Section 1: Classical Thermodynamics Preliminaries |
|
The Ideal Gas Law |
46:05 |
| |
Intro |
0:00 | |
| |
Course Overview |
0:16 | |
| |
| Thermodynamics & Classical Thermodynamics |
0:17 | |
| |
| Structure of the Course |
1:30 | |
| |
The Ideal Gas Law |
3:06 | |
| |
| Ideal Gas Law: PV=nRT |
3:07 | |
| |
| Units of Pressure |
4:51 | |
| |
| Manipulating Units |
5:52 | |
| |
| Atmosphere : atm |
8:15 | |
| |
| Millimeter of Mercury: mm Hg |
8:48 | |
| |
| SI Unit of Volume |
9:32 | |
| |
| SI Unit of Temperature |
10:32 | |
| |
| Value of R (Gas Constant): Pv = nRT |
10:51 | |
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Extensive and Intensive Variables (Properties) |
15:23 | |
| |
| Intensive Property |
15:52 | |
| |
| Extensive Property |
16:30 | |
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| Example: Extensive and Intensive Variables |
18:20 | |
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Ideal Gas Law |
19:24 | |
| |
| Ideal Gas Law with Intensive Variables |
19:25 | |
| |
Graphing Equations |
23:51 | |
| |
| Hold T Constant & Graph P vs. V |
23:52 | |
| |
| Hold P Constant & Graph V vs. T |
31:08 | |
| |
| Hold V Constant & Graph P vs. T |
34:38 | |
| |
| Isochores or Isometrics |
37:08 | |
| |
| More on the V vs. T Graph |
39:46 | |
| |
| More on the P vs. V Graph |
42:06 | |
| |
| Ideal Gas Law at Low Pressure & High Temperature |
44:26 | |
| |
| Ideal Gas Law at High Pressure & Low Temperature |
45:16 | |
|
Math Lesson 1: Partial Differentiation |
46:02 |
| |
Intro |
0:00 | |
| |
Math Lesson 1: Partial Differentiation |
0:38 | |
| |
| Overview |
0:39 | |
| |
Example I |
3:00 | |
| |
Example II |
6:33 | |
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Example III |
9:52 | |
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Example IV |
17:26 | |
| |
Differential & Derivative |
21:44 | |
| |
| What Does It Mean? |
21:45 | |
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| Total Differential (or Total Derivative) |
30:16 | |
| |
| Net Change in Pressure (P) |
33:58 | |
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| General Equation for Total Differential |
38:12 | |
| |
Example 5: Total Differential |
39:28 | |
Section 2: Energy |
|
Energy & the First Law I |
1:06:45 |
| |
Intro |
0:00 | |
| |
Properties of Thermodynamic State |
1:38 | |
| |
| Big Picture: 3 Properties of Thermodynamic State |
1:39 | |
| |
| Enthalpy & Free Energy |
3:30 | |
| |
| Associated Law |
4:40 | |
| |
Energy & the First Law of Thermodynamics |
7:13 | |
| |
| System & Its Surrounding Separated by a Boundary |
7:14 | |
| |
| In Other Cases the Boundary is Less Clear |
10:47 | |
| |
State of a System |
12:37 | |
| |
| State of a System |
12:38 | |
| |
| Change in State |
14:00 | |
| |
| Path for a Change in State |
14:57 | |
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| Example: State of a System |
15:46 | |
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Open, Close, and Isolated System |
18:26 | |
| |
| Open System |
18:27 | |
| |
| Closed System |
19:02 | |
| |
| Isolated System |
19:22 | |
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Important Questions |
20:38 | |
| |
| Important Questions |
20:39 | |
| |
Work & Heat |
22:50 | |
| |
| Definition of Work |
23:33 | |
| |
| Properties of Work |
25:34 | |
| |
| Definition of Heat |
32:16 | |
| |
| Properties of Heat |
34:49 | |
| |
| Experiment #1 |
42:23 | |
| |
| Experiment #2 |
47:00 | |
| |
More on Work & Heat |
54:50 | |
| |
| More on Work & Heat |
54:51 | |
| |
Conventions for Heat & Work |
60:50 | |
| |
| Convention for Heat |
62:40 | |
| |
| Convention for Work |
64:24 | |
| |
| Schematic Representation |
65:00 | |
|
Energy & the First Law II |
1:06:33 |
| |
Intro |
0:00 | |
| |
The First Law of Thermodynamics |
0:53 | |
| |
| The First Law of Thermodynamics |
0:54 | |
| |
Example 1: What is the Change in Energy of the System & Surroundings? |
8:53 | |
| |
Energy and The First Law II, cont. |
11:55 | |
| |
| The Energy of a System Changes in Two Ways |
11:56 | |
| |
| Systems Possess Energy, Not Heat or Work |
12:45 | |
| |
| Scenario 1 |
16:00 | |
| |
| Scenario 2 |
16:46 | |
| |
| State Property, Path Properties, and Path Functions |
18:10 | |
| |
Pressure-Volume Work |
22:36 | |
| |
| When a System Changes |
22:37 | |
| |
| Gas Expands |
24:06 | |
| |
| Gas is Compressed |
25:13 | |
| |
| Pressure Volume Diagram: Analyzing Expansion |
27:17 | |
| |
| What if We do the Same Expansion in Two Stages? |
35:22 | |
| |
| Multistage Expansion |
43:58 | |
| |
| General Expression for the Pressure-Volume Work |
46:59 | |
| |
| Upper Limit of Isothermal Expansion |
50:00 | |
| |
| Expression for the Work Done in an Isothermal Expansion |
52:45 | |
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Example 2: Find an Expression for the Maximum Work Done by an Ideal Gas upon Isothermal Expansion |
56:18 | |
| |
Example 3: Calculate the External Pressure and Work Done |
58:50 | |
|
Energy & the First Law III |
1:02:17 |
| |
Intro |
0:00 | |
| |
Compression |
0:20 | |
| |
| Compression Overview |
0:34 | |
| |
| Single-stage compression vs. 2-stage Compression |
2:16 | |
| |
| Multi-stage Compression |
8:40 | |
| |
Example I: Compression |
14:47 | |
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| Example 1: Single-stage Compression |
14:47 | |
| |
| Example 1: 2-stage Compression |
20:07 | |
| |
| Example 1: Absolute Minimum |
26:37 | |
| |
More on Compression |
32:55 | |
| |
| Isothermal Expansion & Compression |
32:56 | |
| |
| External & Internal Pressure of the System |
35:18 | |
| |
Reversible & Irreversible Processes |
37:32 | |
| |
| Process 1: Overview |
38:57 | |
| |
| Process 2: Overview |
39:36 | |
| |
| Process 1: Analysis |
40:42 | |
| |
| Process 2: Analysis |
45:29 | |
| |
| Reversible Process |
50:03 | |
| |
| Isothermal Expansion and Compression |
54:31 | |
| |
Example II: Reversible Isothermal Compression of a Van der Waals Gas |
58:10 | |
| |
| Example 2: Reversible Isothermal Compression of a Van der Waals Gas |
58:11 | |
|
Changes in Energy & State: Constant Volume |
1:04:39 |
| |
Intro |
0:00 | |
| |
Recall |
0:37 | |
| |
| State Function & Path Function |
0:38 | |
| |
First Law |
2:11 | |
| |
| Exact & Inexact Differential |
2:12 | |
| |
Where Does (∆U = Q - W) or dU = dQ - dU Come from? |
8:54 | |
| |
| Cyclic Integrals of Path and State Functions |
8:55 | |
| |
| Our Empirical Experience of the First Law |
12:31 | |
| |
| ∆U = Q - W |
18:42 | |
| |
Relations between Changes in Properties and Energy |
22:24 | |
| |
| Relations between Changes in Properties and Energy |
22:25 | |
| |
| Rate of Change of Energy per Unit Change in Temperature |
29:54 | |
| |
| Rate of Change of Energy per Unit Change in Volume at Constant Temperature |
32:39 | |
| |
| Total Differential Equation |
34:38 | |
| |
Constant Volume |
41:08 | |
| |
| If Volume Remains Constant, then dV = 0 |
41:09 | |
| |
| Constant Volume Heat Capacity |
45:22 | |
| |
| Constant Volume Integrated |
48:14 | |
| |
| Increase & Decrease in Energy of the System |
54:19 | |
| |
Example 1: ∆U and Qv |
57:43 | |
| |
Important Equations |
62:06 | |
|
Joule's Experiment |
16:50 |
| |
Intro |
0:00 | |
| |
Joule's Experiment |
0:09 | |
| |
| Joule's Experiment |
1:20 | |
| |
Interpretation of the Result |
4:42 | |
| |
| The Gas Expands Against No External Pressure |
4:43 | |
| |
| Temperature of the Surrounding Does Not Change |
6:20 | |
| |
| System & Surrounding |
7:04 | |
| |
| Joule's Law |
10:44 | |
| |
| More on Joule's Experiment |
11:08 | |
| |
| Later Experiment |
12:38 | |
| |
| Dealing with the 2nd Law & Its Mathematical Consequences |
13:52 | |
|
Changes in Energy & State: Constant Pressure |
43:40 |
| |
Intro |
0:00 | |
| |
Changes in Energy & State: Constant Pressure |
0:20 | |
| |
| Integrating with Constant Pressure |
0:35 | |
| |
| Defining the New State Function |
6:24 | |
| |
| Heat & Enthalpy of the System at Constant Pressure |
8:54 | |
| |
| Finding ∆U |
12:10 | |
| |
| dH |
15:28 | |
| |
| Constant Pressure Heat Capacity |
18:08 | |
| |
Important Equations |
25:44 | |
| |
| Important Equations |
25:45 | |
| |
| Important Equations at Constant Pressure |
27:32 | |
| |
Example I: Change in Enthalpy (∆H) |
28:53 | |
| |
Example II: Change in Internal Energy (∆U) |
34:19 | |
|
The Relationship Between Cp & Cv |
32:23 |
| |
Intro |
0:00 | |
| |
The Relationship Between Cp & Cv |
0:21 | |
| |
| For a Constant Volume Process No Work is Done |
0:22 | |
| |
| For a Constant Pressure Process ∆V ≠ 0, so Work is Done |
1:16 | |
| |
| The Relationship Between Cp & Cv: For an Ideal Gas |
3:26 | |
| |
| The Relationship Between Cp & Cv: In Terms of Molar heat Capacities |
5:44 | |
| |
| Heat Capacity Can Have an Infinite # of Values |
7:14 | |
| |
| The Relationship Between Cp & Cv |
11:20 | |
| |
When Cp is Greater than Cv |
17:13 | |
| |
| 2nd Term |
18:10 | |
| |
| 1st Term |
19:20 | |
| |
Constant P Process: 3 Parts |
22:36 | |
| |
| Part 1 |
23:45 | |
| |
| Part 2 |
24:10 | |
| |
| Part 3 |
24:46 | |
| |
Define : γ = (Cp/Cv) |
28:06 | |
| |
| For Gases |
28:36 | |
| |
