature PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc is given by:
      I5VgzaFTeWRA3dnAZpVUuhifvTG2B6DMNa8nq1 G5zkrgIqgzVgfmZ6biWT BlsRMIPrzWPEy04p7j31q2Yp5Bc Bw2HTA4hR5eGj1YdvQH5lfo9cj9N3VvHJERPDG2WOY2NqQo
      Where R0 = Resistance at 0 , = Resistance at a temperature MgLlAXaV9H NwfZX 70ib6hkFq5oCGOAwQilQ F1qIqZjAyXQ43eDhoZWarlL03OmmBKodJSCWls6Z0600LioMn B5CAb6rgrCOUcM P0d7Ot7W IyH5SqNo2a OLxg6ftqystg It can be shown that where ‘a’ and ‘b’ are physical constant Image?w=237&h=52&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      In practice”b” is much less than ―a‖ and hence we can ignore the term bPG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc2
      L4hgZkxTdmGEltT LNYnYzyIGtRMt6lMr75 XdYWtRgGM LoWvEAWb0MrFt HQh0vUP1kh3YzXWPjIm4TEa NWOXrr0EmA Z0 S1RLSinWXlGuBiOmRmokbsYmWU8ctQGT8UMuo = R0 (1 + aPG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc)
      Here ―a‖ is called temperature coefficient of resistance of the material of the wire (symbol,
      PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos)
      For platinum wire PubkfuTp1dQ 4AxoxUg Yxky3qtpDYf5hhj70DRyrSTJ7M TeCJEIYMqCxYswfQr8EmTDsoWyzST8L6PkfXeziCPNcjtj1R MueMKU OoFEcu8ct222MEtamrbvGBRs8mU0ATos = 3.8 x 10-4/IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM-1
       2SLI2ZEHVaSBp2BDpUZg2kz39WmEI8qEQ9qNXWeAg3ElQjvvdK1Rb44r5iT5xkalIVmHm1BLNgiCSd6ynATczJHhgRqGeJYmegf PNoYMtOqgLF WO8Me5neE842QrNMGNnaBY
      CONSTRUCTION
      A sample from a platinum resistance thermometer consist of a platinum wire that would be around the mica former.
      6PxYbr0BoGOJJkSpRPth3PIGwfDycSZFQi8VAtUVbDEcaRF3ne7pcPFhmh 6jZ6Vsb T2ajVSKxpNNwJSmqo7bTegdHZf TlPhWdsnsow3 EvvVoktmqSmWbBferDO56EIFTSeE
      The wire is enclosed in a protective tube of quartz, glass or porcelain tube depending upon the type of application and temperature range.
      The platinum wire is used because of its high temperature coefficient of resistance and high melting point (1773IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM)
      Therefore, considerable change in resistance occurs for a relatively small change in temperature.
      OPERATION
      The platinum resistance thermometer forms one of the four arms of the Wheatstone bridge.
      4Rbk1Iu7bJzczgoqQGDSyTgPIM0cQ6e3tdIT02dWQLXmCtSX8k1lNerlO7jkFt82 ZGi1SZCF3g3hSYIZe PgJeJoGVnzr3FUU8AtQA5 MhUdc1jPnyOSzEKjwluX74gIvQYMc8
      R1 and R2 are fixed resistors while R3 is a variable resistor.
      The bridge is often kept at a considerable distance from the testing point
      Under ordinary condition the bridge is balanced, that means the galvanometer shows no reading.
      When the temperature changes the resistance r of the resistance thermometer also change
      Consequently, the bridge no longer remains balance and some current flows through the galvanometer.
      The change in resistance (and hence current through G) is a measure of the magnitude of temperature.
      The accuracy of the platinum resistance thermometer depends on how accurately the bridge can be balanced.
      Let R0, R100 and L4hgZkxTdmGEltT LNYnYzyIGtRMt6lMr75 XdYWtRgGM LoWvEAWb0MrFt HQh0vUP1kh3YzXWPjIm4TEa NWOXrr0EmA Z0 S1RLSinWXlGuBiOmRmokbsYmWU8ctQGT8UMuo be resistance of platinum wire at ice point (0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM), steam point (100IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM) and at the unknown temperature MgLlAXaV9H NwfZX 70ib6hkFq5oCGOAwQilQ F1qIqZjAyXQ43eDhoZWarlL03OmmBKodJSCWls6Z0600LioMn B5CAb6rgrCOUcM P0d7Ot7W IyH5SqNo2a OLxg6ftqystg respectively
      The temperature PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc of the scale is given by:
      WTIQ1OFRJdrwzWj1fedc75GvWkAqO7BsfjqK7iPkYZkWsNQCaZUSM G1vsS7cJfEkznNNEZcDS1vhKc2HlFq2Otr5eAjNyinfSs0MvqcEMpVp9qjxGVrwn6h5VSQahOdpJ7GFq0
      ADVANTAGES OF USING PLATINUM RESISTANCE THERMOMETER
      1. High sensitivity (0.00005IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM)
      2. Small size
      3. Measurements can be made over a wide range (260IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM – 1200IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM)
      DISADVANTAGES OF USING PLATINUM RESISTANCE THERMOMETER
      1. High cost
      2. Requires additional equipments such as the bridge circuit, power supply etc.
      3. Larger size than thermocouple
      (iv)THERMOCOUPLE THERMOMETER
      A thermocouple is a device consisting of two dissimilar metal wires welded together at their ends.
