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(68 cards)

1
Q

what is an operational definition of temperature

A

The temperature of a substance is a measure of the mean

translational kinetic energy associated with the disordered microscopic motion of its constituent atoms or molecules.

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2
Q

direction of heat flow

A

Heat flows from a region of higher temperature toward a region of lower temperature.

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3
Q

things needed to make a theromometer

A

a system with a suitable thermometric property,

an easily duplicated method of construction

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4
Q

what does a useful thermometer have

A

reproducible readings, small heat capacity(so it doesnt change the properties of the system), a wide operating range

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5
Q

thermometric property

A

is any physical property that changes measurably with temperature

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6
Q

Good Thermometric Property

A

independent of the properties and sample-dependence of specific substance

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7
Q

pressure temp law

A

The pressure p of a fixed mass of gas at low density in a constant volume is proportional to the absolute temperature, T

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8
Q

Constant-Volume Gas Thermometer operation

A

Allow gas and system to reach thermal
equilibrium, Adjust height of mercury reservoir to
bring meniscus to the constant volume
reference mark, Measure the height h and hence determine the pressure p, Use T = ap, where a is a constant for the thermometer to determine the temperature T

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9
Q

Constant-Volume Gas Thermometer used to compare temp of systems

A

T1=ap1 T2=ap2 therfore T1/T2=p1/p2

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10
Q

Kelvin scale

A

Based on properties of an ideal gas and the 2nd Law of
Thermodynamics, Requires only a single fixed point defined as T triple point= 273.16K, The value for
T triple point is defined so that (T melting point)–(Tboiling point)= 100K

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11
Q

Celcius temperature scale

A

Uses pure water at 101 kPa to determine two fixed points, which are defined as being 100 degrees apart (hence
centigrade)

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12
Q

thermodynamic temperature scale

A

one that does not depend on the properties of the substances that are used to measure temperature

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13
Q

why is kelvin thermodynamic

A

because it is based on: Equation of state of an ideal gas, Properties of a reversible heat engine

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14
Q

Calibration of the CV Gas Thermometer

A

The triple-point of pure water gives a very reproducible temperature reference, Error bounds of +0.0μK/ –150μK are achievable. This allows determination of the calibration constant a for a CV gas
thermometer. For low pressures results become independent of the gas used.

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15
Q

how are thermodynamic properties of a system determined

A

by its thermodynamic state

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16
Q

how is the thermodynamic state of a system specified

A

by values of a suitable set of parameters known as

state variables

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17
Q

State variables

A

density ρ, enthalpy H, entropy S, internal energy

U, mass M, number of moles n, chemical potential μ,pressure p, temperature T, volume V

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18
Q

Equation of State definition

A

a mathematical relationship between state variables

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19
Q

An equation of state properties

A

exists for every thermodynamic system, cannot be determined using thermodynamics, can be determined from experiments or a molecular theory, for a closed system, relates T to two other variables

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20
Q

The equation of state of an ideal gas

A

pV=nRT, useful approximation for real gases at low

p or high T

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21
Q

Path-Independence of State

A

Independent of the path (sequence) of state-variable values used to make the change

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22
Q

The P-V-T Surface

A

The state variables p, V, T, n are the coordinates in a 4-space, The equation of state defines surfaces in this space

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23
Q

Isotherms

A

p vs V at constant temperature

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24
Q

Isobars

A

V vs T at constant pressure

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25
Isochors
p vs T at constant volume
26
critical temperature
above this the gas cant be liqified by preassure alone
27
Van der Waals Equation of State
(p+an^2/V^2)(V-nb)=nRT | a and b are empirical constants that differ for each gas
28
info about Van der Waals Equation of State
takes into account : molecular volume which is nbso the volume available for the molecules to move in is (V–nb),Intermolecular attraction is represented by an^2/V^2.This decreases the pressure at high densities
29
Virial Equation of State
pV/nRT=1+......Bn(n/v)^n | Bn are the virial coefficients. These are specific to each gas and are functions of T
30
Virial Equation of State info
uses a power-series expansion, reduces to the ideal gas equation of state at low densities, can be derived using statistical mechanics, is valid for any isotropic substance if enough terms are used.
31
Equation of State for a Simple Solid
V =V0[1+β(T−T0)−kT(p−p0)] kT=−ΔV/V0Δp is the isothermal compressibility β=ΔV/V0ΔT is the isobaric volumetric expansivity
32
Heat is
measure of the energy transferred between two systems as a result of a temperature difference,
33
specific heat capacity equation
ΔQ=cMΔT
34
Specific heat capacity holding preassure constant
c=1/M(δQ/dT)
35
Specific heat capacity holding volume constant
c=1/M(δQ/dT)
36
three mechanisms that transfer heat between systems
Conduction, Convection, Radiation
37
importance of heat transfer mechanisms depends on
nature of the systems, geometry of the systems, temperature regime involved
38
Conduction is
the transfer of heat through a medium that is stationary on a macroscopic scale
39
thermal resistance equation
R=L/κA k=thermal conductivity L=legnth A=cross sectional area
40
charge thermal equivalent
heat
41
current thermal equivalent
heat flux
42
capacitance thermal equivalent
heat capacity
43
pd thermal equivalent
temp
44
reistance thermal equivalent
thermal resistance
45
Convection
the transfer of heat via the movement of a medium on a macroscopic scale important in fluids
46
Convection forced
externally driven flow
47
Convection free
thermally induced density gradients drive the flow
48
Radiation is
the transfer of heat via electromagnetic waves, No medium is required,
49
Stefan-Boltzmann law
P=εσAT^4 for p net T^4-Tenv^4
50
Kinetic Theory of Gases assumptions
A container with volume V contains a very large number N of identical spherical molecules, each with mass m The molecular radius is small compared with the average distance between molecules and the size of the container The molecules are in constant rapid random motion and obey Newton’s laws There is no force acting between molecules except during collisions. The molecules collide with each other and with the walls of the container. All collisions are perfectly elastic The container walls are perfectly rigid and infinitely massive The gas is in equilibrium
51
Collision Frequency of molecules with wall
(N/2V)A∣v_x∣dt
52
The gas is isotropic so
v^2x=v^2y=v^2z=(1/3)v^2total
53
force exerted by gas
Fx=momentum change x arrival rate =2mv (N/2V)A∣v_x∣
54
pressure equation
force/area = 1/3Nmv^2
55
Microscopic Interpretation of Temperature
mean translational kinetic energy | per molecule
56
Internal Energy of the Ideal Gas assumptions
No intermolecular forces No rotational kinetic energy No vibrational kinetic energy
57
Internal Energy of the Ideal Gas equations
3/2NkT=3/2NnRT
58
The heat capacity of n moles of ideal gas
3/2nRT
59
velocity density | function
f(v)=Aexp(−Bv^2) v=sqrt(ln(v)/2) at half height | A=sqrt(B/pi)
60
speeds of molecules
v most probable < v average < v rms
61
Ideal gas model does not describe
``` thermal conductivity electrical resistivity viscosity diffusion because these depend on the frequency of collisions between molecules ```
62
collision rate of one molecule with other stationary molecules
(N/V)4πr^2⟨v⟩
63
collision rate of one molecule with other moving molecules
(N/V)4√2πr2⟨v⟩
64
mean free path proportionalities
λ∝T. λ∝1/p
65
viscosity
momentum transfer
66
thermal conductivity
energy transfer
67
coefficient of diffusion
mass transfer
68
Thermal Conductivity proportionalities
independent of density κ∝(1/r^2)sqrt(T/m)