| For Liquids |
29:04 | |
| |
| For an Ideal Gas |
30:46 | |
|
The Joule Thompson Experiment |
39:15 |
| |
Intro |
0:00 | |
| |
General Equations |
0:13 | |
| |
| Recall |
0:14 | |
| |
| How Does Enthalpy of a System Change Upon a Unit Change in Pressure? |
2:58 | |
| |
| For Liquids & Solids |
12:11 | |
| |
| For Ideal Gases |
14:08 | |
| |
| For Real Gases |
16:58 | |
| |
The Joule Thompson Experiment |
18:37 | |
| |
| The Joule Thompson Experiment Setup |
18:38 | |
| |
| The Flow in 2 Stages |
22:54 | |
| |
| Work Equation for the Joule Thompson Experiment |
24:14 | |
| |
| Insulated Pipe |
26:33 | |
| |
| Joule-Thompson Coefficient |
29:50 | |
| |
| Changing Temperature & Pressure in Such a Way that Enthalpy Remains Constant |
31:44 | |
| |
Joule Thompson Inversion Temperature |
36:26 | |
| |
| Positive & Negative Joule-Thompson Coefficient |
36:27 | |
| |
| Joule Thompson Inversion Temperature |
37:22 | |
| |
| Inversion Temperature of Hydrogen Gas |
37:59 | |
|
Adiabatic Changes of State |
35:52 |
| |
Intro |
0:00 | |
| |
Adiabatic Changes of State |
0:10 | |
| |
| Adiabatic Changes of State |
0:18 | |
| |
| Work & Energy in an Adiabatic Process |
3:44 | |
| |
| Pressure-Volume Work |
7:43 | |
| |
Adiabatic Changes for an Ideal Gas |
9:23 | |
| |
| Adiabatic Changes for an Ideal Gas |
9:24 | |
| |
| Equation for a Fixed Change in Volume |
11:20 | |
| |
| Maximum & Minimum Values of Temperature |
14:20 | |
| |
Adiabatic Path |
18:08 | |
| |
| Adiabatic Path Diagram |
18:09 | |
| |
| Reversible Adiabatic Expansion |
21:54 | |
| |
| Reversible Adiabatic Compression |
22:34 | |
| |
| Fundamental Relationship Equation for an Ideal Gas Under Adiabatic Expansion |
25:00 | |
| |
| More on the Equation |
28:20 | |
| |
Important Equations |
32:16 | |
| |
| Important Adiabatic Equation |
32:17 | |
| |
| Reversible Adiabatic Change of State Equation |
33:02 | |
Section 3: Energy Example Problems |
|
1st Law Example Problems I |
42:40 |
| |
Intro |
0:00 | |
| |
Fundamental Equations |
0:56 | |
| |
| Work |
2:40 | |
| |
| Energy (1st Law) |
3:10 | |
| |
| Definition of Enthalpy |
3:44 | |
| |
| Heat capacity Definitions |
4:06 | |
| |
| The Mathematics |
6:35 | |
| |
Fundamental Concepts |
8:13 | |
| |
| Isothermal |
8:20 | |
| |
| Adiabatic |
8:54 | |
| |
| Isobaric |
9:25 | |
| |
| Isometric |
9:48 | |
| |
| Ideal Gases |
10:14 | |
| |
Example I |
12:08 | |
| |
| Example I: Conventions |
12:44 | |
| |
| Example I: Part A |
15:30 | |
| |
| Example I: Part B |
18:24 | |
| |
| Example I: Part C |
19:53 | |
| |
Example II: What is the Heat Capacity of the System? |
21:49 | |
| |
Example III: Find Q, W, ∆U & ∆H for this Change of State |
24:15 | |
| |
Example IV: Find Q, W, ∆U & ∆H |
31:37 | |
| |
Example V: Find Q, W, ∆U & ∆H |
38:20 | |
|
1st Law Example Problems II |
1:00:23 |
| |
Intro |
0:00 | |
| |
Example I |
0:11 | |
| |
| Example I: Finding ∆U |
1:49 | |
| |
| Example I: Finding W |
6:22 | |
| |
| Example I: Finding Q |
11:23 | |
| |
| Example I: Finding ∆H |
16:09 | |
| |
| Example I: Summary |
17:07 | |
| |
Example II |
21:16 | |
| |
| Example II: Finding W |
22:42 | |
| |
| Example II: Finding ∆H |
27:48 | |
| |
| Example II: Finding Q |
30:58 | |
| |
| Example II: Finding ∆U |
31:30 | |
| |
Example III |
33:33 | |
| |
| Example III: Finding ∆U, Q & W |
33:34 | |
| |
| Example III: Finding ∆H |
38:07 | |
| |
Example IV |
41:50 | |
| |
| Example IV: Finding ∆U |
41:51 | |
| |
| Example IV: Finding ∆H |
45:42 | |
| |
Example V |
49:31 | |
| |
| Example V: Finding W |
49:32 | |
| |
| Example V: Finding ∆U |
55:26 | |
| |
| Example V: Finding Q |
56:26 | |
| |
| Example V: Finding ∆H |
56:55 | |
|
1st Law Example Problems III |
44:34 |
| |
Intro |
0:00 | |
| |
Example I |
0:15 | |
| |
| Example I: Finding the Final Temperature |
3:40 | |
| |
| Example I: Finding Q |
8:04 | |
| |
| Example I: Finding ∆U |
8:25 | |
| |
| Example I: Finding W |
9:08 | |
| |
| Example I: Finding ∆H |
9:51 | |
| |
Example II |
11:27 | |
| |
| Example II: Finding the Final Temperature |
11:28 | |
| |
| Example II: Finding ∆U |
21:25 | |
| |
| Example II: Finding W & Q |
22:14 | |
| |
| Example II: Finding ∆H |
23:03 | |
| |
Example III |
24:38 | |
| |
| Example III: Finding the Final Temperature |
24:39 | |
| |
| Example III: Finding W, ∆U, and Q |
27:43 | |
| |
| Example III: Finding ∆H |
28:04 | |
| |
Example IV |
29:23 | |
| |
| Example IV: Finding ∆U, W, and Q |
25:36 | |
| |
| Example IV: Finding ∆H |
31:33 | |
| |
Example V |
32:24 | |
| |
| Example V: Finding the Final Temperature |
33:32 | |
| |
| Example V: Finding ∆U |
39:31 | |
| |
| Example V: Finding W |
40:17 | |
| |
| Example V: First Way of Finding ∆H |
41:10 | |
| |
| Example V: Second Way of Finding ∆H |
42:10 | |
|
Thermochemistry Example Problems |
59:07 |
| |
Intro |
0:00 | |
| |
Example I: Find ∆H° for the Following Reaction |
0:42 | |
| |
Example II: Calculate the ∆U° for the Reaction in Example I |
5:33 | |
| |
Example III: Calculate the Heat of Formation of NH₃ at 298 K |
14:23 | |
| |
Example IV |
32:15 | |
| |
| Part A: Calculate the Heat of Vaporization of Water at 25°C |
33:49 | |
| |
| Part B: Calculate the Work Done in Vaporizing 2 Mols of Water at 25°C Under a Constant Pressure of 1 atm |
35:26 | |
| |
| Part C: Find ∆U for the Vaporization of Water at 25°C |
41:00 | |
| |
| Part D: Find the Enthalpy of Vaporization of Water at 100°C |
43:12 | |
| |
Example V |
49:24 | |
| |
| Part A: Constant Temperature & Increasing Pressure |
50:25 | |
| |
| Part B: Increasing temperature & Constant Pressure |
56:20 | |
Section 4: Entropy |
|
Entropy |
49:16 |
| |
Intro |
0:00 | |
| |
Entropy, Part 1 |
0:16 | |
| |
| Coefficient of Thermal Expansion (Isobaric) |
0:38 | |
| |
| Coefficient of Compressibility (Isothermal) |
1:25 | |
| |
| Relative Increase & Relative Decrease |
2:16 | |
| |
| More on α |
4:40 | |
| |
| More on κ |
8:38 | |
| |
Entropy, Part 2 |
11:04 | |
| |
| Definition of Entropy |
12:54 | |
| |
| Differential Change in Entropy & the Reversible Path |
20:08 | |
| |
| State Property of the System |
28:26 | |
| |
| Entropy Changes Under Isothermal Conditions |
35:00 | |
| |
| Recall: Heating Curve |
41:05 | |
| |
| Some Phase Changes Take Place Under Constant Pressure |
44:07 | |
| |
Example I: Finding ∆S for a Phase Change |
46:05 | |
|
Math Lesson II |
33:59 |
| |
Intro |
0:00 | |
| |
Math Lesson II |
0:46 | |
| |
| Let F(x,y) = x²y³ |
0:47 | |
| |
| Total Differential |
3:34 | |
| |
| Total Differential Expression |
6:06 | |
| |
| Example 1 |
9:24 | |
| |
More on Math Expression |
13:26 | |
| |
| Exact Total Differential Expression |
13:27 | |
| |
| Exact Differentials |
19:50 | |
| |
| Inexact Differentials |
20:20 | |
| |
The Cyclic Rule |
21:06 | |
| |
| The Cyclic Rule |
21:07 | |
| |
| Example 2 |
27:58 | |
|
Entropy As a Function of Temperature & Volume |
54:37 |
| |
Intro |
0:00 | |
| |
Entropy As a Function of Temperature & Volume |
0:14 | |
| |
| Fundamental Equation of Thermodynamics |
1:16 | |
| |
| Things to Notice |
9:10 | |
| |
| Entropy As a Function of Temperature & Volume |
14:47 | |
| |
| Temperature-dependence of Entropy |
24:00 | |
| |
Example I |
26:19 | |
| |
Entropy As a Function of Temperature & Volume, Cont. |
31:55 | |
| |
| Volume-dependence of Entropy at Constant Temperature |
31:56 | |
| |
| Differentiate with Respect to Temperature, Holding Volume Constant |
36:16 | |
| |
| Recall the Cyclic Rule |
45:15 | |
| |
Summary & Recap |
46:47 | |
| |
| Fundamental Equation of Thermodynamics |
46:48 | |
| |
| For Entropy as a Function of Temperature & Volume |
47:18 | |
| |
| The Volume-dependence of Entropy for Liquids & Solids |
52:52 | |
|
Entropy as a Function of Temperature & Pressure |
31:18 |
| |
Intro |
0:00 | |
| |
Entropy as a Function of Temperature & Pressure |
0:17 | |
| |
| Entropy as a Function of Temperature & Pressure |
0:18 | |
| |
| Rewrite the Total Differential |
5:54 | |
| |
| Temperature-dependence |
7:08 | |
| |
| Pressure-dependence |
9:04 | |
| |
| Differentiate with Respect to Pressure & Holding Temperature Constant |
9:54 | |
| |
| Differentiate with Respect to Temperature & Holding Pressure Constant |
11:28 | |
| |
Pressure-Dependence of Entropy for Liquids & Solids |
18:45 | |
| |
| Pressure-Dependence of Entropy for Liquids & Solids |
18:46 | |
| |
Example I: ∆S of Transformation |
26:20 | |
|
Summary of Entropy So Far |
23:06 |
| |
Intro |
0:00 | |
| |
Summary of Entropy So Far |
0:43 | |
| |
| Defining dS |
1:04 | |
| |
| Fundamental Equation of Thermodynamics |
3:51 | |
| |
| Temperature & Volume |
6:04 | |
| |
| Temperature & Pressure |
9:10 | |
| |
| Two Important Equations for How Entropy Behaves |
13:38 | |
| |
| State of a System & Heat Capacity |
15:34 | |
| |
| Temperature-dependence of Entropy |
19:49 | |
|
Entropy Changes for an Ideal Gas |
25:42 |
| |
Intro |
0:00 | |
| |
Entropy Changes for an Ideal Gas |
1:10 | |
| |
| General Equation |
1:22 | |
| |
| The Fundamental Theorem of Thermodynamics |
2:37 | |
| |
| Recall the Basic Total Differential Expression for S = S (T,V) |
5:36 | |
| |
| For a Finite Change in State |
7:58 | |
| |