      A thermoelectric ( GAOFE9TrZDim Ji9JbiNTNbOi XVA U22WwiApPoE7mNx7MQGVUTAImkpevMjfLSuXAqYdA8SNNpWV29RLryHu6DaIg9kyNmoRIke T KMWQ7sk65JXd6A136xBhQxSkDbK9az4 ) is generated in the device when the ends are kept at two different temperatures.
       JvY QYkho5VQyISxoVy0QjZzeKQ Xh8atdUrC DBUQsUBV I GauRGrUwXd GEM9btOqdUVpRpkRr MtNHr1ZrYefKJ7tN1wmWlZtb4QxB4euuPvsf9jbg0s6LKSBqSdAp0hko
      The magnitude of the 2y M74Q7JfpRy74HiBpUdUqLoUQ Ud4El1FipxYgYFnQsfErevhoQCI2EGZW960T6aBOKwiJJd167s8FfRqMMpiiswlD4zcK3oINhxx9hyUeNdO3fNG29BRYwTPdEJS8eNLFzos generated is related to the temperature difference between the two junctions.
      This enables a thermocouple to be used as a thermometer over a limited temperature range
      OPERATION
      One of the two junctions called the hot or measuring junction is placed at the temperature to be measured.
      The other junction( the cold or reference junction) is maintained at a known reference temperature (usually 0Image?w=24&h=52&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      The HD B49lpA 4CavkHi VIiicGPZ2DXG3lxbFLqY5he ZWc7KmZDGf FZEHNuTavv1bZq6juSGgqaLp Fx6kGIZN3ttWgLe0xGOqBTkJ NFE21V9zCLt64iYNEaExYfZiU1MEPEww generated is measured by a suitable millvoltmeter or a potentiometer incorporated in the circuit.
      The amount of the 2y M74Q7JfpRy74HiBpUdUqLoUQ Ud4El1FipxYgYFnQsfErevhoQCI2EGZW960T6aBOKwiJJd167s8FfRqMMpiiswlD4zcK3oINhxx9hyUeNdO3fNG29BRYwTPdEJS8eNLFzos generated depends upon the temperature difference between the hot and the cold junction
      The greater the HD B49lpA 4CavkHi VIiicGPZ2DXG3lxbFLqY5he ZWc7KmZDGf FZEHNuTavv1bZq6juSGgqaLp Fx6kGIZN3ttWgLe0xGOqBTkJ NFE21V9zCLt64iYNEaExYfZiU1MEPEwwthe greater is the temperature difference between the junctions.
      VARIATION OF THERMOELECTRIC VW1iotVQUMRn6JjUebvdaDvtAMGB 7gYlRGWMHZ6OQacuBV5HPRfuY4uOJZRHS5kXxlGktrj9KPJLn1C40TJLvbd1 7ZXzBUEazgjNXoXD6WTQf5YHijqlwhq2zwqWUQUiv BhQ WITH TEMPERATURE
      When the cold junction of a given thermocouple is kept constant at 0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM and the hot is varied. The e. m. f is found to relate with the temperature Image?w=324&h=154&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      difference junction by the equation
      Where A 0B1 CQ7QmFlqFdiUaOOaSSL5NzB IU9z XfqNqMQmjiZAGrAIOEnbykfzzDP803SgQOpGq7CoRcvp2uSuRclcuY8L 8RW9GPJxNfhFRCBF55Pkd8BdAU29P0QgrW8NyHtu865Zc B are constants.
      This is a parabolic equation and hence a graph of E against PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc is a parabola of the nature shown in the figure below.
      3eP VMvhNFEo R9OdmBy51fVCStguuImB Il0zghoXNZnQYOcsPYFBtKkjzZz1LP XOndSSSD HEIxFs6by7 I Esz81dPwDWajAvZSa AqECMjxv1sRlKYDQLWHoccKlDGFw
      Where Cto1FmjsZtobi5yjgl2kKq4OkPmwAbFa5FJdOX3pcoq 8bTT8H5c5JkJvd JBgnhTBwPeYGbDN3g6pINskifIsxXqYXBMLfxgACzDP XY2z8PqFxSu5Q2I04p7iizM2AjnQd3ZwTemperature of the cold junction
      Image?w=44&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcwNeutral temperature
      EtqT5hJ4aOiPoKWnBIu3XzwyNlpAZGF1tQhS8K4aYCa9SbZmOk8ytrn7FXaqCuw ZdmI8fQvQ9mOaS8eyfzHWYHo725o3mUzYSbjOQS 0aYwTFcgw7 KaOzWtta9l0teTyf15NsInversion temperature
      Neutral temperature ( Xd0J9mp5yZsj9iZ2pRBeKuHpQxzEXOjvJ7p9J H5K9fxkSrUiq8uAuxFACgBSAOt G2TIs9Jj0qnSBNS6Amp93MwStU98Ifl4rWqc3WxC9O7qfX3Ewa8I2UTegmJvmgS1wxrgN8)
      Is the temperature at which the 1LtwHkyTzE4GxjbB572NNE1 NrEmOHBgq3FmtAzwXPExvetSmIU0trz OP WvwT3XpQigbbPrnx KVExNYYMqBSBPEEpzsupnOrZow YEhwB9PwO5P475vLj0g2f ZaTKFAR3M0 of a thermocouple is maximum.
