Title: Heat and Waves
1Heat and Waves
2Reading Memo Insights
- How do you convert Fahrenheit to Celsius?
- C 5/9 (F - 32)
- Why is it that water stays the same temp when it
hits its boiling point no matter how long you
keep heat on it? - What is an Absolute Zero?
- Heat passes through a vacuum and heats through
radiation? - Are wave movements always symmetrical?
3Summary of Important Equations to understand for
the HW
- ?l a l ?T
- CHANGE in Internal Energy ?U W Q
- Q m c ?T
- v v(F/?)
- v f ? (for light, c ? f)
4Temperature
- Intimately tied to the idea of Energy (see intro
to analogy for energy) - Three scales
- Fahrenheit, Celsius, and Kelvin
- Kelvin Temperature is a measure of the average KE
of particles ? particles have KE! - Higher temperature ? particles move faster ?
higher KE - http//plabpc.csustan.edu/general/tutorials/temper
ature/temperature.htm - Liquids/Solids are bound (solids bound more
tightly than liquids - Imagine connected with springs) ? some particles
also have PE! - Vibrate through greater distance when Temperature
goes up - This vibrational/elastic PE is important in phase
changes - PE is negative when bound
- http//hyperphysics.phy-astr.gsu.edu/hbase/thermo/
inteng.htmlc3
5Temperature vs. Internal Energy
- (Kelvin) Temperature is a property of a typical
molecule of a substance -- how many molecules
there are doesn't matter - Internal Energy, on the other hand, is the total
energy of all the particles - E.g., you can have a few high speed particles in
a very dilute gas, giving it a high temperature
but little total energy, or many low speed
particles in a dense liquid, giving it a low
temperature but a greater total energy overall.
The high temperature dilute gas would not be able
to transfer much heat to a cooler substance but
the lower temperature liquid would! - Absolute Zero (-273.15 oC)
- Average KE almost zero
- Cannot be reached HUP
- Low temperatures superfluids, superconductors,
etc. - High temperatures KE high so no binding so no
liquids/solids - Above 20,000 K electrons break free plasmas only
6Thermal Expansion
- Unconstrained substances expand with increased
temp - Bridges expand in summer, contract in winter
- In gases, higher temp ? higher speeds
- In liquids/solids, more heat added ? vibrate
through larger distance - ?l a l ?T
- a ? coefficient of linear expansion
7In Class Exercise 1
- In summer, lbridge 1,000 m when T 35 oC.
- Calculate change in length on a winter day when
Tf -5 oC - a 12 x 10-6/oC (see Example 5.1 on p. 171)
Known Unknown
lbridge, summer 1,000m
?lwinter ?m
Ti, summer 35oC
Tf, winter -5oC
a 12 x 10-6/oC
- ?T is negative
- ?l is also negative
- This expansion/contraction used in bimetallic
strips in thermostats (Fig 5.9 on p. 172)
8Expansion
- Liquids also expand/contract
- Exception Dice lt Dwater (water expands upon
freezing) - Gases expand too V µ T
- Gases expand 10, liquids 5, and solids 1 with
temperature - Ideal Gas Law PV nRT
- Increasing Temp ? Increasing Volume ? DECREASING
mass ( weight) density - Temperature does not change mass or weight itself!
9Two ways to increase Temp (or energy, since T
KE)
- 0th Law of Thermodynamics
- Temp measures thermal equilibrium (Ta Tb Tc
so Ta Tc) and heat flows from TH to TL - Expose to reservoir at higher Temp (HEAT
TRANSFER) - Doing Work on it (WORK TRANSFER)
- Experiment by James P. Joule established
established relationship between mechanical work
and heat - Temperature depends on average KE of atoms and
molecules - 1st Law of Thermodynamics
- Internal Energy (of atoms molecules) U (KE
PE)atomic - Gases only have KE
- Liquids/solids also have PE (since they're bound
and oscillate)
10U increases with increasing Temp
- Heat, Q, is a form of energy that flows from TH
to TL - As Heat flows, energy is transferred (like work
in mechanics) - As work is done, energy is transferred/transformed
in mechanics - Q and W are energy in transition while U and PE
are stored energy -
- What quantities are measured in units of Joules?
- Energy (KE, PE, and U), which is changed by
- Work
- Heat
- That's because they're all different forms of
energy (stored or in transition)
In Energy in Transition Stored Energy
Mechanics Work transfers energy to/from ? Mechanical Energy (KE PE)
Thermodynamics Heat transfers energy to/from ? Internal Energy
11Review the story so far...
