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The partial derivative of the internal energy with respect to temperature at a constant volume (∂U/∂T)V
heat capacity at a constant volume Cv
molar heat capacity at a constant volume (Cv) for water due to translational and rotational motions is
Cv = 3 R
Etrans = 3/2 R
Erot-nonlinear = 3/2 R
molar heat capacity at a constant volume (Cv) of hydrogen gas due to translational and rotational motions is
Cv = 5/2 R
Etrans = 3/2 R
Erot-linear = 2/2 R = R
molar heat capacity at a constant volume (Cv) for helium gas is
Cv = 3/2 R
what is the correct expression of the partial derivative (∂U/∂V)T = T(∂p/∂T)V - P that obeys the van der Waals equation
(∂U/∂V)T = an2 / V2
isothermal compressibility kt
kt = -1/V (∂V/∂P)T
for an ideal gas is equal to
1/P
how many vibrational motions are present for a linear molecule
3N - 5
where N = number of atoms
how many vibrational motions are present for a nonlinear molecule
3N - 6
where N = number of atoms
rotational levels are typically _____ to one another than electronic levels are
closer
which partial derivative is zero for an ideal gas
(∂U/∂V)T
q = ΔU at constant ___
q = ΔH at constant ___
V , P
from ΔrGo = -RT ln (K) what can be said about favoring products/reactants
products are favored if ΔrGo < 0 and K > 1
consider reaction A ⇌ B, if the reverse is spontaneous (endergonic) at a constant temperature and pressure,
μB > μA and ΔrGo > 0
A and B form an ideal solution when mixed. Vapor pressure of A at 25o C is 50 torr and of B is 30 torr. In an equilibrium molar mixture (xA = xB) what is the vapor pressure of A
25 torr
colligative properties
vapor pressure depression
boiling point elevation
freezing point depression
osmotic pressure
based on vant hoff equation
d ln (k) / dT = ΔrHo / RT2
for an exothermic reaction, if temperature rises, then K will
decrease and the equilibrium will shift away from the products
what is the maximum number of phases that can be in mutual equilibrium in a four-component system?
F = C - P + 2
0 = 4 - P + 2
P = 6
two phases are in equilibrium when
their chemical potentials of each component are equal at a constant temperature and pressure
what pair of substances would most likely mix to form an ideal solution
benzene/toluene
how is the enthalpy of sublimation of a substance related to its enthalpy or vaporization
enthalpy of sublimation is greater than enthalpy of vaporization
joule thomson coefficient
temperature behavior with respect to pressure in a constant enthalpy process, will predict whether a real gas heats or cools on pressure change, can be predicted by the equation of state of the real gas
a and b in van der waals equation
a = attractive forces between molecules
b = volume of gas itself
distance dependance of intermolecular forces
imf exist between real gas particles
low pressure = low attraction
high pressure = high attraction
compressibility factor of a gas (z)
how close a gas behavior is to ideal
z = 1 → ideal
compressibility factor (z) at low pressure
z < 1
reduced parameters in terms of critical parameters
reduced = parameter / critical parameter
ex: Tr = T / Tc
ideal gas law
PV = nRT
critical point
point at the highest temperature end at the liquid/vapor phase equilibrium line in a one component equilibrium diagram, liquid and gas phase become indistinguishable
enthalpy of vaporization at critical point
0
density of gas at critical point
density of gas becomes that of the liquid
pv graph - critical point
derivative is 0
approximate magnitude of molecular size
1 cm3 mol-1
final pressure of a mixture
Pfinal = P1 + P2 + P3 + …
internal pressure of ideal gas (partial derivative)
(∂U/∂V)T = 0
isothermal expansion work
w = -nRT ln (Vf/Vi)
adiabatic expansion work
w = -Pex dV
adiabatic
no heat can enter or leave the system
q = 0
U = w
zeroth law of thermodynamics
In closed systems A,B, and C, if A and B are in thermal contact and B and C are in thermal contact, A and C will be in thermal equilibrium with each other
first law of thermodynamics
ΔU = q + w
When energy changes, it is as heat or as work
second law of thermodynamics
In an isolated system, a spontaneous change occurs with an increase in entropy of the system
third law of thermodynamics
Absolute entropy approaches 0 as the absolute temperature approaches 0
Unique property of ideal gases
Internal energy depends only on temperature, not volume or pressure (ideal gases have no volume and have an internal pressure of zero)
Definition of entropy (Boltzman)
S = R ln(ω)
ω is number of microstates for 1 mol of material
Enthalpy as a state function / Hess law
ΔrHo = ΔHfoproducts - ΔHforeactants
ΔHfoproducts and ΔHforeactants are both multiplied by molar coefficients
Reverse the equation = reverse the sign
Spontaneity conditions for thermodynamic properties
(ΔG)T,P < 0 is spontaneous
Calculation of heat capacity
q = Cp ΔT
(∂G/∂P)T =
V
state function
not path dependent
enthalpy definition
H = U + PV
Definition of chemical potential
μi = (∂G/∂ni)T,P,nk
relationship between number of moles and in the change of enthalpy and internal energy
ΔH = ΔU + Δng RT
Efficiency equation
𝜂 = |w| / q1hot
𝜂 = 1 - (tcold - thot)
Max non pv work
ΔG
Max pv work
ΔA
Finding entropy as the integral from t1 to t2 on a graph
X axis = ln (t)
Y axis = Cp
Application of first law of thermodynamics
|q1 + q2| = |w1 + w2|
What happens to enthalpy of vaporization as you reach critical point
goes to 0, non-linear
clapeyron equation
dP/dT = ΔS/ΔV
dP/dT = ΔH/TΔV
Increasing pressure increases melting point temperature
Raoult’s law
Pi = xi Pi*