First Law of Thermodynamics Physics 202 Professor Lee Carkner Lecture 13.
Entropy Physics 202 Professor Lee Carkner Lecture 15.
-
date post
18-Dec-2015 -
Category
Documents
-
view
215 -
download
0
Transcript of Entropy Physics 202 Professor Lee Carkner Lecture 15.
PAL #14 Internal Energy 3 moles of gas, temperature raised from 300 to
400 K He gas, isochorically
Q = nCVT, CV = (f/2)R = (3/2) R Q = (3)(3/2)R(100) = 3740 J
He gas, isobarically Q = nCPT, CP = CV + R = (5/2) R Q = (3)(5/2)R(100) = 6333 J
H2 gas, isochorically Q = nCVT, CV = (5/2) R, f = 5 for diatomic Q = (3)(5/2)R(100) = 6333 J
H2 gas, isobarically Q = nCPT, CP = CV + R = (7/2) R Q = (3)(7/2)R(100) = 8725 J
PAL #14 Internal Energy 4 moles of N2 gas isobaric expansion from 0.45
m3 to 0.78 m3 and 457 K pressure = p =nRT/V = (4)(8.31)(457)/(0.78)
= 19475 Pa initial temp = T = pV/nR = (19475)(0.45)/(4)
(8.31) = 263.7 K W=pV = (19475)(0.78-0.45) = 6427 J Q=nCp T = (4)(7/2)(8.31)(457-263.7)
=22489 J adiabatic process starts at the same point,
ends where V= 0.78 m3. piVi
pfVf
pf = piVi
Vf(19475)(0.45)1.4/(0.78)1.4 =
9017 Pa
Randomness Classical thermodynamics is deterministic
Every time! But the real world is probabilistic
It is possible that you could add heat to a system and the temperature could go down
The universe only seems deterministic because the number of molecules is so large that the chance of an improbable event happening is absurdly low
Reversible
Why? The smashing plate is an example of an
irreversible process, one that only happens in one direction
Examples: Perfume diffuses throughout a room Heat transfer
Entropy
What do irreversible processes have in common?
The degree of randomness of system is called entropy
In any thermodynamic process that proceeds from an initial to a final point, the change in entropy depends on the heat and temperature, specifically:
S = Sf –Si = ∫ (dQ/T)
Heat Reservoir
Something that is too big to change temperature
A heat reservoir can gain or lose heat
without changing temperature Since Q = mcT, if m is very large, T can
be very small
Second Law of Thermodynamics
(Entropy) Consider objects A and B that exchange heat Q with each other isothermally:
We always find that the positive term is always a larger than the negative term, so:
S>0 Entropy always increases
Entropy Problems Using Q/T Need to find heat
Sign of S is sign of Q (positive in and negative
out)
T constant for phase change or heat reservoir
For total entropy, must add all sources and
sinks of heat
General Entropy
From the first law and the ideal gas law, we get
S = nRln(Vf/Vi) + nCVln(Tf/Ti)
Note that we only need to know the initial and final conditions, not the path
Statistical Mechanics
We will use statistical mechanics to explore the reason why gas diffuses throughout a container
The box contains 4 indistinguishable molecules
Molecules in a Box There are 16 ways that the molecules can
be distributed in the box
Since the molecules are indistinguishable there are only 5 configurations
If all microstates are equally probable than the configuration with equal distribution is the most probable
Configurations and Microstates
Configuration I1 microstate
Probability = (1/16)
Configuration II4 microstates
Probability = (4/16)
Probability
There are more microstates for the configurations with roughly equal distributions
Gas diffuses throughout a room because the probability of a configuration where all of the molecules bunch up is low
Irreversibility Irreversible processes move from a low
probability state to a high probability one
All real processes are irreversible, so entropy will always increases
The universe is stochastic
Arrows of Time
Three arrows of time:
Direction in which entropy increases
Direction that you do not remember
Direction of increasing expansion of the universe
Entropy and Memory
Memory requires energy dissipation as heat
Psychological arrow of time is related to the thermodynamic
Synchronized Arrows Why do all the arrows go in the same direction?
Can life exist with a backwards arrow of time?
Does life only exist because we have a universe with a forward thermodynamic arrow? (anthropic principle)
Heat Death
Everything in the universe trying to be same temperature
Universe gets more and more disordered Left with white dwarfs, neutron stars and
radiation Can live off of compact objects, but eventually will
convert them all to heat
Suppose it is 0 F outside today. What would the temperature need to be outside tomorrow (in F) to be twice as hot?
A) -34B) 0C) 100D) 458E) 510
How much heat does it take to change the temperature of one mole of a monatomic ideal gas 1 degree K in a constant volume process? How much heat does it take to change the temperature of one mole of a monatomic ideal gas 1 degree K in a constant pressure process?
A) 1 J : 1 JB) 1 J : 12.5 JC) 12.5 J : 12.5 JD) 12.5 J : 20.8 JE) 8.3 J : 16.6 J
What is the change in internal energy for an ideal monatomic gas whose temperature increases 1 degree K in a constant volume process? What is the change in internal energy for an ideal monatomic gas whose temperature increases 1 degree K in a constant pressure process?
A) 1 J : 1 JB) 1 J : 12.5 JC) 12.5 J : 12.5 JD) 12.5 J : 20.8 JE) 8.3 J : 16.6 J