Download Physcis Notes Of Thermal Properties Of Matter For Class 11 In PDF

Chapter 11 : Thermal Properties of Matter

The branch dealing with measurement of temperature is called thremometry and the devices used to measure temperature are called thermometers.

Heat is a form of energy called thermal energy which flows from a higher temperature body to a lower temperature body when they are placed in contact.

Heat or thermal energy of a body is the sum of kinetic energies of all its constituent particles, on account of translational, vibrational and rotational motion.

The SI unit of heat energy is joule (J).

The practical unit of heat energy is calorie.

1 cal = 4.18 J

1 calorie is the quantity of heat required to raise the temperature of 1 g of water by 1Â°C.

Mechanical energy or work (W) can be converted into heat (Q) by 1 W = JQ

where J = Jouleâ€™s mechanical equivalent of heat.

J is a conversion factor (not a physical quantity) and its value is 4.186 J/cal.

Temperature of a body is the degree of hotness or coldness of the body. A device which is used to measure the temperature, is called a thermometer.

Highest possible temperature achieved in laboratory is about 108 while lowest possible temperature attained is 10-8 K.

Branch of Physics dealing with production and measurement temperature close to 0 K is known as cryagenics, while that deaf with the measurement of very high temperature is called pyromet

Temperature of the core of the sun is 107 K while that of its surface 6000 K.

NTP or STP implies 273.15 K (0Â°C = 32Â°F).

1. Celsius Scale In this scale of temperature, the melting point ice is taken as 0Â°C and the

boiling point of water as 100Â°C and space between these two points is divided into 100

equal parts

2. Fahrenheit Scale In this scale of temperature, the melt point of ice is taken as 32Â°F and

the boiling point of water as 211 and the space between these two points is divided into

180 equal parts.

3. Kelvin Scale In this scale of temperature, the melting pouxl ice is taken as 273 K and

the boiling point of water as 373 K the space between these two points is divided into

100 equal pss

The property of an object which changes with temperature, is call thermometric property.

Different thermometric properties thermometers have been given below

where p, p_{100}. and pt, are pressure of a gas at constant volume 0Â°C, 100Â°C and tÂ°C.

A constant volume gas thermometer can measure tempera from â€“ 200Â°C to 500Â°C.

R_{t} = R_{0}(1 + Î±t + Î²t2)

where Î± and Î² are constants for a metal.

As Î² is too small therefore we can take

R_{t} = R_{0}(1 + Î±t)

where, Î± = temperature coefficient of resistance and
R_{0} and R_{t}, are electrical resistances at 0Â°C and tÂ°C.

where R_{1} and R_{2} are electrical resistances at temperatures t_{1 }and t_{2}.

where R_{100} is the resistance at 100Â°C.

Platinum resistance thermometer can measure temperature from â€”200Â°C to 1200Â°C.

(iii) Length of Mercury Column in a Capillary Tube

l_{t}= l_{0}(1 + Î±t)

where Î± = coefficient of linear expansion and l0, lt are lengths of mercury column at 0Â°C and tÂ°C.

Thermo Electro Motive Force

When two junctions of a thermocouple are kept at different temperatures, then a thermo-emf is produced between the junctions, which changes with temperature difference between the junctions.

E = at + bt^{2}

where a and b are constants for the pair of metals.

Unknown temperature of hot junction when cold junction is at 0Â°C.

Where E_{100} is the thermo-emf when hot junction is at 100Â°C.

A thermo-couple thermometer can measure temperature from â€”200Â°C to 1600Â°C.

When there is no transfer of heat between two bodies in contact, the the bodies are called in thermal equilibrium.

If two bodies A and B are separately in thermal equilibrium with thirtli body C, then bodies A and B will be in thermal equilibrium with each other.

The values of pressure and temperature at which water coexists inequilibrium in all three states of matter, i.e., ice, water and vapour called triple point of water.

Triple point of water is 273 K temperature and 0.46 cm of mere pressure.