| If Cv is Constant Over the Particular Temperature Range |
9:05 | |
| |
Change in Entropy of an Ideal Gas as a Function of Temperature & Pressure |
11:35 | |
| |
| Change in Entropy of an Ideal Gas as a Function of Temperature & Pressure |
11:36 | |
| |
| Recall the Basic Total Differential expression for S = S (T, P) |
15:13 | |
| |
| For a Finite Change |
18:06 | |
| |
Example 1: Calculate the ∆S of Transformation |
22:02 | |
Section 5: Entropy Example Problems |
|
Entropy Example Problems I |
43:39 |
| |
Intro |
0:00 | |
| |
Entropy Example Problems I |
0:24 | |
| |
| Fundamental Equation of Thermodynamics |
1:10 | |
| |
| Entropy as a Function of Temperature & Volume |
2:04 | |
| |
| Entropy as a Function of Temperature & Pressure |
2:59 | |
| |
| Entropy For Phase Changes |
4:47 | |
| |
| Entropy For an Ideal Gas |
6:14 | |
| |
| Third Law Entropies |
8:25 | |
| |
| Statement of the Third Law |
9:17 | |
| |
| Entropy of the Liquid State of a Substance Above Its Melting Point |
10:23 | |
| |
| Entropy For the Gas Above Its Boiling Temperature |
13:02 | |
| |
| Entropy Changes in Chemical Reactions |
15:26 | |
| |
| Entropy Change at a Temperature Other than 25°C |
16:32 | |
| |
Example I |
19:31 | |
| |
| Part A: Calculate ∆S for the Transformation Under Constant Volume |
20:34 | |
| |
| Part B: Calculate ∆S for the Transformation Under Constant Pressure |
25:04 | |
| |
Example II: Calculate ∆S fir the Transformation Under Isobaric Conditions |
27:53 | |
| |
Example III |
30:14 | |
| |
| Part A: Calculate ∆S if 1 Mol of Aluminum is taken from 25°C to 255°C |
31:14 | |
| |
| Part B: If S°₂₉₈ = 28.4 J/mol-K, Calculate S° for Aluminum at 498 K |
33:23 | |
| |
Example IV: Calculate Entropy Change of Vaporization for CCl₄ |
34:19 | |
| |
Example V |
35:41 | |
| |
| Part A: Calculate ∆S of Transformation |
37:36 | |
| |
| Part B: Calculate ∆S of Transformation |
39:10 | |
|
Entropy Example Problems II |
56:44 |
| |
Intro |
0:00 | |
| |
Example I |
0:09 | |
| |
| Example I: Calculate ∆U |
1:28 | |
| |
| Example I: Calculate Q |
3:29 | |
| |
| Example I: Calculate Cp |
4:54 | |
| |
| Example I: Calculate ∆S |
6:14 | |
| |
Example II |
7:13 | |
| |
| Example II: Calculate W |
8:14 | |
| |
| Example II: Calculate ∆U |
8:56 | |
| |
| Example II: Calculate Q |
10:18 | |
| |
| Example II: Calculate ∆H |
11:00 | |
| |
| Example II: Calculate ∆S |
12:36 | |
| |
Example III |
18:47 | |
| |
| Example III: Calculate ∆H |
19:38 | |
| |
| Example III: Calculate Q |
21:14 | |
| |
| Example III: Calculate ∆U |
21:44 | |
| |
| Example III: Calculate W |
23:59 | |
| |
| Example III: Calculate ∆S |
24:55 | |
| |
Example IV |
27:57 | |
| |
| Example IV: Diagram |
29:32 | |
| |
| Example IV: Calculate W |
32:27 | |
| |
| Example IV: Calculate ∆U |
36:36 | |
| |
| Example IV: Calculate Q |
38:32 | |
| |
| Example IV: Calculate ∆H |
39:00 | |
| |
| Example IV: Calculate ∆S |
40:27 | |
| |
| Example IV: Summary |
43:41 | |
| |
Example V |
48:25 | |
| |
| Example V: Diagram |
49:05 | |
| |
| Example V: Calculate W |
50:58 | |
| |
| Example V: Calculate ∆U |
53:29 | |
| |
| Example V: Calculate Q |
53:44 | |
| |
| Example V: Calculate ∆H |
54:34 | |
| |
| Example V: Calculate ∆S |
55:01 | |
|
Entropy Example Problems III |
57:06 |
| |
Intro |
0:00 | |
| |
Example I: Isothermal Expansion |
0:09 | |
| |
| Example I: Calculate W |
1:19 | |
| |
| Example I: Calculate ∆U |
1:48 | |
| |
| Example I: Calculate Q |
2:06 | |
| |
| Example I: Calculate ∆H |
2:26 | |
| |
| Example I: Calculate ∆S |
3:02 | |
| |
Example II: Adiabatic and Reversible Expansion |
6:10 | |
| |
| Example II: Calculate Q |
6:48 | |
| |
| Example II: Basic Equation for the Reversible Adiabatic Expansion of an Ideal Gas |
8:12 | |
| |
| Example II: Finding Volume |
12:40 | |
| |
| Example II: Finding Temperature |
17:58 | |
| |
| Example II: Calculate ∆U |
19:53 | |
| |
| Example II: Calculate W |
20:59 | |
| |
| Example II: Calculate ∆H |
21:42 | |
| |
| Example II: Calculate ∆S |
23:42 | |
| |
Example III: Calculate the Entropy of Water Vapor |
25:20 | |
| |
Example IV: Calculate the Molar ∆S for the Transformation |
34:32 | |
| |
Example V |
44:19 | |
| |
| Part A: Calculate the Standard Entropy of Liquid Lead at 525°C |
46:17 | |
| |
| Part B: Calculate ∆H for the Transformation of Solid Lead from 25°C to Liquid Lead at 525°C |
52:23 | |
Section 6: Entropy and Probability |
|
Entropy & Probability I |
54:35 |
| |
Intro |
0:00 | |
| |
Entropy & Probability |
0:11 | |
| |
| Structural Model |
3:05 | |
| |
| Recall the Fundamental Equation of Thermodynamics |
9:11 | |
| |
| Two Independent Ways of Affecting the Entropy of a System |
10:05 | |
| |
| Boltzmann Definition |
12:10 | |
| |
Omega |
16:24 | |
| |
| Definition of Omega |
16:25 | |
| |
Energy Distribution |
19:43 | |
| |
| The Energy Distribution |
19:44 | |
| |
| In How Many Ways can N Particles be Distributed According to the Energy Distribution |
23:05 | |
| |
Example I: In How Many Ways can the Following Distribution be Achieved |
32:51 | |
| |
Example II: In How Many Ways can the Following Distribution be Achieved |
33:51 | |
| |
Example III: In How Many Ways can the Following Distribution be Achieved |
34:45 | |
| |
Example IV: In How Many Ways can the Following Distribution be Achieved |
38:50 | |
| |
Entropy & Probability, cont. |
40:57 | |
| |
| More on Distribution |
40:58 | |
| |
| Example I Summary |
41:43 | |
| |
| Example II Summary |
42:12 | |
| |
| Distribution that Maximizes Omega |
42:26 | |
| |
| If Omega is Large, then S is Large |
44:22 | |
| |
| Two Constraints for a System to Achieve the Highest Entropy Possible |
47:07 | |
| |
| What Happened When the Energy of a System is Increased? |
49:00 | |
|
Entropy & Probability II |
35:05 |
| |
Intro |
0:00 | |
| |
Volume Distribution |
0:08 | |
| |
| Distributing 2 Balls in 3 Spaces |
1:43 | |
| |
| Distributing 2 Balls in 4 Spaces |
3:44 | |
| |
| Distributing 3 Balls in 10 Spaces |
5:30 | |
| |
| Number of Ways to Distribute P Particles over N Spaces |
6:05 | |
| |
| When N is Much Larger than the Number of Particles P |
7:56 | |
| |
| Energy Distribution |
25:04 | |
| |
| Volume Distribution |
25:58 | |
| |
Entropy, Total Entropy, & Total Omega Equations |
27:34 | |
| |
| Entropy, Total Entropy, & Total Omega Equations |
27:35 | |
Section 7: Spontaneity, Equilibrium, and the Fundamental Equations |
|
Spontaneity & Equilibrium I |
28:42 |
| |
Intro |
0:00 | |
| |
Reversible & Irreversible |
0:24 | |
| |
| Reversible vs. Irreversible |
0:58 | |
| |
| Defining Equation for Equilibrium |
2:11 | |
| |
| Defining Equation for Irreversibility (Spontaneity) |
3:11 | |
| |
| TdS ≥ dQ |
5:15 | |
| |
Transformation in an Isolated System |
11:22 | |
| |
| Transformation in an Isolated System |
11:29 | |
| |
Transformation at Constant Temperature |
14:50 | |
| |
| Transformation at Constant Temperature |
14:51 | |
| |
Helmholtz Free Energy |
17:26 | |
| |
| Define: A = U - TS |
17:27 | |
| |
| Spontaneous Isothermal Process & Helmholtz Energy |
20:20 | |
| |
| Pressure-volume Work |
22:02 | |
|
Spontaneity & Equilibrium II |
34:38 |
| |
Intro |
0:00 | |
| |
Transformation under Constant Temperature & Pressure |
0:08 | |
| |
| Transformation under Constant Temperature & Pressure |
0:36 | |
| |
| Define: G = U + PV - TS |
3:32 | |
| |
| Gibbs Energy |
5:14 | |
| |
| What Does This Say? |
6:44 | |
| |
| Spontaneous Process & a Decrease in G |
14:12 | |
| |
| Computing ∆G |
18:54 | |
| |
Summary of Conditions |
21:32 | |
| |
| Constraint & Condition for Spontaneity |
21:36 | |
| |
| Constraint & Condition for Equilibrium |
24:54 | |
| |
A Few Words About the Word Spontaneous |
26:24 | |
| |
| Spontaneous Does Not Mean Fast |
26:25 | |
| |
| Putting Hydrogen & Oxygen Together in a Flask |
26:59 | |
| |
| Spontaneous Vs. Not Spontaneous |
28:14 | |
| |
| Thermodynamically Favorable |
29:03 | |
| |
| Example: Making a Process Thermodynamically Favorable |
29:34 | |
| |
Driving Forces for Spontaneity |
31:35 | |
| |
| Equation: ∆G = ∆H - T∆S |
31:36 | |
| |
| Always Spontaneous Process |
32:39 | |
| |
| Never Spontaneous Process |
33:06 | |
| |
| A Process That is Endothermic Can Still be Spontaneous |
34:00 | |
|
The Fundamental Equations of Thermodynamics |
30:50 |
| |
Intro |
0:00 | |
| |
The Fundamental Equations of Thermodynamics |
0:44 | |
| |
| Mechanical Properties of a System |
0:45 | |
| |
| Fundamental Properties of a System |
1:16 | |
| |
| Composite Properties of a System |
1:44 | |
| |
| General Condition of Equilibrium |
3:16 | |
| |
| Composite Functions & Their Differentiations |
6:11 | |
| |
| dH = TdS + VdP |
7:53 | |
| |
| dA = -SdT - PdV |
9:26 | |
| |
| dG = -SdT + VdP |
10:22 | |
| |
Summary of Equations |
12:10 | |
| |
| Equation #1 |
14:33 | |
| |
| Equation #2 |
15:15 | |
| |
| Equation #3 |
15:58 | |
| |
| Equation #4 |
16:42 | |
| |
Maxwell's Relations |
20:20 | |
| |
| Maxwell's Relations |
20:21 | |
| |
| Isothermal Volume-Dependence of Entropy & Isothermal Pressure-Dependence of Entropy |
26:21 | |
|
The General Thermodynamic Equations of State |
34:06 |
| |
Intro |
0:00 | |
| |
The General Thermodynamic Equations of State |