      When the temperature is increased beyond the thermoelectric e. m. f decreases untill it becomes zero when the temperature is called inversion temperature. Image?w=56&h=49&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Inversion Temperature
      Is the temperature to which the hot junction of a thermocouple must be raised in order that the thermoelectric e. m. f in the whole circuit becomes zero.
       LOi80h4osyFRLXqHK4fwqs8QtIzOiYx4Cf8EVGoa5cX8nG 8hWc4SNfWcDs32onEHH6SgHEvcgb D7a4sYpZHYkqsLHop2cHb2cNByYm2PvELMqvzJ9 39eqsBFszvMDJXm5xA THERMOCOUPLE
      From the graph above
      Image?w=108&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw =
      Image?w=120&h=26&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw + =
      2 = + Image?w=105&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Ef ADm0lDMyPqedX7s7s9zGcYD6bCwaWp40kvh3ID 7MBCvCY T5X7Hp0EIw99rZqypfHGafWWmbuOQI 7VXlgJHLBKFno2WeGZBaQ710dQkaQ88oWDu41Rhf2N3oOZhN1 UmbY
      From the relationship between E and PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc
      E BFt9eo1F P7Ss ZlrS0uCDuS D215HlS3pYravZZIWFzYtnxnI2NIDfbsQA UifPRhcH68pzKwxuUJPEfY5dO6SetyQlU6aWTh9aGp6FbRmB9tZ6iCMttRLJBeTVJjzLT1FN3IM
      Differentiating this equation with respect to PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc
      811at1fSo8Zs4mP34kga3S55PYaK8VK5xN79nh1M7FCBJuTrPEDm4uWahBgUv 26KxJ0g4XuUcYvS1l9V9AffaRrRtjw8UEk24tvGfmjZS06phEHOIT5rRXrxnqIYpXP ZbYgGw
      When Image?w=110&h=37&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw = 0 (slope of tangent at neutral temp)
      0 = A + 2BPG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtcn
      2BImage?w=59&h=28&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      HEyOFZ2jektHWKZTFpV30j1YFvGfByEQUumpT4ZFLFXSvwaOoRJrOnw1a2AtxQ413FmO1Vt047IhH4iimCOOVV8WZqE1OAQ1KlQBRtq9OdL6L8Za3a9v2SRQvEhDacRXSTP Vts
      EXPRESSION OF INVERSION TEMPERATURE
      From the relationship between E and PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc
      E = A – B 2 Image?w=49&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      When E = 0 then = Image?w=46&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      X5TdVOvDphfAQ0zR87VKzrkykBAxOvbYTa2x0Z4JOIYQC4C71pTxoNWJQj4B5ArtXSaGZZimNFi3bgHtSbA1HpSVhDQbHYPGaW4aHCvIPt0DxPJIyO0sSzOZ DxdR8T VGXChf0
      Tk1YETyfrs5yy4aFVU 962Uxa9u33dralaGtocwn5zmIqX7nPLYJble QDbbxCTxzhxhlzPG5qiTLuWjWZqlxAjZ5SNZz34WNKLB Hmb ET3Tkonccsv9vwzdqb7NZnVCn2Kv68
      RrocLFTbkGA3oJUKuXJvik1W55iquxPIWx7uIq6xVl5HLDII3sSjwsRVVTrmRJmlBkE044TAXIBNyx0Qm7Y1A1HwI9bgEC EGs GgvOTCNhVElCKbHnqbLDlYcmJWh3t2Cp IY4
      1. When the inversion temperature is exceeded the thermoelectric (e. m. f) in the thermocouple is reversed.
      2. The use of a thermocouple is restricted in the temperature range between 0 and neutral temperature AVNXDSp GssDDeZhM4q5zlE0z2c RdlAnkx3 7 Lho 4I4bdInJ GwAUrPXJZHdAnAIN5dst2ldcP D6NM W FP9 TJzSKI BD7yN0McClwquyJ1UrIdfP73QePTAJ84RD7hLqo It is because, beyond neutral temperature AVNXDSp GssDDeZhM4q5zlE0z2c RdlAnkx3 7 Lho 4I4bdInJ GwAUrPXJZHdAnAIN5dst2ldcP D6NM W FP9 TJzSKI BD7yN0McClwquyJ1UrIdfP73QePTAJ84RD7hLqo the thermoelectric e. m. f decreases with increasing temperature
      ADVANTAGES OF USING THERMOCOUPLES
      1. They have small heat capacities.
      Therefore they have very little effect on the temperature of the body they are measuring.
      1. They can measure rapidly fluctuating (changing) temperatures.
      1. They are more accurate.
      1. They are cheap and easy to use
      2. They have a wide range of temperature measurement (-200IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM to 1500IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM) depending upon the metals used.
      DISADVANTAGES OF USING THERMOCOUPLES
      1. Reference temperature has to be kept constant.
      2. As the output voltage is less than 10mV a very sensitive meter is required. (iii) The variation of e.m.f with temperature is non-linear
      (v) RADIATION THERMOMETERS (PYROMETERS)
      For measuring very high temperatures radiation thermometers (Pyrometers) are used.
      In these instruments high temperatures are measured by observing the radiation from the hot body.
       P1IypXvsHHeVzkbAqVjHJdJiwqnZQZmDeiUyZbCGsEn4CQmkKyBziWtS LsYqevrVnfrmioRWeZ3yWtZXp9yIEUfX4wsy7NXDZ4ulh6QYatNAfKHQqcha7Qr5t6xznDL19Nmu4
      The thermal radiation from the hot body is compared in terms of color with thermal radiation from the lamp filament.
