Physical Chemistry 2 Flashcards

1
Q

What is thermodynamics?

A

The study of energy transformations

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2
Q

What is energy and work?

A

Work - a form of energy which can transfer in and out of a system, stored in the organized motion of molecules.
It is done when an object is moved against as opposing force.

Energy - capacity to do work. Energy of a system can be changed by work and heat.

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3
Q

How is work done calculated / defined?

A

W = Fx

By definition;
dW = -Fdz
and pressure, P = F/A

So by substitution,
dW = -PAdz
and Adz has units of volume (x³)

Therefore dW = -PdV
Which can then be integrated

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4
Q

What’s a diathermic and adiabatic system?

A

Diathermic - energy can transfer in and out as heat

Adiabatic - no heat can be transferred in and out

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5
Q

What’s internal energy?

A

Total energy of a system, as a function of state, and is an extensive property (dependent on the amount of matter).

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6
Q

For an adiabatic process, what is internal energy equal to?

A

Overall energy balance:
ΔU = Q + W

However ΔQ is 0 as there is no transfer of heat so:
ΔU = W

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7
Q

For an isobaric process, what is internal energy equal to?

A

Overall energy balance:
ΔU = Q + W

Both still exist for this process (although ΔP is 0)

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8
Q

What is an isochoric process?

A

One with a constant volume.

ΔV = 0

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9
Q

For an isochoric process, what’s internal energy equal to?

A

Overall energy balance:
ΔU = Q + W

However, ΔV = 0 (and W=PΔV)
Therefore:
ΔU = Q

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10
Q

For an isothermal process, what is internal energy equal to?

A

Temperature is fixed (ΔT = 0) and it’s energy stays constant so ΔU = 0

Therefore:
Q = -W

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11
Q

For an cyclic process, what is internal energy equal to?

A

Certain processes have the same initial and final states, represented by a closed path and ΔU = 0.

Therefore:
Q = -W

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12
Q

What’s a reversible and irreversible process?

A

Reversible - the system is never more than infinitesimally far from equilibrium and an infinitesimal change in external conditions can reverse the process

Irreversible - cannot be reversed by an infinitesimal change in external conditions

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13
Q

How can work by an ideal gas be calculated?

A

Using pV = nRT and W = pΔV

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14
Q

How is heat capacity at constant volume defined/calculated?

A

Cᵥ = (dU/dT)ᵥ = Q v

->

dU = CᵥdT
For a certain range of T where Cv is constant

No work is done

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15
Q

What’s molar heat capacity and specific heat capacity (how is it found)?

A

Molar: C vm = Cv / n

Specific heat is in terms of mass

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16
Q

How’s enthalpy found?

A

H = U + pV

= internal energy + work

17
Q

How is enthalpy found for an isothermal process?

A

Change in U = 0.

Therefore ΔH = pV = ΔnRT

If no chemical reaction and no change in the # moles, ΔH = 0.
Otherwise ΔH = RTΔn

18
Q

What’s the relation between Cp and Cv?

A

Cp - Cv = nR

19
Q

What changes occur when a gas expands adiabatically?

A

Work is done since there’s a change in pV

Internal energy will fall

Temperature will decrease

Microscopic Ek of molecules will fall

20
Q

What’s the standard enthalpy of transition, Δ trs H’?

A

Standard enthalpy change accompanying a phase change.

Enthalpy is a state function, so ∆H differs only in sign for forward and reverse processes.

Phase changes include: mixing, solution, atomisation, combustion etc.

21
Q

What’s standard reaction enthalpy, ΔrH?

A

Change in enthalpy when reactants in standard states change to products in standard states
Enthalpies of mixing and separation are usually ignored.

22
Q

How is standard reaction enthalpy found?

A

= enthalpy of products - enthalpy of reactants

Enthalpy of formation often used

23
Q

What’s the standard enthalpy of formation?

What’s their reference state?

A

Changein enthalpy for formation of compound from its constituent elements in their reference states, which is the most stable state of an element at a certain temperature and 1 bar.