0:10 | |
| |
| Equations of State for Liquids & Solids |
0:52 | |
| |
| More General Condition for Equilibrium |
4:02 | |
| |
| General Conditions: Equation that Relates P to Functions of T & V |
6:20 | |
| |
| The Second Fundamental Equation of Thermodynamics |
11:10 | |
| |
| Equation 1 |
17:34 | |
| |
| Equation 2 |
21:58 | |
| |
| Recall the General Expression for Cp - Cv |
28:11 | |
| |
| For the Joule-Thomson Coefficient |
30:44 | |
| |
| Joule-Thomson Inversion Temperature |
32:12 | |
|
Properties of the Helmholtz & Gibbs Energies |
39:18 |
| |
Intro |
0:00 | |
| |
Properties of the Helmholtz & Gibbs Energies |
0:10 | |
| |
| Equating the Differential Coefficients |
1:34 | |
| |
| An Increase in T; a Decrease in A |
3:25 | |
| |
| An Increase in V; a Decrease in A |
6:04 | |
| |
| We Do the Same Thing for G |
8:33 | |
| |
| Increase in T; Decrease in G |
10:50 | |
| |
| Increase in P; Decrease in G |
11:36 | |
| |
| Gibbs Energy of a Pure Substance at a Constant Temperature from 1 atm to any Other Pressure. |
14:12 | |
| |
| If the Substance is a Liquid or a Solid, then Volume can be Treated as a Constant |
18:57 | |
| |
| For an Ideal Gas |
22:18 | |
| |
| Special Note |
24:56 | |
| |
Temperature Dependence of Gibbs Energy |
27:02 | |
| |
| Temperature Dependence of Gibbs Energy #1 |
27:52 | |
| |
| Temperature Dependence of Gibbs Energy #2 |
29:01 | |
| |
| Temperature Dependence of Gibbs Energy #3 |
29:50 | |
| |
| Temperature Dependence of Gibbs Energy #4 |
34:50 | |
|
The Entropy of the Universe & the Surroundings |
19:40 |
| |
Intro |
0:00 | |
| |
Entropy of the Universe & the Surroundings |
0:08 | |
| |
| Equation: ∆G = ∆H - T∆S |
0:20 | |
| |
| Conditions of Constant Temperature & Pressure |
1:14 | |
| |
| Reversible Process |
3:14 | |
| |
| Spontaneous Process & the Entropy of the Universe |
5:20 | |
| |
| Tips for Remembering Everything |
12:40 | |
| |
| Verify Using Known Spontaneous Process |
14:51 | |
Section 8: Free Energy Example Problems |
|
Free Energy Example Problems I |
54:16 |
| |
Intro |
0:00 | |
| |
Example I |
0:11 | |
| |
| Example I: Deriving a Function for Entropy (S) |
2:06 | |
| |
| Example I: Deriving a Function for V |
5:55 | |
| |
| Example I: Deriving a Function for H |
8:06 | |
| |
| Example I: Deriving a Function for U |
12:06 | |
| |
Example II |
15:18 | |
| |
Example III |
21:52 | |
| |
Example IV |
26:12 | |
| |
| Example IV: Part A |
26:55 | |
| |
| Example IV: Part B |
28:30 | |
| |
| Example IV: Part C |
30:25 | |
| |
Example V |
33:45 | |
| |
Example VI |
40:46 | |
| |
Example VII |
43:43 | |
| |
| Example VII: Part A |
44:46 | |
| |
| Example VII: Part B |
50:52 | |
| |
| Example VII: Part C |
51:56 | |
|
Free Energy Example Problems II |
31:17 |
| |
Intro |
0:00 | |
| |
Example I |
0:09 | |
| |
Example II |
5:18 | |
| |
Example III |
8:22 | |
| |
Example IV |
12:32 | |
| |
Example V |
17:14 | |
| |
Example VI |
20:34 | |
| |
| Example VI: Part A |
21:04 | |
| |
| Example VI: Part B |
23:56 | |
| |
| Example VI: Part C |
27:56 | |
|
Free Energy Example Problems III |
45:00 |
| |
Intro |
0:00 | |
| |
Example I |
0:10 | |
| |
Example II |
15:03 | |
| |
Example III |
21:47 | |
| |
Example IV |
28:37 | |
| |
| Example IV: Part A |
29:33 | |
| |
| Example IV: Part B |
36:09 | |
| |
| Example IV: Part C |
40:34 | |
|
Three Miscellaneous Example Problems |
58:05 |
| |
Intro |
0:00 | |
| |
Example I |
0:41 | |
| |
| Part A: Calculating ∆H |
3:55 | |
| |
| Part B: Calculating ∆S |
15:13 | |
| |
Example II |
24:39 | |
| |
| Part A: Final Temperature of the System |
26:25 | |
| |
| Part B: Calculating ∆S |
36:57 | |
| |
Example III |
46:49 | |
Section 9: Equation Review for Thermodynamics |
|
Looking Back Over Everything: All the Equations in One Place |
25:20 |
| |
Intro |
0:00 | |
| |
Work, Heat, and Energy |
0:18 | |
| |
| Definition of Work, Energy, Enthalpy, and Heat Capacities |
0:23 | |
| |
| Heat Capacities for an Ideal Gas |
3:40 | |
| |
| Path Property & State Property |
3:56 | |
| |
| Energy Differential |
5:04 | |
| |
| Enthalpy Differential |
5:40 | |
| |
| Joule's Law & Joule-Thomson Coefficient |
6:23 | |
| |
| Coefficient of Thermal Expansion & Coefficient of Compressibility |
7:01 | |
| |
| Enthalpy of a Substance at Any Other Temperature |
7:29 | |
| |
| Enthalpy of a Reaction at Any Other Temperature |
8:01 | |
| |
Entropy |
8:53 | |
| |
| Definition of Entropy |
8:54 | |
| |
| Clausius Inequality |
9:11 | |
| |
| Entropy Changes in Isothermal Systems |
9:44 | |
| |
| The Fundamental Equation of Thermodynamics |
10:12 | |
| |
| Expressing Entropy Changes in Terms of Properties of the System |
10:42 | |
| |
| Entropy Changes in the Ideal Gas |
11:22 | |
| |
| Third Law Entropies |
11:38 | |
| |
| Entropy Changes in Chemical Reactions |
14:02 | |
| |
| Statistical Definition of Entropy |
14:34 | |
| |
| Omega for the Spatial & Energy Distribution |
14:47 | |
| |
Spontaneity and Equilibrium |
15:43 | |
| |
| Helmholtz Energy & Gibbs Energy |
15:44 | |
| |
| Condition for Spontaneity & Equilibrium |
16:24 | |
| |
| Condition for Spontaneity with Respect to Entropy |
17:58 | |
| |
| The Fundamental Equations |
18:30 | |
| |
| Maxwell's Relations |
19:04 | |
| |
| The Thermodynamic Equations of State |
20:07 | |
| |
| Energy & Enthalpy Differentials |
21:08 | |
| |
| Joule's Law & Joule-Thomson Coefficient |
21:59 | |
| |
| Relationship Between Constant Pressure & Constant Volume Heat Capacities |
23:14 | |
| |
| One Final Equation - Just for Fun |
24:04 | |
Section 10: Quantum Mechanics Preliminaries |
|
Complex Numbers |
34:25 |
| |
Intro |
0:00 | |
| |
Complex Numbers |
0:11 | |
| |
| Representing Complex Numbers in the 2-Dimmensional Plane |
0:56 | |
| |
| Addition of Complex Numbers |
2:35 | |
| |
| Subtraction of Complex Numbers |
3:17 | |
| |
| Multiplication of Complex Numbers |
3:47 | |
| |
| Division of Complex Numbers |
6:04 | |
| |
| r & θ |
8:04 | |
| |
| Euler's Formula |
11:00 | |
| |
| Polar Exponential Representation of the Complex Numbers |
11:22 | |
| |
Example I |
14:25 | |
| |
Example II |
15:21 | |
| |
Example III |
16:58 | |
| |
Example IV |
18:35 | |
| |
Example V |
20:40 | |
| |
Example VI |
21:32 | |
| |
Example VII |
25:22 | |
|
Probability & Statistics |
59:57 |
| |
Intro |
0:00 | |
| |
Probability & Statistics |
1:51 | |
| |
| Normalization Condition |
1:52 | |
| |
| Define the Mean or Average of x |
11:04 | |
| |
Example I: Calculate the Mean of x |
14:57 | |
| |
Example II: Calculate the Second Moment of the Data in Example I |
22:39 | |
| |
Define the Second Central Moment or Variance |
25:26 | |
| |
| Define the Second Central Moment or Variance |
25:27 | |
| |
| 1st Term |
32:16 | |
| |
| 2nd Term |
32:40 | |
| |
| 3rd Term |
34:07 | |
| |
Continuous Distributions |
35:47 | |
| |
| Continuous Distributions |
35:48 | |
| |
Probability Density |
39:30 | |
| |
| Probability Density |
39:31 | |
| |
| Normalization Condition |
46:51 | |
| |
Example III |
50:13 | |
| |
| Part A - Show that P(x) is Normalized |
51:40 | |
| |
| Part B - Calculate the Average Position of the Particle Along the Interval |
54:31 | |
| |
Important Things to Remember |
58:24 | |
|
Schrӧdinger Equation & Operators |
42:05 |
| |
Intro |
0:00 | |
| |
Schrӧdinger Equation & Operators |
0:16 | |
| |
| Relation Between a Photon's Momentum & Its Wavelength |
0:17 | |
| |
| Louis de Broglie: Wavelength for Matter |
0:39 | |
| |
| Schrӧdinger Equation |
1:19 | |
| |
| Definition of Ψ(x) |
3:31 | |
| |
| Quantum Mechanics |
5:02 | |
| |
| Operators |
7:51 | |
| |
Example I |
10:10 | |
| |
Example II |
11:53 | |
| |
Example III |
14:24 | |
| |
Example IV |
17:35 | |
| |
Example V |
19:59 | |
| |
Example VI |
22:39 | |
| |
Operators Can Be Linear or Non Linear |
27:58 | |
| |
| Operators Can Be Linear or Non Linear |
28:34 | |
| |
Example VII |
32:47 | |
| |
Example VIII |
36:55 | |
| |
Example IX |
39:29 | |
|
Schrӧdinger Equation as an Eigenvalue Problem |
30:26 |
| |
Intro |
0:00 | |
| |
Schrӧdinger Equation as an Eigenvalue Problem |
0:10 | |
| |
| Operator: Multiplying the Original Function by Some Scalar |
0:11 | |
| |
| Operator, Eigenfunction, & Eigenvalue |
4:42 | |
| |
| Example: Eigenvalue Problem |
8:00 | |
| |
| Schrӧdinger Equation as an Eigenvalue Problem |
9:24 | |
| |
| Hamiltonian Operator |
15:09 | |
| |
Quantum Mechanical Operators |
16:46 | |
| |
| Kinetic Energy Operator |
19:16 | |
| |
| Potential Energy Operator |
20:02 | |
| |
| Total Energy Operator |
21:12 | |
| |
| Classical Point of View |
21:48 | |
| |
| Linear Momentum Operator |
24:02 | |
| |
Example I |
26:01 | |
|
The Plausibility of the Schrӧdinger Equation |
21:34 |
| |
Intro |
0:00 | |
| |
The Plausibility of the Schrӧdinger Equation |
1:16 | |
| |
| The Plausibility of the Schrӧdinger Equation, Part 1 |
1:17 | |
| |
| The Plausibility of the Schrӧdinger Equation, Part 2 |
8:24 | |
| |
| The Plausibility of the Schrӧdinger Equation, Part 3 |
13:45 | |
Section 11: The Particle in a Box |
|
The Particle in a Box Part I |
56:22 |
| |
Intro |
0:00 | |
| |
Free Particle in a Box |
0:28 | |
| |
| Definition of a Free Particle in a Box |