      When a pyrometer is used a hot wire filament in the pyrometer is viewed against a glowing object.
      The filament current increased from zero until it makes the filament exactly the same color as the following object.
      A meter in series with the filament can then be calibrated directly in terms of source temperatures, known using the laws of radiation.
      They fall into two classes:
      1. Total radiation py
        rometer
      Which respond to the total radiation from the hot body
      1. Optical pyrometer
      Which respond only to the visible light
      Problem 01
      A thermometer uses mercury as liquid in glass experiments show that the length of mercury at 0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM and 100IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM are 5cm and 7cm respectively. At a certain temperature the length of the mercury is found to be 6.5cm, find this certain temperature. (Answer = 75 ) Image?w=57&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Problem 02
      The pressure recorded by a constant volume gas thermometer at a Kelvin temperature T is 4.80 x 104Nm-2.
      Calculate T if the pressure at triple point 273.16K is 4.20 x 104Nm-2. (Answer. T = 312K) Problem 03
      The resistance of a platinum wire at a temperatureMgLlAXaV9H NwfZX 70ib6hkFq5oCGOAwQilQ F1qIqZjAyXQ43eDhoZWarlL03OmmBKodJSCWls6Z0600LioMn B5CAb6rgrCOUcM P0d7Ot7W IyH5SqNo2a OLxg6ftqystg, measured on gas scale is given by L4hgZkxTdmGEltT LNYnYzyIGtRMt6lMr75 XdYWtRgGM LoWvEAWb0MrFt HQh0vUP1kh3YzXWPjIm4TEa NWOXrr0EmA Z0 S1RLSinWXlGuBiOmRmokbsYmWU8ctQGT8UMuo = R0 (1 + a + b 2) Image?w=45&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Where P7xlA6MWk7xtZxik WFT3OE8B1Jv5oxqbkojjZrcqfQj3Vd1r28vh1uCk45XHnjYWktG4t8 O5aF3hKpyy13IIwfTj6OY4kjl8 Nr6x5xIHlepWQLfJVWvH70z61zIud4LVXzE 3.8 x 10-3 and DzSSDayj5jTTC8mHVN7gj2cSFI1daPM67CCiDCmfFqyiTQqcemB71ew2GlBOenX9QEeUn8mXLtH7BepHrJkyOcJtZdw76iF2fDNtONAhXBYLC3ycFLOAOgij6JbBHOO I18r4JU5.6 x 10-7
      What temperature will the platinum thermometer indicate when the temperature on a gas scale is 200IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM
      Problem 04
      The pressure of air in a constant volume gas thermometer is 80cm and 109.3cm at 0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM and
      100IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM respectively. When the bulb is placed in hot water, the pressure is 100cm. calculate the temperature of hot water
      Problem 05
      The resistance of a platinum resistance thermometer is 100HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis at room temperature of 25IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM. In an experiment for measurement of temperature, the resistance of the thermometer is found to be 115.68HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis. find the value of temperature given that the temperature coefficient of resistance of platinum is 0.004/IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM.
      Problem 06
      A constant mass of a gas maintained at constant pressure has a volume of 200Dj6 MJ8Fy2dfhJwt ApZLMVu6 HT2GoD9639IcjeVVCrywoxt2dvLPZddKUeBdeIWM0NT2C0 9xF8qq2FWDkaf9aGUHBda8Z6BWX4EtB V0vMyVFdNNO3yWg3GRGBRKmrkmoiw at the temperature of melting ice, 273.2Dj6 MJ8Fy2dfhJwt ApZLMVu6 HT2GoD9639IcjeVVCrywoxt2dvLPZddKUeBdeIWM0NT2C0 9xF8qq2FWDkaf9aGUHBda8Z6BWX4EtB V0vMyVFdNNO3yWg3GRGBRKmrkmoiw at the temperature of water boiling under standard pressure and 525.1 at the normal boiling point of sulphur. A platinum wire has resistances of 2.00 , 2.778 , and 5.280HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis at these temperatures. Calculate the values of boiling- point of sulphur given by the two sets of observations and comment on the results. Image?w=71&h=49&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Problem 07
      In the thermocouple, the temperature of the cold junction is 10IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM while the neutral temperature is 270IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM. What is the value of temperature of inversion?.
      Problem 08
      In a certain thermocouple the thermo e. m. f E is given by
      E = Image?w=115&h=30&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw +
      Where PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc is the temperature of the hot junction and the cold junction being at 0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM.
      If = 10 V / and Image?w=120&h=33&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw = , find Image?w=96&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      1. The neutral temperature
      2. The temperature of inversion
      Problem 09
      1. What does one require in order to establish a scale of temperature?
      2. A Copper – constant thermocouple with its cold junction at 0IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM had an EMF of 4.28mV with its other junction at 100 . The EMF becomes 9.29mV when the temperature of the hot junction was 200 . If the EMF E is related to the temperature different PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc by the equation E = A + B 2, Calculate Image?w=100&h=75&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      1. The values of A and B
      2. The range of temperature of which E may be assumed proportional to PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc without incurring an error of more that 1%?
