Try doing this activity as a follow-up to the Changes in Internal Energy (Remote) about the first law of thermodynamics.
INSTRUCTIONS:
Orient: Imagine that you have water vapor in a container where you can control the temperature of the gas. The temperature and pressure axes show possible values of temperature and pressure for 1kg of water vapor.
It may be helpful to give an example of a state on the surface, or a full example of playing this “game”.
Provide Graph Axes Here: Need the empty \(T\) and \(p\) axes.
Goal: Gets at the idea that you only need two variables to specify the state. Cartesian or polar coordinates might come up as another example---talk about how axes in this case have different dimensions --- generally true in thermo.
Coordinate: Now imagine you did an experiment where you measured the pressure, \(p\) of the water vapor as you varied the temperature, \(T\), for several fixed values of entropy, \(S\), and volume, \(V\), and plotted these curves on the same set of axes. The new contour map shows these plots.
Prep: Need a contour map with \(U(T,p)\) with \(S, V\) contours, no states.
Goal: Gets at the idea that you can specify the state with any two of the four variables.
Note: Students might try to over-specify the state. Ask how many of the 3 or 4 variables you can independently pick. Maybe as a WCD have 3 groups each specify a different variable
Explore: Choose a second, nearby state and mark it on the graph. In as many different ways as you can, describe how to get from your old state to your new state.
Goal: Gets at the idea that you need to specify changes in two variables (“constant” is a specified change of zero)
Discussion: How many pieces of information did you have to give to describe a path? Could you have given less information?
Can you find a nearby state where the path involves holding one of the thermodynamic variables constant? 2 variables? 3 variables?
Goal: Gets at the idea that you can specify one variable to be constant. If you try to specify 2 (or 3) variables to be constant, then the new state is the same as the old state (you haven't gone anywhere).
New Representation: Can you find the states you have been considering on these alternate representations:
A rubber sheet that can be stretched and squished so that the \(S\) and \(V\) contours are straight and perpendicular to each other square.
Goal: The set of numbers that describes a state is unique and can be located on different representations of the system.
A plastic surface whose height represents the internal energy of the system.
Students will need to be told what the axes represent.
Extension:
Prep: Could have a demonstration \(U(T,p)\) surface to show students.
Goal: The set of numbers that describes a state is unique and can be located on different representations of the system.
Goals
- The number of pieces of information you need to specify a state/the number of independent variables is equal to the number of ways you can get energy into or out of the system (2 in the simplest thermo examples)
- Which variables are independent can be chosen for convenience.
- You cannot hold two variables constant and change the state if there are only two degrees of freedom.
Time Estimate: 30 minutes
Tools/Equipment
- Graph with empty \(T\) and \(p\) axes
- Graph of \(S\) and \(V\) contours on \(T\) and \(p\) axes
- (optional, for demonstration) \(U(T,p)\) plastic surface (blue)
Intro
- Little is needed. The only thing students need to know about entropy for this activity is that it is another state variable.
- This activity is a good follow-up to the Changes in Internal Energy activity about the 1st law of thermodynamics.
Whole Class Discussion:
- Get students to articulate that they needed 2 pieces of information to identify a state, but it didn't need to be the numbers located on the perpendicular axes - it could have been any two pieces of information.
- Introduce the language that simple thermal systems have 2 degrees of freedom (number of independent variables). The number of degrees of freedom is equal to the number of ways of getting energy into or out of the system. For simple thermal systems, you get energy into or out of the system through heat or work (1st law of thermodynamics)
- Changes in state also require specifying two changes - you can only hold 1 variable constant and change the state! If you hold two variables constant, you're stuck!
- There is freedom to choose which variables you want to be independent. “Choices” are usually related to what is controlled in an experiment.
- Two common ways to think about 2D graphs with 2 independent variables: with 1 independent variable on the horizontal axis, a dependent variable on the vertical axis, and the other independent variable labeling the curve (more common in thermo) OR with both independent variables on the axes and a dependent variables as a surface with levels curves on the graph (more common in E&M and mechanics)
group Small Group Activity
30 min.
assignment_ind Small White Board Question
10 min.
Cylindrical coordinates spherical coordinates curvilinear coordinates
First, students are shown diagrams of cylindrical and spherical coordinates. Common notation systems are discussed, especially that physicists and mathematicians use opposite conventions for the angles \(\theta\) and \(\phi\). Then students are asked to check their understanding by sketching several coordinate equals constant surfaces on their small whiteboards.group Small Group Activity
30 min.
group Small Group Activity
10 min.
face Lecture
120 min.
Gibbs entropy information theory probability statistical mechanics
These lecture notes for the first week of Thermal and Statistical Physics include a couple of small group activities in which students work with the Gibbs formulation of the entropy.group Small Group Activity
30 min.
group Small Group Activity
30 min.
group Small Group Activity
30 min.
group Small Group Activity
30 min.
accessibility_new Kinesthetic
10 min.