Transcript of Physics 105 Physics for Decision Makers: The Global Energy Crisis Lecture 8 Thermodynamics II Fall...
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- Physics 105 Physics for Decision Makers: The Global Energy
Crisis Lecture 8 Thermodynamics II Fall 2011
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- Physics 105 Fall 11 Energy Audit Energy Audit Project: Download
assignment info sheet from Elms -Group project -When you meet ->
Each person should have a role one person needs to be responsible
for organization. -Project Due Dates: Assignment #1 - Sept 30 only
one person needs to turn something in, but the whole group needs to
be involved Assignment #2 - Oct 7 Assignment #3 - Oct 21 Assignment
#4 - Oct 28 Assignment #5 (Presentations in Discussion) Oct 29 -
Nov 1. Page 2
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- Physics 105 Fall 11 Food Supply and Climate CNN today - Why is
'food security' sparking unrest -Russian Drought wiped out 25% of
their wheat crop -This caused them to stop grain exports -Bread
prices went up dramatically 30% in some countries -Riots ensued in
Mozambique Decisions we make about using biofuels can affect people
around the world Page 3
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- Physics 105 Fall 11 Activities: Guided Tours Thermodynamics:
What is Thermodynamics?
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- Physics 105 Fall 11 Page 5
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- Physics 105 Fall 11 The Zeroth Law of Thermodynamics
Temperature - if two objects are in thermal equilibrium with a
third object (like a thermometer) then they are in thermal
equilibrium with each other - -Another way of saying it is that
temperature is a measurable quantity and it tells us about the
energy content of an object - -this law asserts that we can define
a temperature function, or more informally, that we can 'construct
a thermometer'
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- Physics 105 Fall 11 Thermal Equilibrium if Q=0 then we are in
thermal equilibrium T A = T B A B Q
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- Physics 105 Fall 11 Heat Transfer Three methods Conduction
Transfer Of Energy Through Matter Air Is A Poor Conductor - Metal
is a good one Only important at the earth's surface Convection
Transfer of energy by movement of mass Can only take place in
liquids & gases - e.g. Air Convection on a global scale creates
worldwide atmospheric circulation Radiation Proportional to the 4th
power of the temperature How we get energy from the sun Why it gets
cold on a clear night
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- Physics 105 Fall 11 Fig. 2-2, p. 30
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- Physics 105 Fall 11
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- Radiation
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- Physics 105 Fall 11 The First Law of Thermodynamics Energy
Conservation Many statements: - -Energy is conserved - -Heat is a
form of energy - -The energy of an isolated system (e.g. the
universe) is constant - -Energy is conserved during any change in
state. Specifically: - -Heat absorbed by a system + work done on
the system = change in internal energy of the system
Mathematically: Q+W= U Q is heat, W is work and U is internal
energy
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- Physics 105 Fall 11 The internal energy of a system does NOT
depend on which of the following: 1. 1.The temperature of the
system 2. 2.The amount of material in the system 3. 3.The type of
material 4. 4.The amount heat that has been put into the system 5.
5.It depends on all of them
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- Physics 105 Fall 11 First Law - energy is conserved Where did
energy to power the light come from?
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- Physics 105 Fall 11 Heat Capacity The specific heat is the
amount of heat per unit mass required to raise the temperature by
one degree Celsius (or Kelvin) Heat Capacity = Q/ T - -Heat
Capacity of a lake depends on the size of the lake (extrinsic) -
-Specific Heat = Heat Capacity/kg - property of the water
(intrinsic)
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- Physics 105 Fall 11 Latent Heat Latent Heat of vaporization -
-If we add heat to water - its temperature goes up - -1 Kcal - will
raise 1kg of water 1 o C - -Until water hits 100 o C - then the
temperature stops going up - -What happens? - -It vaporizes
(boils). - -It takes 539 kcal to boil 1kg of water - -Eventually
once its all steam the temp will start going up again - -539
kcal/kg is the latent heat of vaporization
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- Physics 105 Fall 11 Latent Heat Latent heat of fusion - -Take
1kg of ice at -20 o C and add heat at a rate of 1kcal/min - -The
Ice will warm up at 2 o C/min - (why 2)? - -Once it hits 0 o C -
(after 10 min) the ice will start to melt - -It will take 80
minutes to melt the ice - -So the latent heat of fusion of ice is
80kcal/kg
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- Physics 105 Fall 11 Does the 1st law prohibit a lake from
freezing on a warm day? 1. 1.Yes 2. 2.No 3. 3.Doesnt apply
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- Physics 105 Fall 11 The 2nd Law of Thermodynamics Many
formulations: - -It is impossible to convert heat completely into
work. - -No perfect engine - -Cant just pull heat out of the
environment - -Heat cannot spontaneously flow from a material at
lower temperature to a material at higher temperature. - -No
perfect refrigerator - -In an isolated system, a process can occur
only if it increases the total entropy of the system.
