lecture 3 - stanford universitydionne.stanford.edu › matsci152_2013 › lecture3_ppt.pdfgas in an...
TRANSCRIPT
![Page 1: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/1.jpg)
Lecture 3Lecture 3
Turning up the heat: Kinetic molecular theory & et c o ecu a t eo y &
thermal expansion
![Page 2: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/2.jpg)
Gas in an oven: at the “hot” of materials i science
Here, the size of helium atoms relative to their spacing is shown to scale under 1950 atm of pressure. The atoms have a certain, average scale under 1950 atm of pressure. The atoms have a certain, average speed, slowed down here two trillion fold from room temperature.
![Page 3: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/3.jpg)
Kinetic Molecular Theory
• The temperature of an ideal monatomic gas is a measure of the average kinetic energy of its atoms. g gy
• Experimental evidence for kinetic theory is generally perceived as the fist demonstration of the existence of atoms and molecules
![Page 4: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/4.jpg)
Kinetic Molecular Theory
Main idea:
D i th f th t i ll i Derive the pressure of a gas on the container walls, using Newtonian mechanics. Then, compare the expression with the
ideal gas law.
Ch i M t f M l lChange in Momentum of a Molecule
p = 2mvxp x
p = change in momentum, m = mass of the molecule, vx = l i i h di ivelocity in the x direction
![Page 5: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/5.jpg)
Rate of change of momentum:
F pt
2mvx
(2a / v )
mvx2
at (2a / vx ) aF = force exerted by the molecule, Δp = change in momentum, Δt = change in time m = mass of the molecule v = velocity in Δt = change in time, m = mass of the molecule, vx = velocity in
the x direction, a = side length of cubic container
T t l t d b N l l
PmNvx
2
Total pressure exerted by N molecules:
P x
VP = total pressure, m = mass of the molecule, p
= mean square velocity along x, V = volume of the cubic container
2xv
![Page 6: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/6.jpg)
Relating Gas Pressure to Energy
P mNvx
2
V
Mean square velocity:
V
vx2 vy
2 vz2
Mean square velocities in the x, y, and z directions are the same
2 2 2 2 3 2
Total mean square velocity for a molecule:
v2 vx2 vy
2 vz2 3vx
2
![Page 7: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/7.jpg)
Gas Pressure in the Kinetic Theory
22
1== vvNmP
P = gas pressure N = number of molecules m = mass of the
33v
V
P = gas pressure, N = number of molecules, m = mass of the gas molecule, v = velocity, V = volume, = density.
Compare with the ideal gas law:
N b f l l R T
PV = (N/NA)RT
N = number of molecules, R = gas constant, T = temperature, P = gas pressure, V = volume, NA = Avogadro’s number
![Page 8: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/8.jpg)
Mean Kinetic Energy for a Molecule
KE =12
mv2 = 32
kT
k = Boltzmann constant, T = temperature2 2
1. The temperature of an ideal monatomic gas is a measure of the average kinetic energy of its atoms measure of the average kinetic energy of its atoms.
2. When heat is added to a gas, it’s internal energy and therefore it’s temperature will increasetherefore it s temperature will increase.
3. The rise in internal energy per unit temperature is the heat capacityheat capacity
![Page 9: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/9.jpg)
Internal Energy per Mole for a Monatomic Gas
U = NA12
mv2
=
32
NAkT
U = total internal energy per mole, NA = Avogadro’s number, m = mass of the gas molecule k = Boltzmann constant T =
2 2
M l H t C it t C t t V l
m = mass of the gas molecule, k = Boltzmann constant, T = temperature
Molar Heat Capacity at Constant Volume
Cm = dUdT
= 32
NAk = 32
RdT 2 2
Cm = heat capacity per mole at constant volume (J K-1 mole-1), U t t l i t l l R t tU = total internal energy per mole, R = gas constant
![Page 10: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/10.jpg)
Maxwell’s theorem: Equipartition of Energy
Translation Rotation
Possible translational and rotational motions of a diatomic molecule. Vibrational motions are neglected.
![Page 11: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/11.jpg)
Thermal Expansion
The potential energy PE curve has a minimum when the atoms in the solid attain the interatomic separation r = r0. Due to thermal energy, the atoms will be vibrating
and will have vibrational kinetic energy. At T = T1, the atoms will be vibrating in such a way that the bond will be stretched and compressed by an amount such a way that the bond will be stretched and compressed by an amount
corresponding to the KE of the atoms. A pair of atoms will be vibrating between Band C. This average separation will be at A and greater than r0.