      Problem 10
      The resistance HgDYtQXMBNnRQa0e6qzK0 7m7l5hRJgb T2TH0Mpg0wfIbIf BbtVBivfAhFDSBaVTQNpMp7oSxVPdwq 9dOn9EDx7HpcrECdIq0zuHsHeQ5DddMbkXyoYOBBAVYqn6K9w3eNe0 of a platinum varies with temperature t according to the equation Oy0U01MYMuC8zVfAIq4Ir22 Ea1n27rVKxHAee5GVJ6WFDoIZve 2swYzgFlGNtqwBmjIfwldqFrp1k1cHWeJI4gUjQ78bs6C7 Dwz4s2obgPiQ5wcLGkOg ZW18WsYY3RUNh04R0 (1 + 8000bt – bt2) where “b” is a constant.
      Calculate the temperature on platinum scale corresponding to 400IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM on the gas scale
      Problem 11
      1. Define the thermodynamic temperature scale
      2. The resistance of a platinum resistance thermometer is 1.20HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis when measuring a Kelvin temperature T of a body and 1.00HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis at the triple point of water. Find T and its centigrade equivalent.
      Problem 12
      1. What do you understand by the terms
      1. Thermodynamic temperature scale
      2. Triple point of water
      1. The resistance of a platinum wire at temperature TIF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM measured on a gas scale is given by
      R (T) = R0 (LRiTIb48A3xObbjzuD8A 6ITUqrcGF7fCWTfcbXrWpfYn H HS62G7YYLYcQV0S1oFXquSK4BzjA2Lf8axjXcrwWt7sHo F5c6gVJ XHBiMovFMt4FhUgBOA AxDJq Ypuqf9wk)
      What temperature will the platinum thermometer indicate when the temperature on the gas scale is 200IF HWHAVFtm9k69B037oaVVz6duhn2maUBZp IAwS1REgb85J Wnjm4N UHu7HUwI2nelhb2A V6 4xu0 X6Q3XFyEKkkfPYShRhsZSShmpskOIXZJh FOy0nEMwH80gr4uMKVM?
      (Take P4ixJuhx3Vys67kfJnNdOev5wXpSUWm IYyba30gQKufK0ZGOv PT6wLK1t IHI22oHePIiZybyEKYPZNM Lufqa LBryi2GoK1VMhbGjkkcW04yewoAG V5bmFZHgjJyEE4jzU3.8 x 10-3 and P1 52z0lWY2JeqIO8HCjlfQ0IvJ0V4xO GWQrVpyBOdRDvh9wQb4uFAvWiCXjCrms 1Uk9xDf4206rzcN2PN74V GGFXkxXlNWfPTJXhd9GRk8TVYB JmxTLJ63n7hoDrmdhxP05.6 x 10-7)
      Problem 13
      1. Define
      1. Thermodynamic temperature scale
      2. How thermodynamic temperature donated and what is its SI unit?
      3. Explain why a gas thermometer is seldom used for temperature measurement in the laboratory?
      1. Study the table below and answer the questions which follow:
      NfrkWwjgIDVuk6CQwdIh0TGbKbAkvts0Xt20sHP1T2SCa2OjCXYovGJ77oWuO4 2zkaqKueM0t50pkFXSktx9OIS8iZaPEMHnpAmMUbK YWt4WlxXrsvvROfBaxz6zCL6KjShT0
      1. Calculate the temperature of the room for each thermometer
      2. Explain why thermometers disagree in their values of room temperature.
      3. What are the advantages of gas thermometer over liquid in-glass thermometers?
      Problem 14
      (a) (i) Describe how mercury in glass thermometer could be made sensitive.
      (ii) A sensitive thermometer can be used to investigate the difference in temperature between the top and bottom of the waterfall. Calculate the temperature difference of the water fall 50m high.
      (b) (i) Platinum resistance thermometer and constant volume gas thermometer are based on different thermometric properties but they are calibrated using the same fixed points. To what extent are the thermometers likely to agree when used to measure temperature near the ice point and near the steam point.
      (ii)The resistance of the element of a platinum resistance thermometer is 2.0HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis at ice point and 2.73HXtCYgA0QVLULnkiyuwHsMtfrs4bI6ysTHHwE1IixC JGOVNz 9Xzrvj9Ah2N5feOhRDRugOgy 8YlLmYJ5RwSxp91OIcsL8kyMdw9YGc1VFyVzc8OAZkRo3FpG7f43ksqt Sis at steam point. What temperature on the platinum resistance scale would correspond to resistance value of 8.34 and when measured on the gas scale the same temperature will correspond to a value of 1020 ? Explain the discrepancy. Image?w=53&h=49&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Problem 15
      (a). (i) What is meant by a thermometric property of a substance?
      (ii) What qualities make a particular property suitable for use in practical thermometers
      (b) Explain
      1. Why at least two (2) fixed points are required to define a temperature scale?
      2. Mention the type of thermometer which is most suitable for calibration of thermometers.
      This is the transfer of heat energy from one body or system to another as a result of difference in temperature. In general heat energy transfers from the region of higher temperature to the region of lower temperature.
      WAYS OF HEAT TRANSFER
      There are three ways by which heat can be transferred
      1. Conduction
      2. Convection
      3. Radiation
      THERMAL CONDUCTION This is the process in which heat flows from the hot end to the cold end of the solid body without there being any net movement of the particles of the solid.
      MECHANISM OF THERMAL CONDUCTION
      MECHANISM 1
      The molecules of a solid vibrate about their fixed positions with an energy that increases with temperature.
      When a part of the solid is heated, the molecules there start vibrating more violently.