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- Physics 105 Fall 11 The Perfect Heat Engine Takes heat out of
the environment and turns it into work. The solution to all of our
problems - -reduce global warming - -Solve the energy problem 2 nd
Law T1T1 Q1Q1 W out
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- Physics 105 Fall 11 Perfect Refrigerator T 1 Hot T 2 Cold
Q
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- Physics 105 Fall 11 Restatement Zeroth Law Lunch exists
(temperature) First Law TANSTAAFL (energy conserved) Second Law
(heat flows from hot to cold) - -Lunch will be expensive
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- Physics 105 Fall 11 Entropy Toss a penny N times What is
probability that you get Heads every time? ans.
(1/2)(1/2)(1/2)(1/2). = (1/2) N if N =2, p = 0.25 if N= 10, p =.001
if N= 100, p = 8 X 10 -31 if N = 10 4, p = 5 X 10 -3011 !!!! We
expect about N/2 heads What is probability that we get within 1% of
N/2? if N = 10, p = 0.25 if N=1000, p =.248 if N = 10 5, p =.998 if
N = 10 8, p = 1 - 3 X 10 -2174 !!!!
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- Physics 105 Fall 11 I flip a coin 10 times - the first 9 come
up heads.. What is the probability that the next toss is also
heads? 1. 1..001 2. 2.1 - 9/10 = 0.1 3. 3.(9/10)(1/2) = 0.45 4.
4.0.5 5. 5.9/10 = 0.9
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- Physics 105 Fall 11 Entropy - microstates Why is all heads so
rare and ~50/50 so common? - -Lets call each possible outcome a
microstate - -There is only one microstate that is all heads
HHHHHHHHHH - -There are many microstates that are ~ 50/50
HHHHHTTTTT HHHHTHTTTT HHHTHHTTTT HHTHHHTTTT TTTTTHHHHH THTHTHTHTH
Each microstate is equally likely.
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- Physics 105 Fall 11 Entropy and Particles in a box Particles
start all on left - -What happens? - -What are the odds that later
we find all of them on the left? Just like the coin tossing! After
mixing, chance of all on the left is (1/2) N It would take work
push all the molecules back to the left side
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- Physics 105 Fall 11 Entropy and the macrostate We can define
macroscopic properties - -more-or-less uniform distribution between
right and left When a physical system is allowed to evolve in
isolation, some single macroscopic outcome is overwhelmingly more
probable than any other Second Law: If a system of many particles
is permitted to change, it will evolve to the macrostate made of
the largest number of microstates, and stay there.