24
Q

What’s Kirchhoff’s law?

A

ΔᵣH(T2) = ΔᵣH(T1) + ∫(ΔᵣCp)dt

Where the quantity, ΔᵣCp, is the difference in heat capacities between reactants and products under standard conditions, weighted by stoichiometric coefficients.

ΔᵣCp = ΣvCp * [products] - ΣvCp * [reactants]
(where v is stoichiometric coefficients)

25
Q

What is the difference between exact and inexact differentials?

A

Exact - there exists a function of two variables
u(x,y) with continuous partial derivatives

– System is taken along a path, with ∆U = Uf – Ui

Inexact - An infinitesimal which is not the differential of an actual function
– System is heated, total energy transferred as heat is the sum of individual contributions along each point of the path
– Do not write ∆Q! Q depends upon the path of integration
– Path dependence is expressed by saying that dQ is an inexact differential

26
Q

What’s the second law of thermodynamics?

A

The Second Law of Thermodynamics is about the quality of energy. It states that as energy is transferred or transformed, more and more of it is wasted. It also states that there is a natural tendency of any isolated system to degenerate into a more disordered state. Entropy increases.

No process is possible in which the sole result is the absorption of heat from a reservoir and its complete process is possible in which the sole result is the absorption of heat from a reservoir and its complete conversion into work.

The total entropy of an isolated system can never decrease over time.
∆S tot> 0

27
Q

What’s entropy?

A

State function to quantify disorder and randomized motion. Increasing entropy means increasing disorder and randomized motion.

28
Q

How is the change in entropy measured for an infinitesimal change, and for an overall/measurable change?

A

Infinitesimal:
dS = dQᵣₑᵥ/T

Overall:
ΔS = ∫dQᵣₑᵥ/T

29
Q

What’s the Carnot cycle?

A

A theoretical thermodynamic cycle with 4 main steps: isothermal expansion, reversible adiabatic, isothermal compression and adiabatic reversible compression.

It’s the most efficient cycle for converting a given amount of thermal energy into work, or conversely, creating a temperature difference (e.g. refrigeration) by doing a given amount of work

The entropy change along any individual path is cancelled by the entropy change along the path it shares.

30
Q

What are the 4 stages of the Carnot cycle and how does entropy change for these stages?

A
  1. Reversible isothermal expansion from A to B
    ΔS = Qh/Th
  2. Reversible adiabatic expansion from B to C
    ΔS = 0
  3. Reversible isothermal compression from C to D
    ΔS = Q𝒸/T𝒸
  4. Reversible adiabatic compression from D to A
    ΔS = 0

Total change in entropy = dS = Qh/Th + Q𝒸/T𝒸

31
Q

How is engine efficiency calculated?

A

η = work performed / heat absorbed

η = W / Qh

[η = (Qh-Q𝒸)/Qh = 1 - Q𝒸/Qh = 1 -T𝒸/Th)

32
Q

How is entropy at a phase change calculated?

A

Δ trs S = Δ trs H/T

33
Q

What is the third law of thermodynamics?

A

The entropy of a system approaches a constant value as its temperature approaches absolute zero.

At zero entropy, there’s no disorder or thermal motion.

34
Q

How is standard reaction entropy defined?

A

The difference between molar entropies of pure, separated weighted products and reactants.

drS = vSm (prod) - vSm (react)

35
Q

How does the change in entropy relate to Q/T for an ideal cycle, and for a real engine?

A

For ideal, they’re equal.

For a real engine, dS is greater than dQ/T

36
Q

What’s Helmholtz free energy?

A

∆A is the part of change in internal energy that we are free to use for work

37
Q

What’s the formula for the standard Gibbs energy of formation?

A

∆rG = ∆rH - T ∆rS

38
Q

How can the number of moles of a product be determined, with regards to the extent of a reaction?

A

n = n(0) + v ∆Ê

39
Q

What’s Le Châtelier’s principle?

A

A system at equilibrium, when subjected to a disturbance, responds in a way that tends to minimize the effect of the disturbance.