0:29 | |
| |
| Amplitude of the Matter Wave |
6:22 | |
| |
| Intensity of the Wave |
6:53 | |
| |
| Probability Density |
9:39 | |
| |
| Probability that the Particle is Located Between x & dx |
10:54 | |
| |
| Probability that the Particle will be Found Between o & a |
12:35 | |
| |
| Wave Function & the Particle |
14:59 | |
| |
| Boundary Conditions |
19:22 | |
| |
| What Happened When There is No Constraint on the Particle |
27:54 | |
| |
| Diagrams |
34:12 | |
| |
| More on Probability Density |
40:53 | |
| |
The Correspondence Principle |
46:45 | |
| |
| The Correspondence Principle |
46:46 | |
| |
Normalizing the Wave Function |
47:46 | |
| |
| Normalizing the Wave Function |
47:47 | |
| |
| Normalized Wave Function & Normalization Constant |
52:24 | |
|
The Particle in a Box Part II |
45:24 |
| |
Intro |
0:00 | |
| |
Free Particle in a Box |
0:08 | |
| |
| Free Particle in a 1-dimensional Box |
0:09 | |
| |
| For a Particle in a Box |
3:57 | |
| |
Calculating Average Values & Standard Deviations |
5:42 | |
| |
| Average Value for the Position of a Particle |
6:32 | |
| |
| Standard Deviations for the Position of a Particle |
10:51 | |
| |
| Recall: Energy & Momentum are Represented by Operators |
13:33 | |
| |
| Recall: Schrӧdinger Equation in Operator Form |
15:57 | |
| |
| Average Value of a Physical Quantity that is Associated with an Operator |
18:16 | |
| |
| Average Momentum of a Free Particle in a Box |
20:48 | |
| |
The Uncertainty Principle |
24:42 | |
| |
| Finding the Standard Deviation of the Momentum |
25:08 | |
| |
| Expression for the Uncertainty Principle |
35:02 | |
| |
| Summary of the Uncertainty Principle |
41:28 | |
|
The Particle in a Box Part III |
48:43 |
| |
Intro |
0:00 | |
| |
2-Dimension |
0:12 | |
| |
| Dimension 2 |
0:31 | |
| |
| Boundary Conditions |
1:52 | |
| |
| Partial Derivatives |
4:27 | |
| |
Example I |
6:08 | |
| |
The Particle in a Box, cont. |
11:28 | |
| |
| Operator Notation |
12:04 | |
| |
| Symbol for the Laplacian |
13:50 | |
| |
| The Equation Becomes
|
14:30 | |
| |
| Boundary Conditions |
14:54 | |
| |
| Separation of Variables |
15:33 | |
| |
| Solution to the 1-dimensional Case |
16:31 | |
| |
| Normalization Constant |
22:32 | |
| |
3-Dimension |
28:30 | |
| |
| Particle in a 3-dimensional Box |
28:31 | |
| |
| In Del Notation |
32:22 | |
| |
| The Solutions |
34:51 | |
| |
| Expressing the State of the System for a Particle in a 3D Box |
39:10 | |
| |
| Energy Level & Degeneracy |
43:35 | |
Section 12: Postulates and Principles of Quantum Mechanics |
|
The Postulates & Principles of Quantum Mechanics, Part I |
46:18 |
| |
Intro |
0:00 | |
| |
Postulate I |
0:31 | |
| |
| Probability That The Particle Will Be Found in a Differential Volume Element |
0:32 | |
| |
Example I: Normalize This Wave Function |
11:30 | |
| |
Postulate II |
18:20 | |
| |
| Postulate II |
18:21 | |
| |
| Quantum Mechanical Operators: Position |
20:48 | |
| |
| Quantum Mechanical Operators: Kinetic Energy |
21:57 | |
| |
| Quantum Mechanical Operators: Potential Energy |
22:42 | |
| |
| Quantum Mechanical Operators: Total Energy |
22:57 | |
| |
| Quantum Mechanical Operators: Momentum |
23:22 | |
| |
| Quantum Mechanical Operators: Angular Momentum |
23:48 | |
| |
| More On The Kinetic Energy Operator |
24:48 | |
| |
Angular Momentum |
28:08 | |
| |
| Angular Momentum Overview |
28:09 | |
| |
| Angular Momentum Operator in Quantum Mechanic |
31:34 | |
| |
| The Classical Mechanical Observable |
32:56 | |
| |
| Quantum Mechanical Operator |
37:01 | |
| |
| Getting the Quantum Mechanical Operator from the Classical Mechanical Observable |
40:16 | |
| |
Postulate II, cont. |
43:40 | |
| |
| Quantum Mechanical Operators are Both Linear & Hermetical |
43:41 | |
|
The Postulates & Principles of Quantum Mechanics, Part II |
39:28 |
| |
Intro |
0:00 | |
| |
Postulate III |
0:09 | |
| |
| Postulate III: Part I |
0:10 | |
| |
| Postulate III: Part II |
5:56 | |
| |
| Postulate III: Part III |
12:43 | |
| |
| Postulate III: Part IV |
18:28 | |
| |
Postulate IV |
23:57 | |
| |
| Postulate IV |
23:58 | |
| |
Postulate V |
27:02 | |
| |
| Postulate V |
27:03 | |
| |
Average Value |
36:38 | |
| |
| Average Value |
36:39 | |
|
The Postulates & Principles of Quantum Mechanics, Part III |
35:32 |
| |
Intro |
0:00 | |
| |
The Postulates & Principles of Quantum Mechanics, Part III |
0:10 | |
| |
| Equations: Linear & Hermitian |
0:11 | |
| |
| Introduction to Hermitian Property |
3:36 | |
| |
| Eigenfunctions are Orthogonal |
9:55 | |
| |
| The Sequence of Wave Functions for the Particle in a Box forms an Orthonormal Set |
14:34 | |
| |
| Definition of Orthogonality |
16:42 | |
| |
| Definition of Hermiticity |
17:26 | |
| |
| Hermiticity: The Left Integral |
23:04 | |
| |
| Hermiticity: The Right Integral |
28:47 | |
| |
| Hermiticity: Summary |
34:06 | |
|
The Postulates & Principles of Quantum Mechanics, Part IV |
29:55 |
| |
Intro |
0:00 | |
| |
The Postulates & Principles of Quantum Mechanics, Part IV |
0:09 | |
| |
| Operators can be Applied Sequentially |
0:10 | |
| |
| Sample Calculation 1 |
2:41 | |
| |
| Sample Calculation 2 |
5:18 | |
| |
| Commutator of Two Operators |
8:16 | |
| |
| The Uncertainty Principle |
19:01 | |
| |
| In the Case of Linear Momentum and Position Operator |
23:14 | |
| |
| When the Commutator of Two Operators Equals to Zero |
26:31 | |
Section 13: Postulates and Principles Example Problems, Including Particle in a Box |
|
Example Problems I |
54:25 |
| |
Intro |
0:00 | |
| |
Example I: Three Dimensional Box & Eigenfunction of The Laplacian Operator |
0:37 | |
| |
Example II: Positions of a Particle in a 1-dimensional Box |
15:46 | |
| |
Example III: Transition State & Frequency |
29:29 | |
| |
Example IV: Finding a Particle in a 1-dimensional Box |
35:03 | |
| |
Example V: Degeneracy & Energy Levels of a Particle in a Box |
44:59 | |
|
Example Problems II |
46:58 |
| |
Intro |
0:00 | |
| |
Review |
0:25 | |
| |
| Wave Function |
0:26 | |
| |
| Normalization Condition |
2:28 | |
| |
| Observable in Classical Mechanics & Linear/Hermitian Operator in Quantum Mechanics |
3:36 | |
| |
| Hermitian |
6:11 | |
| |
| Eigenfunctions & Eigenvalue |
8:20 | |
| |
| Normalized Wave Functions |
12:00 | |
| |
| Average Value |
13:42 | |
| |
| If Ψ is Written as a Linear Combination |
15:44 | |
| |
| Commutator |
16:45 | |
| |
Example I: Normalize The Wave Function |
19:18 | |
| |
Example II: Probability of Finding of a Particle |
22:27 | |
| |
Example III: Orthogonal |
26:00 | |
| |
Example IV: Average Value of the Kinetic Energy Operator |
30:22 | |
| |
Example V: Evaluate These Commutators |
39:02 | |
|
Example Problems III |
44:11 |
| |
Intro |
0:00 | |
| |
Example I: Good Candidate for a Wave Function |
0:08 | |
| |
Example II: Variance of the Energy |
7:00 | |
| |
Example III: Evaluate the Angular Momentum Operators |
15:00 | |
| |
Example IV: Real Eigenvalues Imposes the Hermitian Property on Operators |
28:44 | |
| |
Example V: A Demonstration of Why the Eigenfunctions of Hermitian Operators are Orthogonal |
35:33 | |
Section 14: The Harmonic Oscillator |
|
The Harmonic Oscillator I |
35:33 |
| |
Intro |
0:00 | |
| |
The Harmonic Oscillator |
0:10 | |
| |
| Harmonic Motion |
0:11 | |
| |
| Classical Harmonic Oscillator |
4:38 | |
| |
| Hooke's Law |
8:18 | |
| |
| Classical Harmonic Oscillator, cont. |
10:33 | |
| |
| General Solution for the Differential Equation |
15:16 | |
| |
| Initial Position & Velocity |
16:05 | |
| |
| Period & Amplitude |
20:42 | |
| |
| Potential Energy of the Harmonic Oscillator |
23:20 | |
| |
| Kinetic Energy of the Harmonic Oscillator |
26:37 | |
| |
| Total Energy of the Harmonic Oscillator |
27:23 | |
| |
| Conservative System |
34:37 | |
|
The Harmonic Oscillator II |
43:04 |
| |
Intro |
0:00 | |
| |
The Harmonic Oscillator II |
0:08 | |
| |
| Diatomic Molecule |
0:10 | |
| |
| Notion of Reduced Mass |
5:27 | |
| |
| Harmonic Oscillator Potential & The Intermolecular Potential of a Vibrating Molecule |
7:33 | |
| |
| The Schrӧdinger Equation for the 1-dimensional Quantum Mechanic Oscillator |
14:14 | |
| |
| Quantized Values for the Energy Level |
15:46 | |
| |
| Ground State & the Zero-Point Energy |
21:50 | |
| |
| Vibrational Energy Levels |
25:18 | |
| |
| Transition from One Energy Level to the Next |
26:42 | |
| |
| Fundamental Vibrational Frequency for Diatomic Molecule |
34:57 | |
| |
| Example: Calculate k |
38:01 | |
|
The Harmonic Oscillator III |
26:30 |
| |
Intro |
0:00 | |
| |
The Harmonic Oscillator III |
0:09 | |
| |
| The Wave Functions Corresponding to the Energies |
0:10 | |
| |
| Normalization Constant |
2:34 | |
| |
| Hermite Polynomials |
3:22 | |
| |
| First Few Hermite Polynomials |
4:56 | |
| |
| First Few Wave-Functions |
6:37 | |
| |
| Plotting the Probability Density of the Wave-Functions |
8:37 | |
| |
| Probability Density for Large Values of r |
14:24 | |
| |
| Recall: Odd Function & Even Function |
19:05 | |
| |
| More on the Hermite Polynomials |
20:07 | |
| |
| Recall: If f(x) is Odd |
20:36 | |
| |
| Average Value of x |
22:31 | |
| |