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- Physics 105 Fall 11 Entropy We define a quantity called entropy
- -Entropy = S = k B ln (no. of microstates) - -With this
definition, it can be shown that: - -S final - S initial = energy
input from heating/T = Q/T Second Law: S > Q/T -
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- Physics 105 Fall 11 Definition of Entropy Change in entropy S=
Q/T - -Take an example - - -Q=30J S cold =+30J/283 o K= +0.106 S
warm =-30J/333 o k= -0.09 S total = +.07J/ o k - -Entropy of the
entire system increases 10 o 60 o Q=30J
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- Physics 105 Fall 11 The 2nd Law of Thermodynamics Most systems
are microscopically reversible - -Particles in a box The 2 nd Law
tells us the direction of time
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Reversible and Irreversible Processes
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- Physics 105 Fall 11 Heat Engines Heat engines take heat from a
hot reservoir and does work and expels heat to the cold reservoir
Note that the first law says - -Q 1 =W+Q 2 The 2nd law tells us the
amount of work we can get from a temperature difference Efficiency
= (work output)/(energy in)
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- Physics 105 Fall 11 Carnot Engine The Carnot Engine is an
idealized engine that works in a reversible way -reversible -What
is a reversible engine? - -A refrigerator - -By adding work we can
take heat from the cold reservoir and deposits it to the hot
reservoir - -Again - 1st law works - -W+Q 1 = Q 2 - -Notice more
heat is delivered than work done!
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- Physics 105 Fall 11 Heat Pump Cools in summer Heats in winter
What is temperature of the air blowing out in summer and
winter?
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- Physics 105 Fall 11 Heat Pump Page 42 Winter Summer
Outside
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- Physics 105 Fall 11 Carnot Efficiency The efficiency
(work/energy in) of a Carnot Engine T 1 -T 2 )/T 1 When is the
efficiency high? - -When T 2 is low - -Example - -T 1 = 500 o C =
773K - -T 2 = 0 o C = 273K T 1 -T 2 )/T 1 = 500/773= 65% - -This
says W=65% Q 2 = 35% - -So if we take 100J from T 1 we get 65J of
work - -Redo if T 1 is 100 o C = 373k T 1 -T 2 )/T 1 = 100/373= 26%
- -so our 100J of energy only gives us 26J of work
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- Physics 105 Fall 11 Proof that no engine can have efficiency
greater than Carnot Assume Engine 1 is higher efficiency than
Carnot - -Operating between T 1 & T 2 it produces W 1. - -W 1
is greater than Wc would produce for the same Q 1. (i.e. Q 2 is
less) - -Since the Carnot is reversible run it backwards powered by
W 1. - -This will pump more heat out of the cold reservoir than
engine 1 put in as Qc >Q 2 Net result - a perfect refrigerator -
which violates the 2nd law since we are moving heat from cold to
hot with no external work (lake freezing) 1 1
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- Physics 105 Fall 11 What is the net effect of putting a
refrigerator in a room opening the door an turning it on? 1. 1.The
room cools down a little 2. 2.The room cools down a lot 3. 3.The
room heats up a little 4. 4.The room heats up a lot
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- Physics 105 Fall 11 System Properties Extensive quantities
(depend on amount of material) - -U = Internal energy - - V =
Volume - - N i = # of Moles - -Heat Capacity The intensive
quantities (do NOT depend on amount of material) - -Pressure -
-Temperature - -Specific Heat
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- Physics 105 Fall 11 Real Heat Engines Real heat engines always
are less efficient than Carnot engines In all heat engines there is
waste heat from the 2 nd law - -Electric motors are not governed by
the 2 nd although generally the production of electricity is In
real engines there is additional waste heat The Carnot engine gives
us a goal
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- Physics 105 Fall 11 Real Engine T1T1 T2T2 Q1Q1 Q2Q2 W out Q
waste
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- Physics 105 Fall 11 Car Engines efficiency of about 25% - -The
efficiency may be as high as 37% at the optimum operating point. -
-Most internal combustion engines waste about 35% of the energy in
gasoline as heat lost to the cooling system and another 35% through
the exhaust. - -The rest, about 5%, is lost to friction
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- Physics 105 Fall 11 Car Engine
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- Physics 105 Fall 11 Does it cost you fuel to use your car
heater while driving? Yes No
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- Physics 105 Fall 11 Q1Q1 Work out Q 2 out Q Waste
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- Physics 105 Fall 11 Real Engine heat recovery T1T1 T2T2 Q1Q1
Q2Q2 W out Q waste T3T3 T2T2 Q3Q3 Q2Q2 W out Q waste
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- Physics 105 Fall 11 Its possible to reduce the entropy of an
object? True False