      Since neighboring molecules are bound to each other, a molecule vibrating with larger energy will transfer some of its energy to its neighbors which in turn will transfer energy to the next neighbors and so on.
      MECHANISM 2
      In case of metals heat energy can also be transported by the free electrons.
      Since the electrons are very small, they can travel rapidly around throughout the specimen transferring energy by collision to other electrons and other molecules.
      Hence, the electrons are more effective in transferring energy from the hotter part to the colder part of the material than the mechanism explained above (mechanism 1)
      This explains why thermal conduction in metals is much more than that in insulators
      In metals heat energy is mainly carried by the free electrons although some energy is carried by intermolecular vibration.
      IMPORTANT TERMS
      1. RATE OF HEAT FLOW
      Symbol, Image?w=92&h=49&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      This is the heat flow per unit time in a material
      1. TEMPERATURE DIFFERENCE
      Symbol ( ) or d Image?w=95&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      This is the difference between higher and lower temperatures.
      Heat flows from the region of higher temperature to the region of lower temperature and if Image?w=53&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw > then,
      Temperature difference = Image?w=49&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      1. TEMPERATURE GRADIENT
      Symbol Image?w=107&h=33&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw or
      This is the temperature difference per unit length of the material.
      It is a fall of temperature with distance between the ends of the body in the direction of heat flow.
      68MbNUjo0ZHdrKYCNRFmfQPIJpNDLmnqc8sGF9gVZDY3rkB9B3FhAIBK XYu 5wKdptuvvBudsqTELNU9yY6VzOyINI92mwrfdtw7 XMjceSf GDoTjxNP8KOHI7ynRXEz4Xi8
      Temperature gradient = Image?w=94&h=33&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw =
      1. STEADY CONDITION
      This is an equilibrium point in a material when at every point the temperatures are constant.
      1. LAGGED MATERIAL
      A material enclosed by an insulator (bad conductor of heat) so that the heat loss to the surrounding is negligible.
      1. UNLAGGED MATERIAL
      A material which is not enclosed by an insulator so that the heat is lost to the surrounding.
      TEMPERATURE DISTRIBUTION ALONG THE CONDUCTOR
      1. UNLAGGED CONDUCTOR
      Consider an unlagged metal bar AB whose ends have been soldered into the metal tanks H and C
      8Rv GeSw9e0MJmq2qUvNK9HaWFGt RtYaCYCm7rJIRTLVzlIl8ETo0FvjNMH5d1S1hDWVVOt8hRyO86RGnqqoLmDguXFYHSa KRWp2whwBdaNXRw5uhBuVJt5LqcviVYdvY7ZBg
      H contains boiling water and C contains ice water.
      Heat flows from the hot end to the cold end of the bar and when the conditions are steady the temperature PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc are measured at points along the length of the bar.
      This happens simply because some amount of heat is lost to the surrounding by convection and radiation.
      2. LAGGED CONDUCTOR
      If the metal bar is well-lagged with a bad conductor of heat such as asbestos and wool the temperature now falls uniformly from the hot end to the cold end of the bar.
      A graph of temperature against length of the bar is shown below:
      GkaoDuXrgTLuPgasEvLcMUqBYjraucnBBDJlKBSrLDs61mckjic1t Ge28Me8 Egoyv0KlNDEyH1txFkWkHhU81cN0dr TRZG0csAmWgMns9jMyah8erGpt UGa4fJIOXsMDjkE
      Since the metal bar is well-lagged no heat is lost to the surrounding and a graph of fall of temperature against length of the bar is a straight line (see figure above)
      THERMAL CONDUCTIVITY
      It is measure of the ability of a material to conduct heat.
      Consider a conductor of length L of cross – sectional area A
      Let and be temperature on the opposite sides of the conductor with Image?w=57&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw > Image?w=67&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Experiments show that the heat flow per second KC8yZO Dc5UsMBNrCJacV Y5o1sRgCfy WRnVvdcd5VJu1NZ189So2Gaj M7B79AnHpieBp FVCFtcy0Oomd JMiiai2radXzHHQU19sttSKMHL6riwi0 32RThPTxYLrbGEatQ from the hot sides to the cold side of the conductor is:
      1. Directly proportional to the cross-sectional area A of the conductor
      Image?w=93&h=49&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw A
      1. Directly proportional to the temperature difference Image?w=60&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw – ) between the two sides
      Image?w=120&h=49&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw )
      1. Inversely proportional to the perpendicular distance between the concerned faces
      Image?w=73&h=45&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Combining the above three factors:
      LiiW1Bn Uo4P Ffe6C1qFLHNf9luQHIwM277eKigjk7m4pGAtyVtu0Hp02uocJ0iwvIKSX9FR1fGgAsvsIUYvZ8TyGwt41L67R3oeMnh51eIdcjSihCMWjj23ZbAlcp XJvD22E
      Where K = constant of proportionality called coefficient of thermal conductivity (thermal conductivity) of the material.
      Equation (1) above assumes that:
      1. The opposite sides are parallel
      2. There is no heat loss through the sides.
      From equation (1)
      E9qOsoJfDsaJodSEuu8m7gnqEe2AbjNDmcGZFr23b VBJmkH3T95Tq5M TzFvclBc5F7Jy88AC1pkBwfTD05jIfBOJrufc3x XOTpLfrkr8Eb J4iPoMTsliDvFRaGF4LdtrEmA
      Definition
      The coefficient of thermal conductivity K of a material is the rate of flow of heat per unit area per unit temperature gradient when the heat flow is perpendicular to the faces of a thin parallel – sided slab of the material under steady state conditions.
