Thermodynamics - Entropy and Heat Capacities

0.0(0)
Studied by 0 people
call kaiCall Kai
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/14

flashcard set

Earn XP

Description and Tags

Flashcards covering molar heat capacities, Poisson's ratio for various gases, and entropy change formulas for phase transitions and gas processes.

Last updated 4:36 PM on 6/19/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

15 Terms

1
New cards

Monoatomic Gas (He,Ne,ArHe, Ne, Ar)

CV=32RC_V = \frac{3}{2}R, CP=52RC_P = \frac{5}{2}R, and Poison's Ratio (r) = 1.671.67

2
New cards

Diatomic Gas (O2,N2,H2O_2, N_2, H_2)

CV=52RC_V = \frac{5}{2}R, CP=72RC_P = \frac{7}{2}R, and Poison's Ratio (r) = 1.401.40

3
New cards

Linear Polyatomic Gas (CO2,HCNCO_2, HCN)

CV=52RC_V = \frac{5}{2}R, CP=72RC_P = \frac{7}{2}R, and Poison's Ratio (r) = 1.401.40

4
New cards

Non-linear Polyatomic Gas (CH4,H2O,NH3CH_4, H_2O, NH_3)

CV=3RC_V = 3R, CP=4RC_P = 4R, and Poison's Ratio (r) = 1.331.33

5
New cards

Reaction: 2A(g)A2(g)2A(g) \rightarrow A_2(g) (Bond Formation)

The enthalpy change is negative (ΔH<0\Delta H < 0) and the entropy change is negative (ΔS<0\Delta S < 0)

6
New cards

Entropy Change of System (ΔSsys\Delta S_{sys}) General Formula

ΔSsys=nCVln(T2T1)+nRln(V2V1)\Delta S_{sys} = n C_V \ln\left(\frac{T_2}{T_1}\right) + n R \ln\left(\frac{V_2}{V_1}\right)

7
New cards

Entropy of Fusion (ΔSfus\Delta S_{fus})

ΔSfus=ΔHfusTmp\Delta S_{fus} = \frac{\Delta H_{fus}}{T_{mp}} (per mol)

8
New cards

Entropy of Vaporization (ΔSvap\Delta S_{vap})

ΔSvap=ΔHvapTbp\Delta S_{vap} = \frac{\Delta H_{vap}}{T_{bp}} (per mol)

9
New cards

Entropy of Sublimation (ΔSsub\Delta S_{sub})

ΔSsub=ΔHsubTsub\Delta S_{sub} = \frac{\Delta H_{sub}}{T_{sub}} (per mol)

10
New cards

ΔSsys\Delta S_{sys} for Isothermal Reversible Process

ΔSsys=nRln(V2V1)=nRln(P1P2)\Delta S_{sys} = n R \ln\left(\frac{V_2}{V_1}\right) = n R \ln\left(\frac{P_1}{P_2}\right)

11
New cards

Universe Entropy (ΔSuniv\Delta S_{univ}) for Reversible Process

ΔSuniv=0\Delta S_{univ} = 0 because ΔSsys=ΔSsurr\Delta S_{sys} = -\Delta S_{surr}

12
New cards

Entropy Change for Reversible Adiabatic Process

ΔSsys=0\Delta S_{sys} = 0 and ΔSsurr=0\Delta S_{surr} = 0, hence ΔSuniv=0\Delta S_{univ} = 0

13
New cards

Entropy Change for Irreversible Adiabatic Process

ΔSsys>0\Delta S_{sys} > 0 and ΔSsurr=0\Delta S_{surr} = 0, hence ΔSuniv>0\Delta S_{univ} > 0

14
New cards

ΔSsurr\Delta S_{surr} in Irreversible Isothermal Expansion

ΔSsurr=Pext(V2V1)T\Delta S_{surr} = \frac{-P_{ext}(V_2 - V_1)}{T}

15
New cards

Spontaneous Process Criterion

A process is spontaneous when the total entropy change of the universe is positive (ΔSuniv>0\Delta S_{univ} > 0)