The amount of heat required to raise the temperature of unit mass the substance through 1Â°C is called its specific heat.

It is denoted by c or s.

Its SI unit is joule/kilogram-Â°C'(J/kg-Â°C). Its dimensions is [L^{2}T^{-2}Î¸^{-1}].

The specific heat of water is 4200 J kg^{-1}Â°C^{-1} or 1 cal g^{-1} C^{-1}, which high compared with most other substances.

Gases have two types of specific heat

1. The specific heat capacity at constant volume (C_{v}
).

2. The specific heat capacity at constant pressure (C_{r}).

Specific heat at constant pressure (C_{p}) is greater than specific heat constant volume (C_{V}), i.e., C_{p} > C_{V} .

For molar specific heats C_{p} â€“ C_{V} = R

where R = gas constant and this relation is called Mayerâ€™s formula.

The ratio of two principal sepecific heats of a gas is represented by Î³.

The value of y depends on atomicity of the gas.

Amount of heat energy required to change the temperature of any substance is given by

Q = mcÎ”t

â€¢ where, m = mass of the substance,

â€¢ c = specific heat of the substance and

â€¢ Î”t = change in temperature.

Heat capacity of any body is equal to the amount of heat energy required to increase its temperature through 1Â°C.

Heat capacity = me

where c = specific heat of the substance of the body and m = mass of the body.

Its SI unit is joule/kelvin (J/K).

It is the quantity of water whose thermal capacity is same as the heat capacity of the body. It is denoted by W.

W = ms = heat capacity of the body.

The heat energy absorbed or released at constant temperature per unit mass for change of state is called latent heat.

Heat energy absorbed or released during change of state is given by Q = mL

where m = mass of the substance and L = latent heat.

Its unit is cal/g or J/kg and its dimension is [L^{2}T^{-2}
].

For water at its normal boiling point or condensation temperature (100Â°C), the latent heat of vaporisation is

L = 540 cal/g

= 40.8 kJ/ mol

= 2260 kJ/kg

For water at its normal freezing temperature or melting point (0Â°C), the latent heat of fusion is

L = 80 cal/ g = 60 kJ/mol

= 336 kJ/kg

It is more painful to get burnt by steam rather than by boiling was 100Â°C gets converted to water at 100Â°C, then it gives out 536 heat. So, it is clear that steam at 100Â°C has more heat than wat 100Â°C (i.e., boiling of water).

After snow falls, the temperature of the atmosphere becomes very This is because the snow absorbs the heat from the atmosphere to down. So, in the mountains, when snow falls, one does not feel too but when ice melts, he feels too cold.

There is more shivering effect of ice cream on teeth as compare that of water (obtained from ice). This is because when ice cream down, it absorbs large amount of heat from teeth.

Conversion of solid into liquid state at constant temperature is melting.

Conversion of liquid into vapour at all temperatures (even below boiling point) is called cevaporation. Boiling

When a liquid is heated gradually, at a particular temperature saturated vapour pressure of the liquid becomes equal to atmospheric pressure, now bubbles of vapour rise to the surface d liquid.

This process is called boiling of the liquid.

The temperature at which a liquid boils, is called boiling point The boiling point of water increases with increase in pre sure decreases with decrease in pressure.

The conversion of a solid into vapour state is called sublimation.

The conversion of vapours into solid state is called hoar fr..

This is the branch of heat transfer that deals with the measorette heat. The heat is usually measured in calories or kilo calories.

When a hot body is mixed with a cold body, then heat lost by ha is equal to the heat gained by cold body

Heat lost = Heat gain

Increase in size on heating is called thermal expansion. There are three types of thermal expansion.

1. Expansion of solids

2. Expansion of liquids

3. Expansion of gases

Three types of expansion -takes place in solid.

Linear Expansion Expansion in length on heating is called linear expansion.

l_{2} = l_{1}(1 + Î± Î”t)

where, l_{l} and l_{2} are initial and final lengths,Î”t = change in temperature and Î± = coefficient of linear expansion.