| Average Value of Momentum |
23:56 | |
Section 15: The Rigid Rotator |
|
The Rigid Rotator I |
41:10 |
| |
Intro |
0:00 | |
| |
Possible Confusion from the Previous Discussion |
0:07 | |
| |
| Possible Confusion from the Previous Discussion |
0:08 | |
| |
Rotation of a Single Mass Around a Fixed Center |
8:17 | |
| |
| Rotation of a Single Mass Around a Fixed Center |
8:18 | |
| |
| Angular Velocity |
12:07 | |
| |
| Rotational Inertia |
13:24 | |
| |
| Rotational Frequency |
15:24 | |
| |
| Kinetic Energy for a Linear System |
16:38 | |
| |
| Kinetic Energy for a Rotational System |
17:42 | |
| |
Rotating Diatomic Molecule |
19:40 | |
| |
| Rotating Diatomic Molecule: Part 1 |
19:41 | |
| |
| Rotating Diatomic Molecule: Part 2 |
24:56 | |
| |
| Rotating Diatomic Molecule: Part 3 |
30:04 | |
| |
Hamiltonian of the Rigid Rotor |
36:48 | |
| |
| Hamiltonian of the Rigid Rotor |
36:49 | |
|
The Rigid Rotator II |
30:32 |
| |
Intro |
0:00 | |
| |
The Rigid Rotator II |
0:08 | |
| |
| Cartesian Coordinates |
0:09 | |
| |
| Spherical Coordinates |
1:55 | |
| |
| r |
6:15 | |
| |
| θ |
6:28 | |
| |
| φ |
7:00 | |
| |
| Moving a Distance 'r' |
8:17 | |
| |
| Moving a Distance 'r' in the Spherical Coordinates |
11:49 | |
| |
| For a Rigid Rotator, r is Constant |
13:57 | |
| |
| Hamiltonian Operator |
15:09 | |
| |
| Square of the Angular Momentum Operator |
17:34 | |
| |
| Orientation of the Rotation in Space |
19:44 | |
| |
| Wave Functions for the Rigid Rotator |
20:40 | |
| |
| The Schrӧdinger Equation for the Quantum Mechanic Rigid Rotator |
21:24 | |
| |
| Energy Levels for the Rigid Rotator |
26:58 | |
|
The Rigid Rotator III |
35:19 |
| |
Intro |
0:00 | |
| |
The Rigid Rotator III |
0:11 | |
| |
| When a Rotator is Subjected to Electromagnetic Radiation |
1:24 | |
| |
| Selection Rule |
2:13 | |
| |
| Frequencies at Which Absorption Transitions Occur |
6:24 | |
| |
| Energy Absorption & Transition |
10:54 | |
| |
| Energy of the Individual Levels Overview |
20:58 | |
| |
| Energy of the Individual Levels: Diagram |
23:45 | |
| |
| Frequency Required to Go from J to J + 1 |
25:53 | |
| |
| Using Separation Between Lines on the Spectrum to Calculate Bond Length |
28:02 | |
| |
Example I: Calculating Rotational Inertia & Bond Length |
29:18 | |
| |
| Example I: Calculating Rotational Inertia |
29:19 | |
| |
| Example I: Calculating Bond Length |
32:56 | |
Section 16: Oscillator and Rotator Example Problems |
|
Example Problems I |
33:48 |
| |
Intro |
0:00 | |
| |
Equations Review |
0:11 | |
| |
| Energy of the Harmonic Oscillator |
0:12 | |
| |
| Selection Rule |
3:02 | |
| |
| Observed Frequency of Radiation |
3:27 | |
| |
| Harmonic Oscillator Wave Functions |
5:52 | |
| |
| Rigid Rotator |
7:26 | |
| |
| Selection Rule for Rigid Rotator |
9:15 | |
| |
| Frequency of Absorption |
9:35 | |
| |
| Wave Numbers |
10:58 | |
| |
Example I: Calculate the Reduced Mass of the Hydrogen Atom |
11:44 | |
| |
Example II: Calculate the Fundamental Vibration Frequency & the Zero-Point Energy of This Molecule |
13:37 | |
| |
Example III: Show That the Product of Two Even Functions is even |
19:35 | |
| |
Example IV: Harmonic Oscillator |
24:56 | |
|
Example Problems II |
46:43 |
| |
Intro |
0:00 | |
| |
Example I: Harmonic Oscillator |
0:12 | |
| |
Example II: Harmonic Oscillator |
23:26 | |
| |
Example III: Calculate the RMS Displacement of the Molecules |
38:12 | |
Section 17: The Hydrogen Atom |
|
The Hydrogen Atom I |
40:00 |
| |
Intro |
0:00 | |
| |
The Hydrogen Atom I |
1:31 | |
| |
| Review of the Rigid Rotator |
1:32 | |
| |
| Hydrogen Atom & the Coulomb Potential |
2:50 | |
| |
| Using the Spherical Coordinates |
6:33 | |
| |
| Applying This Last Expression to Equation 1 |
10:19 | |
| |
| Angular Component & Radial Component |
13:26 | |
| |
| Angular Equation |
15:56 | |
| |
| Solution for F(φ) |
19:32 | |
| |
| Determine The Normalization Constant |
20:33 | |
| |
| Differential Equation for T(a) |
24:44 | |
| |
| Legendre Equation |
27:20 | |
| |
| Legendre Polynomials |
31:20 | |
| |
| The Legendre Polynomials are Mutually Orthogonal |
35:40 | |
| |
| Limits |
37:17 | |
| |
| Coefficients |
38:28 | |
|
The Hydrogen Atom II |
35:58 |
| |
Intro |
0:00 | |
| |
Associated Legendre Functions |
0:07 | |
| |
| Associated Legendre Functions |
0:08 | |
| |
| First Few Associated Legendre Functions |
6:39 | |
| |
| s, p, & d Orbital |
13:24 | |
| |
| The Normalization Condition |
15:44 | |
| |
Spherical Harmonics |
20:03 | |
| |
| Equations We Have Found |
20:04 | |
| |
| Wave Functions for the Angular Component & Rigid Rotator |
24:36 | |
| |
| Spherical Harmonics Examples |
25:40 | |
| |
Angular Momentum |
30:09 | |
| |
| Angular Momentum |
30:10 | |
| |
| Square of the Angular Momentum |
35:38 | |
| |
| Energies of the Rigid Rotator |
38:21 | |
|
The Hydrogen Atom III |
36:18 |
| |
Intro |
0:00 | |
| |
The Hydrogen Atom III |
0:34 | |
| |
| Angular Momentum is a Vector Quantity |
0:35 | |
| |
| The Operators Corresponding to the Three Components of Angular Momentum Operator: In Cartesian Coordinates |
1:30 | |
| |
| The Operators Corresponding to the Three Components of Angular Momentum Operator: In Spherical Coordinates |
3:27 | |
| |
| Z Component of the Angular Momentum Operator & the Spherical Harmonic |
5:28 | |
| |
| Magnitude of the Angular Momentum Vector |
20:10 | |
| |
| Classical Interpretation of Angular Momentum |
25:22 | |
| |
| Projection of the Angular Momentum Vector onto the xy-plane |
33:24 | |
|
The Hydrogen Atom IV |
33:55 |
| |
Intro |
0:00 | |
| |
The Hydrogen Atom IV |
0:09 | |
| |
| The Equation to Find R( r ) |
0:10 | |
| |
| Relation Between n & l |
3:50 | |
| |
| The Solutions for the Radial Functions |
5:08 | |
| |
| Associated Laguerre Polynomials |
7:58 | |
| |
| 1st Few Associated Laguerre Polynomials |
8:55 | |
| |
| Complete Wave Function for the Atomic Orbitals of the Hydrogen Atom |
12:24 | |
| |
| The Normalization Condition |
15:06 | |
| |
| In Cartesian Coordinates |
18:10 | |
| |
| Working in Polar Coordinates |
20:48 | |
| |
| Principal Quantum Number |
21:58 | |
| |
| Angular Momentum Quantum Number |
22:35 | |
| |
| Magnetic Quantum Number |
25:55 | |
| |
| Zeeman Effect |
30:45 | |
|
The Hydrogen Atom V: Where We Are |
51:53 |
| |
Intro |
0:00 | |
| |
The Hydrogen Atom V: Where We Are |
0:13 | |
| |
| Review |
0:14 | |
| |
| Let's Write Out ψ₂₁₁ |
7:32 | |
| |
| Angular Momentum of the Electron |
14:52 | |
| |
| Representation of the Wave Function |
19:36 | |
| |
| Radial Component |
28:02 | |
| |
| Example: 1s Orbital |
28:34 | |
| |
| Probability for Radial Function |
33:46 | |
| |
| 1s Orbital: Plotting Probability Densities vs. r |
35:47 | |
| |
| 2s Orbital: Plotting Probability Densities vs. r |
37:46 | |
| |
| 3s Orbital: Plotting Probability Densities vs. r |
38:49 | |
| |
| 4s Orbital: Plotting Probability Densities vs. r |
39:34 | |
| |
| 2p Orbital: Plotting Probability Densities vs. r |
40:12 | |
| |
| 3p Orbital: Plotting Probability Densities vs. r |
41:02 | |
| |
| 4p Orbital: Plotting Probability Densities vs. r |
41:51 | |
| |
| 3d Orbital: Plotting Probability Densities vs. r |
43:18 | |
| |
| 4d Orbital: Plotting Probability Densities vs. r |
43:48 | |
| |
Example I: Probability of Finding an Electron in the 2s Orbital of the Hydrogen |
45:40 | |
|
The Hydrogen Atom VI |
51:53 |
| |
Intro |
0:00 | |
| |
The Hydrogen Atom VI |
0:07 | |
| |
| Last Lesson Review |
0:08 | |
| |
| Spherical Component |
1:09 | |
| |
| Normalization Condition |
2:02 | |
| |
Complete 1s Orbital Wave Function |
4:08 | |
| |
| 1s Orbital Wave Function |
4:09 | |
| |
| Normalization Condition |
6:28 | |
| |
| Spherically Symmetric |
16:00 | |
| |
| Average Value |
17:52 | |
| |
Example I: Calculate the Region of Highest Probability for Finding the Electron |
21:19 | |
| |
2s Orbital Wave Function |
25:32 | |
| |
| 2s Orbital Wave Function |
25:33 | |
| |
| Average Value |
28:56 | |
| |
| General Formula |
32:24 | |
|
The Hydrogen Atom VII |
34:29 |
| |
Intro |
0:00 | |
| |
The Hydrogen Atom VII |
0:12 | |
| |
| p Orbitals |
1:30 | |
| |
| Not Spherically Symmetric |
5:10 | |
| |
| Recall That the Spherical Harmonics are Eigenfunctions of the Hamiltonian Operator |
6:50 | |
| |
| Any Linear Combination of These Orbitals Also Has The Same Energy |
9:16 | |
| |
| Functions of Real Variables |
15:53 | |
| |
| Solving for Px |
16:50 | |
| |
| Real Spherical Harmonics |
21:56 | |
| |
| Number of Nodes |
32:56 | |
Section 18: Hydrogen Atom Example Problems |
|
Hydrogen Atom Example Problems I |
43:49 |
| |
Intro |
0:00 | |
| |
Example I: Angular Momentum & Spherical Harmonics |
0:20 | |
| |
Example II: Pair-wise Orthogonal Legendre Polynomials |
16:40 | |
| |
Example III: General Normalization Condition for the Legendre Polynomials |
25:06 | |
| |
Example IV: Associated Legendre Functions |
32:13 | |
|
The Hydrogen Atom Example Problems II |
1:01:57 |
| |
Intro |
0:00 | |
| |
Example I: Normalization & Pair-wise Orthogonal |
0:13 | |
| |
| Part 1: Normalized |
0:43 | |
| |
| Part 2: Pair-wise Orthogonal |
16:53 | |
| |
Example II: Show Explicitly That the Following Statement is True for Any Integer n |
