1. Xtra Edge February 2012 - Career Point
1. Xtra Edge February 2012 - Career Point
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