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Welcome to our Physics lesson on Degrees of Freedom and Molar Specific Heats, this is the fourth lesson of our suite of physics lessons covering the topic of Molar Specific Heats and Degrees of Freedom, you can find links to the other lessons within this tutorial and access additional physics learning resources below this lesson.
With degrees of freedom, we understand independent ways of a particle's motion. For example, a train moving on a railway has only one degree of freedom as it can move only according one direction - the direction determined by the tracks.
A translational motion can be a combination of motion in three linear directions, which we usually call X, Y and Z according the names of the three well-known perpendicular axes we have already seen in previous tutorials.
All atoms in monoatomic gases are assumed to move only in a translational way as even if they spin around themselves, this is not observable and relevant. Indeed, when you watch a football match, you don't care about the spinning effect of ball but only about its translational motion. This is why the internal energy of monoatomic gases is equal to
The number 3 is because there are three degrees of freedom in translational motion. The division by 2 is because every individual direction includes two sub-directions in itself. (left-right, back-forth, up-down).
In diatomic (two-atomic) molecules, there is a spinning effect produced which causes a double direction of rotation.
Therefore, in total we have 5 degrees of freedom for the internal energy, i.e.
If molecules are three or more atomic (polyatomic), there is another spinning direction added because two points form a line (one direction) while three point form a plane (two directions). Therefore, the total internal energy becomes
The table below shows the relationship between molar specific heats and degrees of freedom in ideal gases.
Based on the above analysis, James Clerk Maxwell formulated the theorem of the equipartition of energy, which says:
Every molecule has a certain number of degrees of freedom, which represent independent ways of storing energy. A portion of energy associated with a single degree of freedom is given by the expression
U = 1/2 kT (for a single molecule) or U = 1/2 RT (for a mole)
Thus, we can obtain a general form of the relationship between the number of degrees of freedom f and the molar specific heat at constant volume CV for an ideal gas in terms of the ideal gas constant R:
There is also a vibrational motion caused by the oscillations of diatomic or polyatomic molecules, whose behaviour is described through quantum theory, but which goes beyond the scope of this tutorial. It required higher amounts of energy to take place then the other two types of motion explained here. Therefore, we neglect this kind of motion when energy stored in molecules is relatively small.
You have reached the end of Physics lesson 13.8.4 Degrees of Freedom and Molar Specific Heats. There are 4 lessons in this physics tutorial covering Molar Specific Heats and Degrees of Freedom, you can access all the lessons from this tutorial below.
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