Î± = (Î”l/l * Î”t)

where 1= real length and Î”l = change in length and Î”t= change in temperature.

Superficial Expansion Expansion in area on heating is called superficial expansion.

Increase in area A_{2} = A_{1}(1 + Î² Î”t)

where, A_{1} and A_{2} are initial and final areas and Î² is a coefficient of superficial expansion.

Î² = (Î”A/A * Î”t)

where. A = area, AA = change in area and At = change in temperature.

Cubical Expansion Expansion in volume on heating is called cubical expansion.

Increase in volume V_{2} = V_{1}(1 + Î³Î”t)

where V_{1}
and V_{2}
are initial and final volumes and Î³ is a coefficient of cubical expansion.

where V = real volume, AV =change in volume and Î”t = change in temperature.

Relation between coefficients of linear, superficial and cubical expansions

Î² = 2Î± and Î³ = 3Î±

Or Î±:Î²:Î³ = 1:2:3

In liquids only expansion in volume takes place on heating.

(i) Apparent Expansion of Liquids When expansion of th container containing liquid, on heating is not taken into accoun then observed expansion is called apparent expansion of liquids.

Coefficient of apparent expansion of a liquid

(ii) Real Expansion of Liquids When expansion of the container, containing liquid, on heating is also taken into account, then observed expansion is called real expansion of liquids.

Coefficient of real expansion of a liquid

Both, yr, and ya are measured in Â°C^{-1}.

We can show that y_{r} = y_{a}+ y_{g}

where, y_{r}, and y_{a} are coefficient of real and apparent expansion of liquids and y_{g} is coefficient of cubical expansion of the container.

Anamalous Expansion of Water

When temperature of water is increased from 0Â°C, then its vol decreases upto 4Â°C, becomes minimum at 4Â°C and then increases. behaviour of water around 4Â°C is called, anamalous expansion water.

3. Expansion of Gases

There are two types of coefficient of expansion in gases

(i) Volume Coefficient (γv) At constant pressure, the change in volume per unit volume per degree celsius is called volume coefficient.

where V_{0}, V_{1}, and V_{2}
are volumes of the gas at 0Â°C, t_{1}Â°C and t_{2}Â°C.

(ii) Pressure Coefficient (Î³_{p}) At constant volume, the change in pressure per unit pressure pe degree celsius is called pressure coefficient.

where p_{0}, p_{1} and p_{2} are pressure of the gas at 0Â°C, t_{1}Â° C and t_{2}Â° C.

1. When rails are laid down on the ground, space is left between the end of two rails.

2. The transmission cables are not tightly fixed to the poles.

3. The iron rim to be put on a cart wheel is always of slightly smaller diameter than that of
wheel.

4. A glass stopper jammed in the neck of a glass bottle can be taken out by warming the
neck of the bottles.

â€¢ Due to increment in its time period a pendulum clock becomes slow in summer and will
lose time.

â€¢ Loss of time in a time period Î”T =(1/2)Î± Î”Î¸T

âˆ´ Loss of time in any given time interval t can be given by

Î”T =(1/2)Î± Î”Î¸t

â€¢ At some higher temperature a scale will expand and scale reading will be lesser than true values, so that true value = scale reading (1 + Î± Î”t)

Here, Î”t is the temperature difference.

â€¢ However, at lower temperature scale reading will be more or true value will be less.

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- Chapter 2 Units and Measurements
- Chapter 3 Motion in a straight
- Chapter 4 Motion in a Plane
- Chapter 5 Laws of Motion
- Chapter 6 Work Energy and Power
- Chapter 7 : System Of Particles And Rotational Motion
- Chapter 8 : Gravitation
- Chapter 9 : Mechanical Properties of Solids
- Chapter 10 : Mechanical Properties Of Fluids
- Chapter 11 : Thermal Properties of Matter
- Chapter 12 : Thermodynamics
- Chapter 13 : Kinetic Theory

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