thermodynamics (chem) Flashcards

1
Q

State functions/state variables

A

Any measurable property which can be defined for a system present in a state is called state function. doesnt depend upon path followed

e.g. moles, temperature, pressure, density, mass

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2
Q

Path functions

A

Quantities defined at path as well as values depending on path

Heat (Q), Work (W)

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3
Q

Isothermal process

A

Temperature remains constant throughout the process
dT = 0
ΔT = if∫dT = 0

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4
Q

Isobaric process

A

Pressure remains constant throughout the process
dP = infinitesimally small change in P = 0

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5
Q

Isochoric process

A

Volume remains constant throughout the process
dV = 0

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6
Q

Adiabatic process

A

No heat exchange throughout the process
dq = 0

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7
Q

Cyclic process

A

System undergoes a series of processes and finally comes back to its original state, then the process is collectively known as cyclic process

Change in state function is zero in cyclic processes

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8
Q

Heat capacity of substance (c)

A

The amount of heat required/released by a substance to increase or decrease its temperature by 1 Celsius or 1K for a substance

C= dq/dT (heat req or released/ Change in temp)

unit: J/K or cal/K

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9
Q

Specific heat capacity (Cs)

A

The amount of heat required/released by 1g of a substance to change its temperature by 1oC

Heat capacity per unit mass of a substance

Cs = C/m
= dq/m dT

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10
Q

Molar heat capacity (Cm)

A

intensive property (mass independent/non-additive)
Heat capacity per mole of a substance

Cm = C/n
= dq/n dT

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11
Q

molar heat capacity at constant pressure, volume

A

heat capacity at
constant pressure: Cp
constant volume: Cv

molar heat capacity at
constant pressure: Cpm
constant volume: Cvm

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12
Q

Relation between Cpm and Cvm for ideal gas

A

Cpm - Cvm = R (gas constant)
Cp - Cv = nR (gas constant)
Cpm/Cvm = γ (specific heat ratio)
Cvm = R/(γ -1)

only valid for molar heat capacities and not for specific heat capacity

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13
Q

Internal energy (U or E)

A
  • It is a state function
  • It is an extensive property (mass dependent)
  • for a system internal energy is the sum of all types of molecular energies as follows= KE of particles + PE of particles
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14
Q

First law of thermodynamics

A
  • Related to conservation of energy
  • Can neither be created nor destroyed, only transformed from one form to another
  • the total energy of the universe remains conserved

dU = dq + dw
ΔU = q + w

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15
Q

IUPAC sign convention
1. heat given to the system
2. heat absorbed by the system
3. heat released by the surroundings

A

all +ve

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16
Q

IUPAC sign convention
1. Heat given by the system
2. Heat released by the system
3. Heat absorbed by the surroundings

A

All -ve

17
Q

IUPAC sign convention
1. work done on the system
2. work done by the surroundings
3. work done by the system
4. work done on the surroundings

A

1 and 2 are +ve
3 and 4 are -ve

18
Q

Calculation of work donr

A

dW = -pextdV
compression: dV —> -ve
expansion dV —> +ve

19
Q

irreversible work done

A

done against constant external pressure
W = -pext(V2 - V1)

20
Q

reversible work done

A

dW = PintdV
for ideal gas
dW = -PgdV
dW = -nRT/V dV
integrating both sides from V1 to V2

W = -2.303nRT log(V2/V1)
IDEAL GAS, REVERSIBLE, ISOTHERMAL WORK

21
Q

work done from graph

A

area under P-V curve

22
Q

for an ideal gas del U is a function of ___?

A

Temperature

23
Q

pressure in vacuum

A

zero

24
Q

change in internal energy for an ideal gas

A

ΔU = CvΔT
ΔU = nCvmΔT
ΔU = mCvsΔT

25
Q

Enthalpy (H)

A
  • form of energy
  • state function
  • extensive property
  • for a system it is defined as the total heat (energy) content of the system and it is given as

H = U + PV

26
Q

enthalpy for ideal gas

A

H = U + PV
H = U + nRT
both U and nRT are f(t)

therefore, for ideal gas H is a function of temperature

27
Q

relation between ΔH and ΔU for gaseous species

A

ΔH = ΔU + RTΔng

Δng = ng,p - ng,r

28
Q

Entropy

A
  • state function
  • extensive property
  • measure of randomness/disorderness/disturbance
  • third law
29
Q

entropy of pure substance vs mixture

A

S of pure < S of mixture

30
Q

In solids, what has more entropy crystalline or amorphous

A

amorphous because crystalline substances have regular arrangement of particles

31
Q

Second law of thermodynamics

A
  • Complete conversion of heat into work is not possible
  • Heat cant flow from a low temp body to a high temp body without application of external help
  • Spontaneous process cannot proceed in reverse direction in similar conditions
  • During a sponteneous process entropy of the universe increases and at equilibrium it remains constant

ΔS (univ) >= 0

32
Q

If ΔS
1. > 0
2. = 0
3. < 0

A
  1. spontaneous ΔS > 0
  2. equilibrium ΔS = 0
  3. non spontaneous ΔS < 0
33
Q

Third law of thermodynamics

A

At absolute zero temperature (0K) the entropy of a crystalline substance is zero

34
Q

Gibbs free energy (G)

A
  • state function
  • extensive property

ΔG = ΔH - TΔS