entropy - Helios
Download
Report
Transcript entropy - Helios
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 = nCVDT, CV = (f/2)R = (3/2) R
Q = (3)(3/2)R(100) = 3740 J
He gas, isobarically
Q = nCPDT, CP = CV + R = (5/2) R
Q = (3)(5/2)R(100) = 6333 J
H2 gas, isochorically
Q = nCVDT, CV = (5/2) R, f = 5 for diatomic
Q = (3)(5/2)R(100) = 6333 J
H2 gas, isobarically
Q = nCPDT, 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=pDV = (19475)(0.78-0.45) = 6427 J
Q=nCp DT = (4)(7/2)(8.31)(457-263.7) =22489 J
adiabatic process starts at the same point, ends where
V= 0.78 m3.
piVig = pfVfg
pf = piVig /Vfg = (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:
DS = Sf –Si = ∫ (dQ/T)
Isothermal Entropy
DS = (1/T) ∫ dQ
DS = Q/T
Like heating something up by 1 degree
Heat Reservoir
Something that is too big to change
temperature
A heat reservoir can gain or lose heat
without changing temperature
Since Q = mcDT, if m is very large, DT 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:
DS>0
Entropy always increases
Entropy Problems Using Q/T
Need to find heat
Sign of DS 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
DS = 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 I
1 microstate
Probability = (1/16)
Configuration II
4 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)
Fate of the Universe
Head towards the Big Crunch
Will the others reverse as well?
Expand forever
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
Next Time
Read: 20.5-20.7
Suppose it is 0 F outside today. What would
the temperature need to be outside
tomorrow (in F) to be twice as hot?
A)
B)
C)
D)
E)
-34
0
100
458
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)
B)
C)
D)
E)
1J:1J
1 J : 12.5 J
12.5 J : 12.5 J
12.5 J : 20.8 J
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)
B)
C)
D)
E)
1J:1J
1 J : 12.5 J
12.5 J : 12.5 J
12.5 J : 20.8 J
8.3 J : 16.6 J