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1. Xtra Edge February 2012 - Career Point

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PHYSICS FUNDAMENTAL FOR IIT-JEE<br />

Thermal Expansion, Thermodynamics<br />

Thermal Expansion :<br />

.(a) When the temperature of a substance is increased,<br />

it expands. The heat energy which is supplied to<br />

the substance is gained by the constituent<br />

particles of the substance as its kinetic energy.<br />

Because of this the collisions between the<br />

constituents particles are accompanied with<br />

greater force which increase the distance between<br />

the constituent particles.<br />

∆l = lα∆T ; ∆A = Aβ∆T ; ∆V = Vγ∆T<br />

or l' = l (1 + α∆T) ; A' = A(1 + β∆T) ;<br />

V' = V(1 + γ∆T)<br />

(b) Also ρ = ρ'(1 + γ∆T) where ρ' is the density at<br />

higher temperature clearly ρ' < ρ for substances<br />

which have positive value of γ<br />

* β = 2α and γ = 3α<br />

Water has negative value of γ for certain temperature<br />

range (0º to 4ºC). This means that for that<br />

temperature range the volume decreases with<br />

increase in temperature. In other words the density<br />

increases with increase in temperature.<br />

30 ml<br />

25 ml<br />

20 ml<br />

15 ml<br />

10 ml<br />

5 ml<br />

0 ml<br />

If a liquid is kept in a container and the temperature<br />

of the system is increased then the volume of the<br />

liquid as well as the container increases. The<br />

apparent change in volume of the liquid as shown by<br />

the scale is<br />

∆Vapp = V(γ – 3α) ∆T<br />

Where V is the volume of liquid at lower temperature<br />

∆Vapp is the apparent change in volume<br />

γ is the coefficient of cubical expansion of liquid<br />

α is the coefficients of linear expansion of the<br />

container.<br />

Loss or gain in time by a pendulum clock with<br />

1<br />

change in temperature is ∆t = α(∆T) × t<br />

2<br />

KEY CONCEPTS & PROBLEM SOLVING STRATEGY<br />

Where ∆t is the loss or gain in time in a time interval t<br />

∆T is change in temperature and d is coefficient of<br />

linear expansion.<br />

If a rod is heated or cooled but not allowed to expand<br />

or contract then the thermal stresses developed<br />

F<br />

= γα∆T.<br />

A<br />

If a scale is calibrated at a temperature T1 but used at<br />

a temperature T2, then the observed reading will be<br />

wrong. In this case the actual reading is given by<br />

R = R0(1 + α∆T)<br />

Where R0 is the observed reading, R is the actual<br />

reading.<br />

For difference between two rods to the same at all<br />

temperatures l 1α1 = l2α2.<br />

Thermodynamics<br />

According to first law of thermodynamics<br />

q = ∆U + W<br />

For an isothermal process (for a gaseous system)<br />

(a) The pressure volume relationship is ρV = constt.<br />

(b) ∆U = 0<br />

(c) q = W<br />

(d) W = 2.303 nRT log10<br />

V f<br />

p<br />

= 2.303 nRT i log10<br />

Vi<br />

pf<br />

(e) Graphs T2 > T1<br />

<strong>Xtra</strong><strong>Edge</strong> for IIT-JEE 25 FEBRUARY <strong>2012</strong><br />

P<br />

T2<br />

T1<br />

P<br />

V<br />

T<br />

T<br />

These lines are called isotherms (parameters at<br />

constant temperature)<br />

For an adiabatic process (for a gaseous system)<br />

(a) The pressure-volume relationship is PV γ = constt.<br />

(b) The pressure-volume-temperature relationship is<br />

PV<br />

= constt.<br />

T<br />

(c) From (a) and (b) TV γ–I = constt.<br />

(d) q = 0<br />

(e) W = –∆U<br />

V

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