27:10 | |
| |
Example III: Spherical Harmonics |
29:26 | |
| |
Angular Momentum Cones |
56:37 | |
| |
| Angular Momentum Cones |
56:38 | |
| |
| Physical Interpretation of Orbital Angular Momentum in Quantum mechanics |
60:16 | |
|
The Hydrogen Atom Example Problems III |
48:33 |
| |
Intro |
0:00 | |
| |
Example I: Show That ψ₂₁₁ is Normalized |
0:07 | |
| |
Example II: Show That ψ₂₁₁ is Orthogonal to ψ₃₁₀ |
11:48 | |
| |
Example III: Probability That a 1s Electron Will Be Found Within 1 Bohr Radius of The Nucleus |
18:35 | |
| |
Example IV: Radius of a Sphere |
26:06 | |
| |
Example V: Calculate <r> for the 2s Orbital of the Hydrogen-like Atom |
36:33 | |
|
The Hydrogen Atom Example Problems IV |
48:33 |
| |
Intro |
0:00 | |
| |
Example I: Probability Density vs. Radius Plot |
0:11 | |
| |
Example II: Hydrogen Atom & The Coulombic Potential |
14:16 | |
| |
Example III: Find a Relation Among <K>, <V>, & <E> |
25:47 | |
| |
Example IV: Quantum Mechanical Virial Theorem |
48:32 | |
| |
Example V: Find the Variance for the 2s Orbital |
54:13 | |
|
The Hydrogen Atom Example Problems V |
48:33 |
| |
Intro |
0:00 | |
| |
Example I: Derive a Formula for the Degeneracy of a Given Level n |
0:11 | |
| |
Example II: Using Linear Combinations to Represent the Spherical Harmonics as Functions of the Real Variables θ & φ |
8:30 | |
| |
Example III: Using Linear Combinations to Represent the Spherical Harmonics as Functions of the Real Variables θ & φ |
23:01 | |
| |
Example IV: Orbital Functions |
31:51 | |
Section 19: Spin Quantum Number and Atomic Term Symbols |
|
Spin Quantum Number: Term Symbols I |
59:18 |
| |
Intro |
0:00 | |
| |
Quantum Numbers Specify an Orbital |
0:24 | |
| |
| n |
1:10 | |
| |
| l |
1:20 | |
| |
| m |
1:35 | |
| |
| 4th Quantum Number: s |
2:02 | |
| |
Spin Orbitals |
7:03 | |
| |
| Spin Orbitals |
7:04 | |
| |
| Multi-electron Atoms |
11:08 | |
| |
Term Symbols |
18:08 | |
| |
| Russell-Saunders Coupling & The Atomic Term Symbol |
18:09 | |
| |
Example: Configuration for C |
27:50 | |
| |
| Configuration for C: 1s²2s²2p² |
27:51 | |
| |
| Drawing Every Possible Arrangement |
31:15 | |
| |
| Term Symbols |
45:24 | |
| |
| Microstate |
50:54 | |
|
Spin Quantum Number: Term Symbols II |
34:54 |
| |
Intro |
0:00 | |
| |
Microstates |
0:25 | |
| |
| We Started With 21 Possible Microstates |
0:26 | |
| |
| ³P State |
2:05 | |
| |
| Microstates in ³P Level |
5:10 | |
| |
| ¹D State |
13:16 | |
| |
| ³P State |
16:10 | |
| |
| ²P₂ State |
17:34 | |
| |
| ³P₁ State |
18:34 | |
| |
| ³P₀ State |
19:12 | |
| |
| 9 Microstates in ³P are Subdivided |
19:40 | |
| |
| ¹S State |
21:44 | |
| |
| Quicker Way to Find the Different Values of J for a Given Basic Term Symbol |
22:22 | |
| |
| Ground State |
26:27 | |
| |
Hund's Empirical Rules for Specifying the Term Symbol for the Ground Electronic State |
27:29 | |
| |
| Hund's Empirical Rules: 1 |
28:24 | |
| |
| Hund's Empirical Rules: 2 |
29:22 | |
| |
| Hund's Empirical Rules: 3 - Part A |
30:22 | |
| |
| Hund's Empirical Rules: 3 - Part B |
31:18 | |
| |
| Example: 1s²2s²2p² |
31:54 | |
|
Spin Quantum Number: Term Symbols III |
38:03 |
| |
Intro |
0:00 | |
| |
Spin Quantum Number: Term Symbols III |
0:14 | |
| |
| Deriving the Term Symbols for the p² Configuration |
0:15 | |
| |
| Table: MS vs. ML |
3:57 | |
| |
| ¹D State |
16:21 | |
| |
| ³P State |
21:13 | |
| |
| ¹S State |
24:48 | |
| |
| J Value |
25:32 | |
| |
| Degeneracy of the Level |
27:28 | |
| |
| When Given r Electrons to Assign to n Equivalent Spin Orbitals |
30:18 | |
| |
| p² Configuration |
32:51 | |
| |
| Complementary Configurations |
35:12 | |
|
Term Symbols & Atomic Spectra |
57:49 |
| |
Intro |
0:00 | |
| |
Lyman Series |
0:09 | |
| |
| Spectroscopic Term Symbols |
0:10 | |
| |
| Lyman Series |
3:04 | |
| |
Hydrogen Levels |
8:21 | |
| |
| Hydrogen Levels |
8:22 | |
| |
Term Symbols & Atomic Spectra |
14:17 | |
| |
| Spin-Orbit Coupling |
14:18 | |
| |
| Selection Rules for Atomic Spectra |
21:31 | |
| |
| Selection Rules for Possible Transitions |
23:56 | |
| |
| Wave Numbers for The Transitions |
28:04 | |
| |
Example I: Calculate the Frequencies of the Allowed Transitions from (4d) ²D →(2p) ²P |
32:23 | |
| |
Helium Levels |
49:50 | |
| |
| Energy Levels for Helium |
49:51 | |
| |
Transitions & Spin Multiplicity |
52:27 | |
| |
| Transitions & Spin Multiplicity |
52:28 | |
Section 20: Term Symbols Example Problems |
|
Example Problems I |
1:01:20 |
| |
Intro |
0:00 | |
| |
Example I: What are the Term Symbols for the np¹ Configuration? |
0:10 | |
| |
Example II: What are the Term Symbols for the np² Configuration? |
20:38 | |
| |
Example III: What are the Term Symbols for the np³ Configuration? |
40:46 | |
|
Example Problems II |
56:34 |
| |
Intro |
0:00 | |
| |
Example I: Find the Term Symbols for the nd² Configuration |
0:11 | |
| |
Example II: Find the Term Symbols for the 1s¹2p¹ Configuration |
27:02 | |
| |
Example III: Calculate the Separation Between the Doublets in the Lyman Series for Atomic Hydrogen |
41:41 | |
| |
Example IV: Calculate the Frequencies of the Lines for the (4d) ²D → (3p) ²P Transition |
48:53 | |
Section 21: Equation Review for Quantum Mechanics |
|
Quantum Mechanics: All the Equations in One Place |
18:24 |
| |
Intro |
0:00 | |
| |
Quantum Mechanics Equations |
0:37 | |
| |
| De Broglie Relation |
0:38 | |
| |
| Statistical Relations |
1:00 | |
| |
| The Schrӧdinger Equation |
1:50 | |
| |
| The Particle in a 1-Dimensional Box of Length a |
3:09 | |
| |
| The Particle in a 2-Dimensional Box of Area a x b |
3:48 | |
| |
| The Particle in a 3-Dimensional Box of Area a x b x c |
4:22 | |
| |
| The Schrӧdinger Equation Postulates |
4:51 | |
| |
| The Normalization Condition |
5:40 | |
| |
| The Probability Density |
6:51 | |
| |
| Linear |
7:47 | |
| |
| Hermitian |
8:31 | |
| |
| Eigenvalues & Eigenfunctions |
8:55 | |
| |
| The Average Value |
9:29 | |
| |
| Eigenfunctions of Quantum Mechanics Operators are Orthogonal |
10:53 | |
| |
| Commutator of Two Operators |
10:56 | |
| |
| The Uncertainty Principle |
11:41 | |
| |
| The Harmonic Oscillator |
13:18 | |
| |
| The Rigid Rotator |
13:52 | |
| |
| Energy of the Hydrogen Atom |
14:30 | |
| |
| Wavefunctions, Radial Component, and Associated Laguerre Polynomial |
14:44 | |
| |
| Angular Component or Spherical Harmonic |
15:16 | |
| |
| Associated Legendre Function |
15:31 | |
| |
| Principal Quantum Number |
15:43 | |
| |
| Angular Momentum Quantum Number |
15:50 | |
| |
| Magnetic Quantum Number |
16:21 | |
| |
| z-component of the Angular Momentum of the Electron |
16:53 | |
| |
| Atomic Spectroscopy: Term Symbols |
17:14 | |
| |
| Atomic Spectroscopy: Selection Rules |
18:03 | |
Section 22: Molecular Spectroscopy |
|
Spectroscopic Overview: Which Equation Do I Use & Why |
50:02 |
| |
Intro |
0:00 | |
| |
Spectroscopic Overview: Which Equation Do I Use & Why |
1:02 | |
| |
| Lesson Overview |
1:03 | |
| |
| Rotational & Vibrational Spectroscopy |
4:01 | |
| |
| Frequency of Absorption/Emission |
6:04 | |
| |
| Wavenumbers in Spectroscopy |
8:10 | |
| |
| Starting State vs. Excited State |
10:10 | |
| |
| Total Energy of a Molecule (Leaving out the Electronic Energy) |
14:02 | |
| |
| Energy of Rotation: Rigid Rotor |
15:55 | |
| |
| Energy of Vibration: Harmonic Oscillator |
19:08 | |
| |
| Equation of the Spectral Lines |
23:22 | |
| |
Harmonic Oscillator-Rigid Rotor Approximation (Making Corrections) |
28:37 | |
| |
| Harmonic Oscillator-Rigid Rotor Approximation (Making Corrections) |
28:38 | |
| |
| Vibration-Rotation Interaction |
33:46 | |
| |
| Centrifugal Distortion |
36:27 | |
| |
| Anharmonicity |
38:28 | |
| |
| Correcting for All Three Simultaneously |
41:03 | |
| |
| Spectroscopic Parameters |
44:26 | |
| |
Summary |
47:32 | |
| |
| Harmonic Oscillator-Rigid Rotor Approximation |
47:33 | |
| |
| Vibration-Rotation Interaction |
48:14 | |
| |
| Centrifugal Distortion |
48:20 | |
| |
| Anharmonicity |
48:28 | |
| |
| Correcting for All Three Simultaneously |
48:44 | |
|
Vibration-Rotation |
59:47 |
| |
Intro |
0:00 | |
| |
Vibration-Rotation |
0:37 | |
| |
| What is Molecular Spectroscopy? |
0:38 | |
| |
| Microwave, Infrared Radiation, Visible & Ultraviolet |
1:53 | |
| |
| Equation for the Frequency of the Absorbed Radiation |
4:54 | |
| |
| Wavenumbers |
6:15 | |
| |
| Diatomic Molecules: Energy of the Harmonic Oscillator |
8:32 | |
| |
| Selection Rules for Vibrational Transitions |
10:35 | |
| |
| Energy of the Rigid Rotator |
16:29 | |
| |
| Angular Momentum of the Rotator |
21:38 | |
| |
| Rotational Term F(J) |
26:30 | |
| |
| Selection Rules for Rotational Transition |
29:30 | |
| |
| Vibration Level & Rotational States |
33:20 | |
| |
| Selection Rules for Vibration-Rotation |
37:42 | |
| |
| Frequency of Absorption |
39:32 | |
| |
| Diagram: Energy Transition |
45:55 | |
| |
| Vibration-Rotation Spectrum: HCl |
51:27 | |
| |
| Vibration-Rotation Spectrum: Carbon Monoxide |
54:30 | |
|
Vibration-Rotation Interaction |
46:22 |
| |
Intro |
0:00 | |
| |
Vibration-Rotation Interaction |
0:13 | |
| |
