Title: Physics 160, April 4, 2006
1Physics 160, April 4, 2006
- In the news
- More energy and thermodynamics basics
- - Reaction theory
- - 1st and 2nd Laws of Thermodynamics
- - Efficiency
- - Entropy
- First debate groups and topics
2In the newsenergy, global warming
- Hybrid cars less energy efficient, says study
- (http//www.thestandard.com.hk/news_detail.asp?pp_
cat17art_id15821sid7367550con_type1) - Bipartisan plans look to cut greenhouse gas
(http//www.sacbee.com/content/politics/story/1423
8609p-15058990c.html)
3Energy mostly from burning fuelReaction
theory
4Schematic of Reactions (Chemical or nuclear.)
Must supply energy to overcome barrier
5More on reactions
- Energy release typically measured as heat of
combustion here are some relevant numbers for
chemical reactions - Heat of combustion is an intrinsic property of a
fuelenergy barrier depends upon environment
6Reaction Barriers
- Generically, under thermal conditions only, rate
of activation over the barrier goes as - exp(-EB/kBT)
- where kB 1.38 x 10-23 J/mole-K is
Boltzmanns constant, and the temperature T is
measured in absolute (Kelvin) units. - Hydrogen as a chemical fuel low barrier to
activation (small match!) SAFETY ISSUE! - Hydrogen as a nuclear fuel (fusion) HUGE BARRIER
due to Coulomb repulsion between positively
charged Hydrogen nuclei. - Catalysts Reduce barrier height without
changing energy release. This is usually
accomplished by reducing the reaction
dimensionalitycatalysts (enzymes) in the
biological context can thereby increase reaction
rates by as much as 1020!!!!!
7Basic law of hydrocarbon reactions
- Natural gas CH4, Oil CH2, Coal CH
- For every hydrocarbon burned, approximately one
carbon dioxide is released - CH4 2 O2 ? CO2 2 H2O
- 2 CH2 3 O2 ? 2 CO2 2 H2O
- 4 CH 5 O2 ? 4 CO2 2 H2O
- In atmosphere with more than Oxygen, other
products possible - ? Release of CO2 into atmosphere from burning of
fossil fuels is unavoidable
8Estimating the characteristic energy in a
chemical bond
- Factoid One barrel (bbl) of oil has about 6
billion Joules of energy and 42 gallons of oil.
One gallon is about 4 liters, or about 4000 cm3 - Oil is approximately CH2, which has a molar mass
of 14 grams or 0.014 kg. - Oil is lighter than waterthe density is about
70 of H2O, or about 0.7 g/cm3 - Hence, one barrel of oil has about .7g/cm3 x 4000
cm3/gallon x 42 gallons 118000 g, which is
118000 g/(14 g/mole) 8400 moles 8400 moles x
6.02 x 1023 molecules/mole 5.1 x 1027
molecules. That means the energy released per
molecule on burning oil is 6 x 109 J/(5 x 1027
molecules) 1.2 x 10-18 J/molecule 7.3
eV/molecule.
9Laws of Thermodynamics
- First Law DQ DU W
- Heat change in process change in internal
energy plus work done - Energy is conserved
- Second Law
- (Version 1) The entropy of a closed system will
always increase or remain constant under any
process. - (Version 2) No heat engine, operating between
high temperature TH and low temperature Tc can
have an efficiency h exceeding 1 Tc/TH which is
the efficiency of a Carnot engine operating
between those two temperatures. (Efficiency of a
heat engine is defined as Wout/QH, where Wout is
the work done by the engine and QH is the heat
taken in at higher temperature.) - Increasing Entropy is the Arrow of Time
10Heat capacity measures temperature rise for
given heat input
- Energy goes into exciting additional motionfor
most materials, this is dominated by the
vibrational energy OR by the kinetic energy
(gases, liquids) - Property of materialcan be defined on per unit
mass or per mole basis. - Per mass dQ added heat, dT temp. change
- c (1/m) dQ/dT
- Water, solids high heat capacity Air/gases
low heat capacity. Thermal inertia
11Efficiency of Thermal Engines
12Question to ponder with your neighbors
- You are working out in the ARC gym on an
elliptical trainer machine. You are paying
attention to the readouts as you exercise. - a) You notice that you burn 1200 Cal/hour
while you produce 300 Watts according to the
readout. Noting that both these numbers are
units of energy per unit time or power, you seek
to compare them. Are they the same? If not, why
not (ie, what does each measure)? - b) Can you use these numbers to estimate your
efficiency as an electrical power plant on
the elliptical trainer? For comparison, typical
automobile engines are about 25 efficient in
converting fuel energy to mechanical work, and
coal/nuclear plants are about 30-35 efficient in
converting heat from fuel to electrical energy.
