(a)
Interpretation:
The total contribution to the molar internal energy of gaseous
Concept Introduction:
According to equipartition theorem, each translational and rotational degree of freedom contributes
(a)
Explanation of Solution
For all atoms and molecules, there are three translational degrees of freedom. The average molar translational energy is therefore
For linear molecules rotate about two axes, perpendicular to the internuclear axis. The average molar rotational energy is therefore
For linear molecules, there are
Consider the molecule
(b)
Interpretation:
The total contribution to the molar internal energy of gaseous
Concept Introduction:
According to equipartition theorem, each translational and rotational degree of freedom contributes
(b)
Explanation of Solution
For all atoms and molecules, there are three translational degrees of freedom. The average molar translational energy is therefore
For linear molecules rotate about two axes, perpendicular to the internuclear axis. The average molar rotational energy is therefore
For linear molecules, there are
Consider the molecule
(c)
Interpretation:
The total contribution to the molar internal energy of gaseous
Concept Introduction:
According to equipartition theorem, each translational and rotational degree of freedom contributes
(c)
Explanation of Solution
For all atoms and molecules, there are three translational degrees of freedom. The average molar translational energy is therefore
For nonlinear molecules rotate about three axes. The average molar rotational energy is therefore
For nonlinear molecules, there are
Consider the molecule
(d)
Interpretation:
The total contribution to the molar internal energy of gaseous
Concept Introduction:
According to equipartition theorem, each translational and rotational degree of freedom contributes
(d)
Explanation of Solution
For all atoms and molecules, there are three translational degrees of freedom. The average molar translational energy is therefore
For nonlinear molecules rotate about three axes. The average molar rotational energy is therefore
For nonlinear molecules, there are
Consider the molecule
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Chapter 2 Solutions
Elements Of Physical Chemistry
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