entropy 7

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Last updated 9:12 AM on 3/15/26
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50 Terms

1
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For an ideal monatomic gas, how does the number of microstates depend on macroscopic variables?

Ω(U,V,N) ∝ V^N · U^(3N/2)

2
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Why does increasing volume increase entropy even if temperature stays constant?

Increasing volume increases positional microstates available to particles.

3
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Why does increasing temperature increase entropy even if volume stays constant?

Higher energy allows more possible momentum microstates.

4
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Why does entropy scale with particle number N?

Each particle adds degrees of freedom, multiplying possible microstates.

5
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If volume doubles for one particle, how does Ω change?

It doubles.

6
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If volume doubles for N particles, how does Ω change?

Ω ∝ V^N so microstates increase exponentially.

7
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Example: if 4 particles double volume, how does Ω change?

Ω₂/Ω₁ = (V₂/V₁)^4 = 2^4 = 16

8
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Why does entropy depend on the logarithm of microstates?

Because microstates multiply while entropy must scale linearly with system size.

9
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Using Boltzmann equation, what is entropy change between two states?

ΔS = k_B ln(Ω₂/Ω₁)

10
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Using Ω ∝ V^N, derive entropy change for volume change.

ΔS = k_B N ln(V₂/V₁)

11
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Convert the particle entropy equation to the mole form.

k_B N = nR so ΔS = nR ln(V₂/V₁)

12
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Why can ΔS be calculated using reversible heat even if the process is irreversible?

Because entropy is a state function.

13
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Why does the entropy formula use q_rev instead of actual heat?

Entropy is defined using a reversible reference path.

14
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If a process is irreversible, what heat must be used to calculate ΔS?

The reversible heat q_rev.

15
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Does entropy depend on the path taken?

No, it depends only on initial and final states.

16
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For isothermal expansion of an ideal gas, what is ΔU?

ΔU = 0

17
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Why is ΔU = 0 during isothermal expansion?

Internal energy depends only on temperature.

18
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If ΔU = 0 during isothermal expansion, what relationship must hold between q and w?

q = −w

19
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What is the reversible work for isothermal expansion?

w = −nRT ln(V₂/V₁)

20
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What is the heat absorbed during reversible isothermal expansion?

q = +nRT ln(V₂/V₁)

21
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What is the entropy change for isothermal expansion?

ΔS = nR ln(V₂/V₁)

22
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Why does heating at constant volume increase entropy?

Increasing temperature increases the number of accessible energy microstates.

23
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What is the entropy change at constant volume when temperature changes?

ΔS = nC_V ln(T₂/T₁)

24
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What is the heat equation at constant volume?

qv = nCV ΔT

25
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Why is work zero at constant volume?

w = −PΔV and ΔV = 0.

26
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What is the entropy change at constant pressure when temperature changes?

ΔS = nC_P ln(T₂/T₁)

27
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At constant pressure, what thermodynamic quantity equals heat?

q_p = ΔH

28
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What is the entropy formula involving pressure and temperature?

ΔS = nC_P ln(T₂/T₁) − nR ln(P₂/P₁)

29
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What contributes to positional entropy?

An increase in volume or available space.

30
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What contributes to thermal entropy?

An increase in temperature.

31
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What is the full entropy equation for an ideal gas with both V and T changes?

ΔS = nR ln(V₂/V₁) + nC_V ln(T₂/T₁)

32
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What is the entropy change of the surroundings?

ΔSsurr = −qsys / T_surr

33
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Why do we use the surroundings temperature instead of the system temperature?

The surroundings act as a large constant-temperature reservoir.

34
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Why does heat for surroundings have the opposite sign of system heat?

Energy conservation between system and surroundings.

35
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What is the condition for a spontaneous process?

ΔS_universe > 0

36
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What is the condition for equilibrium?

ΔS_universe = 0

37
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What happens if ΔS_universe < 0?

The process is nonspontaneous.

38
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What must be true for reversible expansion?

External pressure must be infinitesimally close to internal pressure.

39
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What is the work equation for irreversible expansion against constant external pressure?

w = −P_ext ΔV

40
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Why does reversible expansion produce more work than irreversible expansion?

The gas pushes against higher pressure throughout the expansion.

41
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What is the sign of entropy change during expansion?

Positive.

42
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What is the sign of entropy change during compression?

Negative.

43
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What is the sign of entropy change during heating?

Positive.

44
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What is the sign of entropy change during cooling?

Negative.

45
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Why is ΔS_system identical for reversible and irreversible paths?

Because entropy depends only on initial and final states.

46
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Which entropy term differs between reversible and irreversible processes?

The entropy change of the surroundings.

47
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Why is ΔS_universe larger for irreversible processes?

Irreversible processes generate additional entropy.

48
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What is ΔS_universe for a reversible process?

0

49
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What is ΔS_universe for a spontaneous irreversible process?

Positive.

50
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Why does adding heat at higher temperature produce a smaller entropy change?

Because ΔS = q/T and larger T reduces ΔS.

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