      UNIT OF K
      From equation (2)
      K = CxLT9gqbuKr5JwEGuGq8IRo9ytk47cMLmFdYAmVlKcQY4grjv7AfBuguHv2bvRIqhohkPX4 Tkacrrz0 P30yR17bsHBK1zfcyt3dUvV5 YADx 0 9EvoyKNT2rrFqgET7GTS M
      = EywlJSGiwU JYZrZ0Tv62W17KiSPq0W DPZQHVsvY2wMloS EZfWPIkeW5eoLlu7TI8GldFQ25eMtS4UWn8Jh0SYguALbYeZlj4DIQ9 TrjK1HOCOKVQwgAxZ4JCrScP5r8e7Cs
      = M VH7lwzWUKz2XDM1UX3NpGDUBqsK0p0cUclUTEraOJndW5JlfzbnFSLNme0tClBuTBJr3MnKZ1uRiAoauhQTHwJF2hjsy0B4s GF3gciDgem1DHZaVOvX3nUgC55sKO8LuGHs8
      Hence, the SI unit used Wm -1K-1 Equation (1) can be written as:
      Ny Ev7UjIThu7jrhnXcGgCPzKhqRcF19TSFwtgOtN5hPwGs2I2FFxssC Qff3JxGB5oEhFhr4Qm1MEEPa8CaorpZwEfrlptZ0jFZeleGUnVeCJPB3zg2w7LGR 0UyRBR 5d0MAI ……………………..(3)
      Where V7rSDR8TtLB1R5Z5SeI6v8LXYxsjOzWUXIIhY26axfiB 2l5h2XxfrJlneBmpHRCLfTcBt1K2HUdi0sir6arun98FPjMdgYeM7hdLdpkSBB6PIXYRvEawK3o9XTcJULniDU9K8I = Temperature gradient
      The D4daXBEIpwiY4toVeSagWLUK5ZTGILhvEhmkTqYmXYB KKnfHX77gH NJ8lS56iYGhgrKLc IG Zyyy31neLr YknaTX1v6OTExVRvunT 2tOjJu 9BMkt7Oe61B1cq51WcbSLc sign show that the heat flows in the direction of decreasing temperature i.e the temperature PG9wtd9yWy9WoXRlit66Irru GF EpncSkzdRo3Y HHYZ6iz7rkjXZ744GDcvaGQM5Lo2nm79Oxi9nnPMyrwZ4aimdkNqAhpBXtf80cszY2ZVRK8Py ZO80JRu 248al7jGnDtc diminishes as the length NxpUrFI8yGH8vTIcw7SvAuLTtjugSxoLNLmBqUIAlc25Uj7mPoeV0AyWjoUVA4BWZDssTZADRlprVATBn3eNWmrFpWmdETASmL8Hvxrgxvcfayv7OahDjYy64m8rBMHbt7lakCo increases. The value of K for some common substances at room temperature are as shown in the table below:
      Substance
      K in Wm -1K-1
      Silver
      418
      Copper
      385
      Aluminum
      238
      Iron
      80
      Lead
      38
      Mercury
      8
      Glass (Pyrex)
      1.1
      Brick
      -1
      Rubber
      0.2
      Air
      0.03
      Substance for which SMyq7EDwmZ6r4PBlbqvtuYV G19rF6Y5Uprz5ukHkLJpEJKIasA1AVQ8Sj1HXtdIeImlNU7JS9tzDUwvzvxPANjTze CZa LHZ8tYCw S2JwU3CTifdXJG8Aar8F7tVxxyuBUpE is small is bad conductors of heat.
      Substance for which k is large conducts heat rapidly and are said to be good conductors of heat.
      COMPOSITE BARS
      A composite bars is that bar consisting of two or more metal bars of different materials joined end to end.
      Consider a composite bar made of different materials of coefficient of thermal conductivities K1 and K2 respectively
      70L8OPAJDJ 36xVlprq1ZG1fD8ixULyIjBfOfnOzbmk8 MB7fkJS7HlbMfwzwMVL3aW Pb5nqWADrfoY2AsFJcdHVCg2LcdTHEh0TwrM6Do P7Np72BbLaRWCyVJOx7cRDvTLxg
      Let A be cross sectional area of the bar
      Assuming the bar is well – lagged so that no heat leaves from it.
      Condition
      At steady state condition, the heat flowing into one end of the bar is equal to that flowing out of the other end.
      27oH97RPb0DU4JZLSeFRBaihyeb0aKgQ5nGOMGlRIPJBzaonMC8jPcMmc6K8aDaZnEG1G8ikaSZ 9G4U6nCfqI7CUGoNRbFjdOQ8HkxsyZinQw Ao8p6s4tHNwdEtai1Bmnr1YYThe rate at which heat flows is one material is equal to that in the other material.