13Discussion
- 1300 Cal/hr 1300 x 4.18 x 103 J/hr x (1
hr)/(3600 sec) 1390 Watts 300 Watts! - We conclude that the 1300 Cal/hr is what you burn
internally while 300 Watts is what you produce
mechanically - Efficiency is Energy Out/Energy In 300/1390
22 - This is comparable to internal combustion
engines, low compared to electrical power plants
(30-40)
14Power Plant
15Statistical Definition of Entropy
- For a system with W states, Boltzmann showed
that the entropy per molecule S is given by -
- S kB lnW
- where kB 1.38 x 10-23 J/K is Boltzmanns
constant and ln(x) is the natural logarithm (base
e) of x. In this picture, an open system tends
to the maximum of entropy, and this is expressed
in the thermodynamic Free Energy G given by - G U TS
- where U is the internal energy and T is the
temperature. Thermodynamic stability is implied
by lower free energy, which can be achieved by
decreasing U (through, e.g., increased atomic
bonding in say a crystal vs. a liquid) or
increasing S (through increasing disorder in say
a liquid vs. a solid). At a phase change of
discontinuous type such as melting, the free
energy difference between the phases is zero.
Notice that at lower T, the free energy can be
lowered by increasing order (lowering U) more
than disorder (increasing S).
16Entropy Example Books in two rooms
- Assume you and your housemate are taking the same
courses and you have purchased the relevant N
textbooks, while your housemate has not.
Initially, all books are in your room, but at
time t0, your roommate starts bringing books to
their room, randomly moving them back and forth.
- This is a system with 2N total states since
each book can be either in your room or the
housemates room.
17- The probability PN(m) of finding m books in your
room is the number of ways to select m objects
out of N total divided by the total number of
states, ie - PN(m) 2-N N!/(N-m)!m!
- where N! N(N-1)(N-2)..(2)(1) is N
factorial - Hence, for six books we obtain the table
18N10 books
N36 books
- Above are plots of PN(m) (with lines between the
points) for N10,30. - Notice that the tendency with increasing N is for
the probability distributions become more sharply
peaked about N/2indeed for very large N the
width goes as N1/2 so that the width to peak
ratio goes to zero as 1/N1/2, and the maximum
entropy principle is clear as a statistical law
for large numbers of thingsin this case, books. - Notice that it takes energy to reorder the books!
You would supply that energy and while you
decrease the entropy of the books, you would
increase the entropy of the universe through the
waste heat you produce in the process.
19Initial book distribution
Prob in your room
N10 books
Books in your room
Prob in your room
Prob in your room
N36 books
N20 books
Books in your room
Books in your room
20Debate Topics
- Directions Spend about 30-60 minutes researching
these topics between now and Thursday. Each
group will be given about 15 minutes in class on
Thursday to prepare. - For the last 16 years there has been a battle to
open the Arctic National Wildlife Refuge for oil
drilling. If you were A you must argue pro ANWR
drilling, B you must argue against. - The state of Oregon has plans to replace the tax
per gallon of gasoline you buy in the state by a
tax on the miles you drive within the state. If
you are C you must argue pro mileage tax, and if
you are D you must argue against it.
21Debate Format
- 5 minutes presentation
- 4 minutes discussion between
- 3 minutes rebuttal
- (15 minutes prep before debates)