![Page 12: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/12.jpg)
Thermal Expansion
Vibrations of atoms in the solid. We consider, for simplicity a pair of atoms. Total d h f f b lenergy E = PE + KE and this is constant for a pair of vibrating atoms executing simple
harmonic Motion. At B and C KE is zero (atoms are stationary and about to reverse direction of oscillation) and PE is maximum.
![Page 13: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/13.jpg)
Definition of Thermal Expansion Coefficient
L 1
= thermal coefficient of linear expansion or thermal expansion
TLo p p
coefficient, Lo = original length, L = length at temperature T
Thermal Expansion
L Lo[1 (T To )]L l th t t t T L l th t t t TL = length at temperature T, Lo = length at temperature To
![Page 14: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/14.jpg)
Dependence of the linear thermal expansion coefficient (K-1) on temperature T p p ( ) p(K) on a log-log plot. HDPE, high density polyethylene; PMMA,
Polymethylmethacrylate (acrylic); PC, polycarbonate; PET, polyethylene terepthalate (polyester); fused silica, SiO2; alumina, Al2O3.
![Page 15: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/15.jpg)
Example: Expansion of a Si chip
Assume we have a 1mm long Si chip. How much will it expand upon heating to 320oC?expand upon heating to 320 C?
1 1 1 μm1 mm
![Page 16: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/16.jpg)
Negative coefficient of Thermal Expansion
Some materials contract with increasing temperature. Why?
Quartz Zirconium Tungstate
Water
![Page 17: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/17.jpg)
Molecular velocity & energy distribution
Schematic diagram of a “Stern type experiment” for determining the distribution of molecular velocities
![Page 18: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/18.jpg)
Maxwell-Boltzmann Distribution for Molecular Speeds
![Page 19: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/19.jpg)
Maxwell-Boltzmann Distribution for Molecular Speeds
m
3 / 2 mv2
nv 4N
m2kT
v2 exp
mv2kT
nv = velocity density function, N = total number of molecules, m = molecular mass, k = Boltzmann constant, T = temperature,
v = velocity
![Page 20: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/20.jpg)
Maxwell-Boltzmann Distribution for Translational Kinetic Energies
n =2
N1
3 / 2
E1/ 2 exp E
nE
NkT E exp
kT
nE = number of atoms per unit volume per unit energy at an energy E, N = total number of molecules per unit volume, k = gy , p ,
Boltzmann constant, T = temperature.
![Page 21: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/21.jpg)
Maxwell-Boltzmann Distribution for Translational Kinetic Energies
Energy distribution of gas molecules at two different temperatures. The number of molecules that have energies greater than EA is the shaded area. This
area depends strongly on the temperature as exp(-EA/kT)
![Page 22: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/22.jpg)
Boltzmann Energy Distribution
nE C exp E
k
N
pkT
nE = number of atoms per unit volume per unit energy at an energy E, N = total number of atoms per unit volume in the system, C = a constant that depends on the specific system
(weak energy dependence), k = Boltzmann constant, T = temperaturetemperature
![Page 23: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/23.jpg)
Thermal Fluctuations
Solid in equilibrium in air. During collisions between the gas and solid atoms, kinetic energy is exchanged.
![Page 24: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/24.jpg)
Electrical Noise
Random motion of conduction electrons in a conductor results in electrical noise.
![Page 25: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/25.jpg)
Electrical Noise
Ch i d di h i f i b d d h d Charging and discharging of a capacitor by a conductor due to the random thermal motions of the conduction electrons.
![Page 26: Lecture 3 - Stanford Universitydionne.stanford.edu › MatSci152_2013 › Lecture3_ppt.pdfGas in an oven: at the “hot” of materials sci ience Here, the size of helium atoms relative](https://reader033.vdocuments.site/reader033/viewer/2022060315/5f0be9917e708231d432d4fb/html5/thumbnails/26.jpg)
Root Mean Square Noise Voltage Across a R i tResistance
kTRBv 4rms R = resistance, B = bandwidth of the electrical system in which y
noise is being measured, vrms = root mean square noise voltage, k = Boltzmann constant, T = temperature