Physical Chemistry @ Stockton

All things relevant to Physical Chemistry I & II at Stockton.

Archive for September, 2009

Combined first and second law

Posted by richardm on 25th September 2009

We combined our two laws to form an expression for the internal energy that was a function of the extensive variables S and V. This lead to formal definitions of thermodynamic variables T & P as wells as Maxwell relations. We also introduced H(S,P) which came from our definition of enthalpy. We had a brief discussion about the upcoming exam next Friday, with more details to come later. An old exam from 2008 has been posted online.

We also completed 2 of 3 practice problems. You should prepare the third one for class on Wednesday.

Reminder: we will not be meeting on Monday and Homework #4 is due Wednesday.

Summary - Slides - Practice Problems

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Working with entropy

Posted by richardm on 24th September 2009

We looked at how to determine entropy changes during different processes. We also examined how S for the system and surroundings are different for reversible and irreversible processes. Finally we figured out how to determine entropy changes as a function of temperature.

Summary - Slides

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Entropy and the second law

Posted by richardm on 21st September 2009

We examined entropy, spontaneity and applications to the Carnot cycle.

Homework #4 was distributed and is due next Monday.

Summary - Slides - Homework #4

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Practice problems

Posted by richardm on 18th September 2009

We discussed some of the upcoming homework assignment and then completed the practice problems.

Have a great weekend.

Posted in Lecture | No Comments »

More on thermochemistry

Posted by richardm on 16th September 2009

We talked about how in incorporate phase transition into our understanding of thermochemistry. We then worked on some practice problems.

Summary - Slides - Practice problems

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Homework #2 Question

Posted by richardm on 15th September 2009

There have been several questions regarding part (c) of Question 1. You are asked to find Delta U, q, and w for the composite process, not necessarily each individual part. You cannot find q for each part since you are not given enough information to do the calculation. However, if you can determine U and w, you can then find q for the composite (entire) process.

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Enthalpy and Thermochemistry

Posted by richardm on 14th September 2009

We discussed the uses for enthalpy when working at constant pressure. We also explored the use of enthalpies of reactions and how to deal with non-standard states.

Summary - Slides

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More on the first law, ideal gases, and enthalpy

Posted by richardm on 11th September 2009

We explored ideal gases and the dependence of U and H on temperature. Two practice problems were completed to illustrate this relationship.

Homework #2 will be due on Wednesday, September 16

Summary - Slides

(Updated 9/14/09: Summary has been corrected)

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Heat capacity and working with the first law

Posted by richardm on 9th September 2009

Lecture summary and slides from today’s class. We discussed heat capacity as a way to relate heat transfer to a changed in temperature. Also looked at how to do calculations involving P-V work and an ideal gas.

Model solutions for Homework #1 are posted and Homework #2 was distributed.

Summary - Slides - Practice Problems

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Thermodynamic Variables, Systems, Processes & the First Law

Posted by richardm on 4th September 2009

Lecture summary and slides from today’s class where we discussed different types of thermodynamics variables and the relationship between them. We also introduced different types of processes and systems that will be important in future discussions. Finally we came to the First Law of Thermodynamics and the concepts of work and heat.

Summary - Slides

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