- Atoms have KE and PE ? Internal Energy, U
- We know Work (W) can change the energy (U) and is
energy in transition - We also know that Heat (Q) changes Temperature
(T) ? which is equal to the average KE of the
particles - Therefore, Q also changes energy and is also
energy in transition - So if we can somehow find both Q W, we can
figure out exactly how much the energy of a
system changes and don't need to know anything
about the microscopic U of each atom!
121st Law CHANGE in Internal Energy
- CHANGE in Internal Energy ?U W Q
- http//hyperphysics.phy-astr.gsu.edu/hbase/thermo/
inteng.htmlc3 - W means work done on gas (W -pdV -p?V) and
Q means heat flowing into gas - W F d but if something is dropped from a
building, the distance is just the ?h So W
F?h. But p F/A so F pA. Now Work becomes W
pA?h. But Ah is Volume so W p?V. Now, since
Volume is decreasing (e.g., dropped from a higher
height to a lower height), this is actually
negative of that W -p?V - Restatement of conservation of energy
- Internal Energy is essential to understanding
phase transitions - When Heat is transferred but Temp. remains same ?
Heat goes to PE (to break bonds) - We already know how to calculate work so if we
can now quantify heat, we can figure out ?U
without knowing anything about the microscopic
nature of U!!!
13Heat Transfer Conduction(Solids Liquids)
- Conduction transfer of energy via direct contact
- Takes place at boundary between 2 substances
- Via collision of atoms and molecules
- Conduction poor in gases (direct contact rare)
- Materials with trapped air become good thermal
insulators - A rug is not warmer than cold floor
- Poorer conductor ? less heat conducted away from
feet - Metals are good thermal conductors
- Conduction electrons carry U from hot to cold
areas (valence electrons available for bonding)
14Heat Transfer Convection(Fluids Liquids
Gases)
- Convection transfer of energy by buoyant mixing
in a fluid - Thermal Buoyancy when fluid is heated, it's
Density decreases - Hotter, less dense fluid rises
- Cooler, denser surrounding fluid pushes it up ?
FB, just like in the Law of Archimedes we studied
in the last chapter - Conduction occurs between warm, rising fluid and
cold, static fluid - Cools and falls back down mixing leads to
convection currents - Examples
- Convection happens in the atmosphere oceans
- Sun warming Earth leads to sea/land breezes and
thermals - Sun warms water at Equator leads to underwater
currents
15Heat Transfer Radiation(EM Waves)
- Radiation transfer of energy via electromagnetic
waves - Can operate in a vacuum
- Emission is mainly in the IR part of the spectrum
(for substances with T lt 430oC) - U of atoms converted to EM energy radiation
- Radiation carries the energy through space until
it's absorbed - Upon absorption, converted to U of atoms of
absorbing substance - Everything emits EM Radiation
- Hotter things emit more IR and Visible light
- Emission of radiation cools absorption warms
- Cooling by emission is similar to cooling by
evaporation (which is analogous to a baseball
team's batting average going down when its best
hitters are traded) - Hold hand to side of lightbulb radiation warms
- Place above, both radiation and convection of
heated air warms
16Summary
- Atoms have both KE PE ? Internal Energy (U)
- We know Work (W) is energy in transition and can
change U - Since Heat (Q) changes the Temperature (T ? is
equal to the average KE of the constituent
particles), we know that Q is also energy in
transition - So if we can find both Q W, we can get the
change in Internal Energy (?U) without any
reference whatsoever to the microscopic U of each
individual atom/molecule - Since we already know how to calculate (or
quantify) Work, all we need to do is figure out
how to quantify Heat (Q) now...
17Specific Heat Capacity Q m c ?T
- Heat is transfer of energy
- Units of Joules and c has units of J/kg-oC
- Amount of Q needed to raise T of 1 kg by 1 oC
- Larger c ? more Q needed to raise T by 1oC
- cwater is really high can absorb or release
large amounts of Q (that's why it's used in
radiators, power plants, etc.)
18In Class Exercise 2
- How much heat must be added to 1 cup (0.3 kg) of
water to boil it (raise it from 20 oC to 100 oC)?
- Note cwater 4.18 kJ/kg-oC (see example 5.2 on
p. 186)
Known Unknown
m 0.3kg
Q ? J
Ti 20oC
Tf 100oC
cwater 4.18 kJ/kg-oC
- Q mc ?T 0.3kg 4.18kJ/kg-oC 80oC
19Mechanical Energy can be converted into Heat
Energy
- Mechanical Energy (PE or KE) can be converted
into Heat (Q) through Friction - This extra Heat Energy raises the Temperture ?