      DphXU4pAtpIcZB4NNU 5w8EC9ksfxVgIDuSdSF6b1iTOXnYtv0fskan2yOSxM5R9p1vZ7Lo0n5brDHB8mkJW6PqO2U0S43Q0YomeYliXRMi3bjBl9mChqFwceJTdNlSMhdK FCg = K1A F YdqSxqtjEZx42VXENMCgUWOiGMnlO3ykFMjbe5YCRBqgyyzhJgAIs1 SOgZ3P1qnPM GCPxw 9XH5X1p8I1sOYAnc5Jm Mooa3FMyIFor1q9 U5tazZH4YJ 7JzfFNw4FopOs = K2A  AMEhCJnKgHHcaIyatw4e6nLfScpofQ3rZ KOTODiqjeIyh77ToR27xs5MTBZ2vghByuP GZ7PQRgIVGyyIoFSN KrISf8fOAOtvOm9tpYckVhlUUvoh07eWfOSJdj0NzThmHMI
      Where , and are the temperatures at the ends of the bars respectively. Image?w=86&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      THERMAL RESISTANCE (R)
      From the heat conduction equation:
      DphXU4pAtpIcZB4NNU 5w8EC9ksfxVgIDuSdSF6b1iTOXnYtv0fskan2yOSxM5R9p1vZ7Lo0n5brDHB8mkJW6PqO2U0S43Q0YomeYliXRMi3bjBl9mChqFwceJTdNlSMhdK FCg = KA Hz0ElLZ6BI5fo2DfWLxUHEZwSEcRmrX1pr74fmyWgJMO4x4jOk3fHcvQpDEUmcAwrbccbb8ISYiQ287wSPiycBk Xniz MVctztXPhOlmuBg 5r7G2B7jCLpd5 VXXg7ybyr5MM
      This equation can be linked to Ohm‘s law for electricity
      I = KJq7tPRs3srImWIIoKSSMh9wnpDa TqyH2OSyj9KBU Itvr25XWTu D1Kzk RhGK3spcQI EtD G4tGmwfplm7RwzPabKtNLo5B9nO Oo5wMnflEig E O05 5BwiqkiEIQcJyM
      Ler4PRJLICs8sYEKGBgLiPYdWlad8HNpmBpxpceIlKPp5sITIKILhDNePKSRcF1PEZ6nlC8KVhdDYNm3lSTKGknH8jiCPJLbcIlIqXmwDsI609B FXSWz1g5DH9B0DMDruoNORQ
      From equation (1) and equation (2) above both DphXU4pAtpIcZB4NNU 5w8EC9ksfxVgIDuSdSF6b1iTOXnYtv0fskan2yOSxM5R9p1vZ7Lo0n5brDHB8mkJW6PqO2U0S43Q0YomeYliXRMi3bjBl9mChqFwceJTdNlSMhdK FCg and I are flow quantities.
      In equation (1) the heat flows per second DphXU4pAtpIcZB4NNU 5w8EC9ksfxVgIDuSdSF6b1iTOXnYtv0fskan2yOSxM5R9p1vZ7Lo0n5brDHB8mkJW6PqO2U0S43Q0YomeYliXRMi3bjBl9mChqFwceJTdNlSMhdK FCg produced by a temperature differenceL12KlX15geuzFf32tf K UnIAJqTt0Q FMS1BsvHsMmB1OkH KQ JILt0n2dfpNUnWi97DWYh EdZI2GrukReJyZIZsum3DBC QctGChV6m1LhnTlLoHr1mbMnTFwt9OjafLWKo.
      In equation (2) the flow of current I ( = charge flow per sec) is produces by potential difference V
      Thus, the quantity I4domnsUbbhpSh NJaT1kwULajHc12G5D0A6S3tkwnqG1b Lmy54 Pt7MTKUznNFSxJWqoWDut8zESPf7ItjPxzOGk45SurKfqHL ZYvlTSavywNDi8gULuA PPJD7UB3ssaZOU is thermal Equivalent of DgQDBb4BkZDM2DZqyBGWD6VGoo4CUAENS1JGuj4jQxwoeFs6aNlp1zz3ih8 IT3M7iWtEu9lxfnPrUaKCC C4bj979YhDtLmUtTkkXcssSxUqHwZhEz 7AtmmrCtdKTKH7 Hy1Y
      Image?w=65&h=33&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw =
      WBwAAt2bwQ7cbZrM7SyImR BEobM4kRdoehuWVP376bRGo OqDiyPSSV0ZdDsZidzfhue3MIX4fu4j9H Y4Yp6Bnni24rzuiLDhwH79jk8TP3bvV9qLeQHy8MG DFzB6K6jWfpk
      Where NxpUrFI8yGH8vTIcw7SvAuLTtjugSxoLNLmBqUIAlc25Uj7mPoeV0AyWjoUVA4BWZDssTZADRlprVATBn3eNWmrFpWmdETASmL8Hvxrgxvcfayv7OahDjYy64m8rBMHbt7lakCo = conductor length
      K = Thermal conductivity
      A = across- sectional area of the conductor.
      Alternative expression of R From the heat conduction equation:
      Image?w=101&h=37&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
      Image?w=126&h=37&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw =
      But Image?w=51&h=33&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw =
      NjtJFg0YKrxknsFz9f Ws3XPQ9YywHJ6Dp0zzpguMCyR6EqglvhX6SwpKxT5qUrvhAKJ T5lXati9cYp9oxJ6ggfZqWVjUwUgNXWJ8KKn0jyBOq8GIJXsQUAf 1kEp48FgukqHM




      ');}
      Bc0138c3d2dab0944d91d638547c2715

      subscriber

      1 Comment

      • 259b4d61b3de335bed80e6d077388ae3

        Muhwezi Patrick, May 22, 2026 @ 5:20 amReply

        I appreciate

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