| Vibration-Rotation Spectrum: HCl |
0:14 | |
| |
| Bond Length & Vibrational State |
4:23 | |
| |
| Vibration Rotation Interaction |
10:18 | |
| |
| Case 1 |
12:06 | |
| |
| Case 2 |
17:17 | |
| |
Example I: HCl Vibration-Rotation Spectrum |
22:58 | |
| |
| Rotational Constant for the 0 & 1 Vibrational State |
26:30 | |
| |
| Equilibrium Bond Length for the 1 Vibrational State |
39:42 | |
| |
| Equilibrium Bond Length for the 0 Vibrational State |
42:13 | |
| |
| Bₑ & αₑ |
44:54 | |
|
The Non-Rigid Rotator |
29:24 |
| |
Intro |
0:00 | |
| |
The Non-Rigid Rotator |
0:09 | |
| |
| Pure Rotational Spectrum |
0:54 | |
| |
| The Selection Rules for Rotation |
3:09 | |
| |
| Spacing in the Spectrum |
5:04 | |
| |
| Centrifugal Distortion Constant |
9:00 | |
| |
| Fundamental Vibration Frequency |
11:46 | |
| |
| Observed Frequencies of Absorption |
14:14 | |
| |
| Difference between the Rigid Rotator & the Adjusted Rigid Rotator |
16:51 | |
| |
| Adjusted Rigid Rotator |
21:31 | |
| |
| Observed Frequencies of Absorption |
26:26 | |
|
The Anharmonic Oscillator |
30:53 |
| |
Intro |
0:00 | |
| |
The Anharmonic Oscillator |
0:09 | |
| |
| Vibration-Rotation Interaction & Centrifugal Distortion |
0:10 | |
| |
| Making Corrections to the Harmonic Oscillator |
4:50 | |
| |
| Selection Rule for the Harmonic Oscillator |
7:50 | |
| |
| Overtones |
8:40 | |
| |
| True Oscillator |
11:46 | |
| |
| Harmonic Oscillator Energies |
13:16 | |
| |
| Anharmonic Oscillator Energies |
13:33 | |
| |
| Observed Frequencies of the Overtones |
15:09 | |
| |
| True Potential |
17:22 | |
| |
| HCl Vibrational Frequencies: Fundamental & First Few Overtones |
21:10 | |
| |
Example I: Vibrational States & Overtones of the Vibrational Spectrum |
22:42 | |
| |
| Example I: Part A - First 4 Vibrational States |
23:44 | |
| |
| Example I: Part B - Fundamental & First 3 Overtones |
25:31 | |
| |
Important Equations |
27:45 | |
| |
| Energy of the Q State |
29:14 | |
| |
| The Difference in Energy between 2 Successive States |
29:23 | |
| |
| Difference in Energy between 2 Spectral Lines |
29:40 | |
|
Electronic Transitions |
1:01:33 |
| |
Intro |
0:00 | |
| |
Electronic Transitions |
0:16 | |
| |
| Electronic State & Transition |
0:17 | |
| |
| Total Energy of the Diatomic Molecule |
3:34 | |
| |
| Vibronic Transitions |
4:30 | |
| |
| Selection Rule for Vibronic Transitions |
9:11 | |
| |
| More on Vibronic Transitions |
10:08 | |
| |
| Frequencies in the Spectrum |
16:46 | |
| |
| Difference of the Minima of the 2 Potential Curves |
24:48 | |
| |
| Anharmonic Zero-point Vibrational Energies of the 2 States |
26:24 | |
| |
| Frequency of the 0 → 0 Vibronic Transition |
27:54 | |
| |
| Making the Equation More Compact |
29:34 | |
| |
| Spectroscopic Parameters |
32:11 | |
| |
| Franck-Condon Principle |
34:32 | |
| |
Example I: Find the Values of the Spectroscopic Parameters for the Upper Excited State |
47:27 | |
| |
Table of Electronic States and Parameters |
56:41 | |
Section 23: Molecular Spectroscopy Example Problems |
|
Example Problems I |
33:47 |
| |
Intro |
0:00 | |
| |
Example I: Calculate the Bond Length |
0:10 | |
| |
Example II: Calculate the Rotational Constant |
7:39 | |
| |
Example III: Calculate the Number of Rotations |
10:54 | |
| |
Example IV: What is the Force Constant & Period of Vibration? |
16:31 | |
| |
Example V: Part A - Calculate the Fundamental Vibration Frequency |
21:42 | |
| |
Example V: Part B - Calculate the Energies of the First Three Vibrational Levels |
24:12 | |
| |
Example VI: Calculate the Frequencies of the First 2 Lines of the R & P Branches of the Vib-Rot Spectrum of HBr |
26:28 | |
|
Example Problems II |
1:01:05 |
| |
Intro |
0:00 | |
| |
Example I: Calculate the Frequencies of the Transitions |
0:09 | |
| |
Example II: Specify Which Transitions are Allowed & Calculate the Frequencies of These Transitions |
22:07 | |
| |
Example III: Calculate the Vibrational State & Equilibrium Bond Length |
34:31 | |
| |
Example IV: Frequencies of the Overtones |
49:28 | |
| |
Example V: Vib-Rot Interaction, Centrifugal Distortion, & Anharmonicity |
54:47 | |
|
Example Problems III |
33:31 |
| |
Intro |
0:00 | |
| |
Example I: Part A - Derive an Expression for ∆G( r ) |
0:10 | |
| |
Example I: Part B - Maximum Vibrational Quantum Number |
6:10 | |
| |
Example II: Part A - Derive an Expression for the Dissociation Energy of the Molecule |
8:29 | |
| |
Example II: Part B - Equation for ∆G( r ) |
14:00 | |
| |
Example III: How Many Vibrational States are There for Br₂ before the Molecule Dissociates |
18:16 | |
| |
Example IV: Find the Difference between the Two Minima of the Potential Energy Curves |
20:57 | |
| |
Example V: Rotational Spectrum |
30:51 | |
Section 24: Statistical Thermodynamics |
|
Statistical Thermodynamics: The Big Picture |
1:01:15 |
| |
Intro |
0:00 | |
| |
Statistical Thermodynamics: The Big Picture |
0:10 | |
| |
| Our Big Picture Goal |
0:11 | |
| |
| Partition Function (Q) |
2:42 | |
| |
| The Molecular Partition Function (q) |
4:00 | |
| |
| Consider a System of N Particles |
6:54 | |
| |
| Ensemble |
13:22 | |
| |
| Energy Distribution Table |
15:36 | |
| |
| Probability of Finding a System with Energy |
16:51 | |
| |
| The Partition Function |
21:10 | |
| |
| Microstate |
28:10 | |
| |
| Entropy of the Ensemble |
30:34 | |
| |
| Entropy of the System |
31:48 | |
| |
Expressing the Thermodynamic Functions in Terms of The Partition Function |
39:21 | |
| |
| The Partition Function |
39:22 | |
| |
| Pi & U |
41:20 | |
| |
| Entropy of the System |
44:14 | |
| |
| Helmholtz Energy |
48:15 | |
| |
| Pressure of the System |
49:32 | |
| |
| Enthalpy of the System |
51:46 | |
| |
| Gibbs Free Energy |
52:56 | |
| |
| Heat Capacity |
54:30 | |
| |
Expressing Q in Terms of the Molecular Partition Function (q) |
59:31 | |
| |
| Indistinguishable Particles |
62:16 | |
| |
| N is the Number of Particles in the System |
63:27 | |
| |
| The Molecular Partition Function |
65:06 | |
| |
| Quantum States & Degeneracy |
67:46 | |
| |
| Thermo Property in Terms of ln Q |
70:09 | |
| |
| Example: Thermo Property in Terms of ln Q |
73:23 | |
|
Statistical Thermodynamics: The Various Partition Functions I |
47:23 |
| |
Intro |
0:00 | |
| |
Lesson Overview |
0:19 | |
| |
Monatomic Ideal Gases |
6:40 | |
| |
| Monatomic Ideal Gases Overview |
6:42 | |
| |
| Finding the Parition Function of Translation |
8:17 | |
| |
| Finding the Parition Function of Electronics |
13:29 | |
| |
| Example: Na |
17:42 | |
| |
| Example: F |
23:12 | |
| |
| Energy Difference between the Ground State & the 1st Excited State |
29:27 | |
| |
| The Various Partition Functions for Monatomic Ideal Gases |
32:20 | |
| |
| Finding P |
43:16 | |
| |
| Going Back to U = (3/2) RT |
46:20 | |
|
Statistical Thermodynamics: The Various Partition Functions II |
54:09 |
| |
Intro |
0:00 | |
| |
Diatomic Gases |
0:16 | |
| |
| Diatomic Gases |
0:17 | |
| |
| Zero-Energy Mark for Rotation |
2:26 | |
| |
| Zero-Energy Mark for Vibration |
3:21 | |
| |
| Zero-Energy Mark for Electronic |
5:54 | |
| |
| Vibration Partition Function |
9:48 | |
| |
| When Temperature is Very Low |
14:00 | |
| |
| When Temperature is Very High |
15:22 | |
| |
| Vibrational Component |
18:48 | |
| |
| Fraction of Molecules in the r Vibration State |
21:00 | |
| |
| Example: Fraction of Molecules in the r Vib. State |
23:29 | |
| |
| Rotation Partition Function |
26:06 | |
| |
| Heteronuclear & Homonuclear Diatomics |
33:13 | |
| |
| Energy & Heat Capacity |
36:01 | |
| |
| Fraction of Molecules in the J Rotational Level |
39:20 | |
| |
| Example: Fraction of Molecules in the J Rotational Level |
40:32 | |
| |
| Finding the Most Populated Level |
44:07 | |
| |
Putting It All Together |
46:06 | |
| |
| Putting It All Together |
46:07 | |
| |
| Energy of Translation |
51:51 | |
| |
| Energy of Rotation |
52:19 | |
| |
| Energy of Vibration |
52:42 | |
| |
| Electronic Energy |
53:35 | |
Section 25: Statistical Thermodynamics Example Problems |
|
Example Problems I |
48:32 |
| |
Intro |
0:00 | |
| |
Example I: Calculate the Fraction of Potassium Atoms in the First Excited Electronic State |
0:10 | |
| |
Example II: Show That Each Translational Degree of Freedom Contributes R/2 to the Molar Heat Capacity |
14:46 | |
| |
Example III: Calculate the Dissociation Energy |
21:23 | |
| |
Example IV: Calculate the Vibrational Contribution to the Molar heat Capacity of Oxygen Gas at 500 K |
25:46 | |
| |
Example V: Upper & Lower Quantum State |
32:55 | |
| |
Example VI: Calculate the Relative Populations of the J=2 and J=1 Rotational States of the CO Molecule at 25°C |
42:21 | |
|
Example Problems II |
57:30 |
| |
Intro |
0:00 | |
| |
Example I: Make a Plot of the Fraction of CO Molecules in Various Rotational Levels |
0:10 | |
| |
Example II: Calculate the Ratio of the Translational Partition Function for Cl₂ and Br₂ at Equal Volume & Temperature |
8:05 | |
| |
Example III: Vibrational Degree of Freedom & Vibrational Molar Heat Capacity |
11:59 | |
| |
Example IV: Calculate the Characteristic Vibrational & Rotational temperatures for Each DOF |
45:03 | |