which raises the Internal Energy - But ?T is tiny (e.g., if you assume all KE goes
to Q, even then KE Q m c ?T -- see p. 156) - Usually Mech Energy isn't large enough to change
T significantly (satellite re-entry exception) - James P. Joule established equivalence of
mechanical energy and heat - 1 cal 4.184 J (1 food cal 1 kcal)
20Phase Transition
- Particles "trapped" in a bound state have
negative PE - http//hyperphysics.phy-astr.gsu.edu/hbase/thermo/
phase.htmlc4 - Negative energy compared to free particles
- Bound atoms are also said to have negative PE
- Answer to reading memo Adding heat to boiling
water no longer increases KE - Instead, heat energy goes into breaking the bonds
- Thus, increases PE from negative to 0 (breaking
of bonds) - Molecule becomes water vapor and leaves liquid
water - Same thing happens in melting
- Heat energy goes to increasing PE
- Makes bonds "looser" than they are in a solid
- Temperature remains constant
- Transparency Figure 5.34 on p. 190
PE0
- PE
21Phase Transitions (contd.)
- Transparency Figure 5.34 on p. 190
-
- Phase transitions also depend on pressure (more
pressure higher T) - Heat needed for transitions is latent heat of
fusion (solid-to-liquid) and latent heat of
vaporization (liquid-to-gas)
Temperature
Gas
Boiling
Liquid
Melting
Heat
Solid
22The Second Law of Thermodynamics (Skip)
- Heat engine transforms heat energy into
mechanical energy - 2nd Law Some heat has to go to a reservoir at TL
- Efficiency (Work/QH) 100 Carnot eff (TH
- TL)/TH 100 - Heat Movers (e.g., refrigerators) use Energy
Input and Phase Transitions to reverse process - Alternative form of 2nd Law dS dQ/T ? i.e.,
there is Entropy
23Wave Types Properties
- Waves move and carry energy but do not have mass
- A wave is a disturbance that travels through a
medium (for material waves) from one location to
another. Waves are said to be an energy transport
phenomenon. As a disturbance moves through a
medium from one particle to its adjacent
particle, energy is being transported from one
end of the medium to the other. A pulse is a
single disturbance moving through a medium from
one location to another location. The repeating
and periodic disturbance which moves through a
medium from one location to another is referred
to as a wave. (see also http//www.glenbrook.k12.i
l.us/gbssci/phys/Class/waves/u10l4a.html) - Like Q and W, waves can also be thought of as
energy in transition! - It's a wave if1) energy moves from one place to
another and 2) matter doesn't move from one place
to another (for the most part) - Transverse waves oscillations are perpendicular
(transverse) to direction of wave travel (EM)
(http//id.mind.net/zona/mstm/physics/waves/par
tsOfAWave/waveParts.htm)
24Wave Anatomy Properties
- Longitudinal waves oscillations are along
direction of travel (Sound) - Pulse single wavefront Continuous wave many
wavefronts - Wave properties and Wave Anatomy
http//www.sciencejoywagon.com/physicszone/lesson/
09waves/introwav/sld003.htm - Energy is proportional to amplitude squared
(recalling the definitions of KE -- 1/2 times
velocity squared -- and spring PE -- 1/2 k times
x squared -- should give some feel for this) - Answer to Reading Memo Some waveforms aren't
symmetrical (e.g., in noise, which isn't
periodic) - But you can always measure the amplitude, even if
you can't determine the equilibrium position, by
using a technique called peak to peak amplitude
measurement, which measures the entire height of
a waveform, top to bottom - As wavefront spreads out more and more, material
waves' amplitude decreases (since amplitude is
directly related to energy and energy is spread
over the whole wavefront, as the wavefront
expands, the amount of energy per unit length
decreases as it has to spread out more) - As wavefront spreads out more and more, it begins
to look flat becomes a plane wave (wavefronts
become straight planes rays become parallel)
25Wave Propagation
- Speed of wave rate of movement of disturbance
(depends only on medium for material waves) - v v(F/?), where F is the Tension in the string
and ? m/L (using properties of the medium) - Changes in tension and length alter the frequency
of the pulse's back and forth oscillation, just
like tuning a string or pressing a guitar string
against a fret does the same. - v f ? (using properties of the wave)
- higher frequency shorter wavelength
26In Class Exercise 3
- What is the frequency of light of wavelength 700
nm? Similar to Example 6.3 on p. 213
Known Unknown
? 700nm
f ?Hz
c 3 x 108m/s
27The Doppler Effect
- Doppler Effect wavelength shorter than when
source is at rest (in direction of motion) - http//surendranath.tripod.com/Doppler/Doppler.htm
l - Diffraction wave bends around edges if plane
wave hits opening smaller than wavelength, starts
to bend around, as if new wave originating from
that spot - Interference constructive and destructive when
overlap is ½ wavenlength, destructive when
multiple of whole wavelength, constructive
(http//www.glenbrook.k12.il.us/gbssci/phys/Class/
waves/u10l3c.html)