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An Introduction to Thermodynamics and Statistical Mechanics

Keith Stowe

Chapter 4

Internal energy - all with Video Answers

Educators


Chapter Questions

01:52

Problem 1

Give examples of types of energy that would be part of your body's internal energy, and of types of energy that would not, unless the system were enlarged to include your environment.

Susan Hallstrom
Susan Hallstrom
Numerade Educator
01:26

Problem 2

Consider the average potential energy of a water molecule in an ice crystal and of one in the liquid state. Which is lower? How do you know?

Nicole Smina
Nicole Smina
Numerade Educator
03:12

Problem 3

(a) Show that the function $f(x)=x^3+x^2-2$ has a local minimum at $x=0$.
(b) Expand this function in a Taylor series around the point $x=0$, up to the fourth-order term (the term in $x^4$ ).
(c) If we keep terms only to order $x^2$, what is the range in $x$ for which our error is less than $10 \%$ ?

Charles Machakwa
Charles Machakwa
Numerade Educator
02:27

Problem 4

Repeat the above problem for the function $f(x)=-\mathrm{e}^{-x^2}$.

Anthony Ramos
Anthony Ramos
Numerade Educator
10:16

Problem 5

Expand the functions $\sin x, \cos x, \ln (1+x)$, and $\mathrm{e}^x$ to order $x^4$ in Taylor series expansions around the origin. Do you see any pattern in these expansions that would allow you to continue the expansion to any order? Write out each of these infinite series in closed form.

$$
\left(\text { E.g. }, \sin x=\sum_{n=0}^{\infty} \frac{(-1)^n}{(2 n+1)!} x^{2 v+1}\right)
$$

Mir  Afzal
Mir Afzal
Numerade Educator
06:21

Problem 6

We are going to make a very rough estimate of how much pressure must be applied to a typical solid to compress it to the point where the potential energy reference level $u_0$ of the individual atoms becomes positive. Ordinarily, for a typical solid, $u_0$ is around -0.2 eV .
(a) If the interatomic spacings are typically 0.2 nm , how many atoms are there per cubic meter?
(b) Roughly, how much work (in joules) must be done on one cubic meter of this solid to raise $u_0$ to zero?
(c) Work is equal to force times distance parallel to the force ( $F \mathrm{~d} x$ ) but, by multiplying and dividing by the perpendicular surface area, this can be changed into pressure times volume ( $-p \mathrm{~d} V$ ). Because solids are elastic, the change in volume is proportional to the change in applied pressure, $\mathrm{d} V=-C \mathrm{~d} p$, and the constant $C$ is typically $10^{-17} \mathrm{~m}^5 / \mathrm{N}$. With this background, calculate the work done on a solid as the external pressure is increased from 0 to some final value $p_f$.
(d) With your answer to part (c) above, estimate the pressure that must be exerted on a typical solid to compress it to the point where $u_0$ becomes positive (Figure 4.4, top right).
(e) What is a typical value for the variation of $u_0$ with pressure, $\partial u_0 / \partial p$, at constant temperature and atmospheric pressure in a solid?

Kai Chen
Kai Chen
Princeton University
02:23

Problem 7

Consider the following three systems: (A) the water molecules in a cold soft drink, (B) the copper atoms in a brass doorknob, and (C) the helium atoms in a blimp (a small cigar-shaped airship). Below are listed expressions of the energy for an atom in each system. In each case, fill in the blank with the letter of the most appropriate system.
$-\varepsilon=u_0+\frac{1}{2} \kappa x^2+\frac{1}{2} \kappa y^2+\frac{1}{2} \kappa z^2+\frac{1}{2 m} p_x^2+\frac{1}{2 m} p_y^2+\frac{1}{2 m} p_z^2$
$-\varepsilon=\frac{1}{2 m} p_x^2+\frac{1}{2 m} p_y^2+\frac{1}{2 m} p_z^2$
$-\varepsilon=u_0+\frac{1}{2 m} p_x^2+\frac{1}{2 m} p_y^2+\frac{1}{2 m} p_z^2$

Zhaojie Xu
Zhaojie Xu
Numerade Educator
01:54

Problem 8

We are going to estimate the vibrational energy of the first excited state for a nitrogen molecule $\left(\mathrm{N}_2\right)$. Each atom finds itself in a potential well due to its interactions with the other atom. This potential well is roughly 0.02 nm across.
(a) What are the wavelengths of the longest two standing waves that would fit in this well?
(b) What momenta do these correspond to?
(c) Considering kinetic energy only, how much energy in eV would be required to excite an atom from the ground state to the first excited state? (The mass of a nitrogen atom is $2.34 \times 10^{-26} \mathrm{~kg}$.)
(d) To estimate the minimum temperature needed for excitations to occur, we compare $k T$ (where $k=1.38 \times 10^{-23} \mathrm{~J} / \mathrm{K}=8.63 \times 10^{-5} \mathrm{eV} / \mathrm{K}$ ) with the energy required to reach the first excited state. Roughly what is the minimum temperature needed for vibrational excitations in nitrogen gas?

Chai Santi
Chai Santi
Numerade Educator
04:30

Problem 9

Consider the rotation of diatomic molecules around an axis that runs perpendicular through the midpoint of the line that joins the two atoms (see Figure 4.6). The mass of a nitrogen atom is $2.34 \times 10^{-26} \mathrm{~kg}$, and the interatomic separation in an $\mathrm{N}_2$ molecule is $1.10 \times 10^{-10} \mathrm{~m}$.
(a) What is the rotational inertia of an $\mathrm{N}_2$ molecule around this axis? $\left(I=\sum m_i r_j^2\right)$
(b) Find the energy in eV required to excite this molecule from the nonrotating state to the first excited rotational state (i.e., from $l=0$ to $l=1$, where $\left.L^2=l(l+1) \hbar^2\right)$.
(c) What is the minimum temperature for rotational excitations in nitrogen? See problem 8(d).

Hubert Agamasu
Hubert Agamasu
Numerade Educator
05:19

Problem 10

Repeat problem 9 for an oxygen molecule, $\mathrm{O}_2$, given that the mass of an oxygen atom is $2.67 \times 10^{-26} \mathrm{~kg}$ and the interatomic spacing is $1.21 \times 10^{-10} \mathrm{~m}$.

Linda Winkler
Linda Winkler
Numerade Educator
View

Problem 11

Repeat problem 9 for a hydrogen molecule, given that the mass of a hydrogen atom is $1.67 \times 10^{-27} \mathrm{~kg}$ and the interatomic spacing is $7.41 \times 10^{-11} \mathrm{~m}$.

Eduard Sanchez
Eduard Sanchez
Numerade Educator
05:43

Problem 12

How many degrees of freedom has a sodium atom in a salt crystal?

Susan Hallstrom
Susan Hallstrom
Numerade Educator

Problem 13

Why do you suppose that, at high temperatures, a molecule of water vapor $\left(\mathrm{H}_2 \mathrm{O}\right)$ has three rotational degrees of freedom and a molecule of nitrogen gas ( $\mathrm{N}_2$ ) has only two?

Check back soon!
03:11

Problem 14

Assuming that a conduction electron in a metal is free to roam anywhere within the metal (not being constrained to any small region by a particular well), how many degrees of freedom does it have?

Salamat Ali
Salamat Ali
Numerade Educator
09:01

Problem 15

Consider the phase change for iron from solid to liquid forms.
(a) How many degrees of freedom does each iron atom have in the solid state?
(b) After it has melted?
(c) Did the number of degrees of freedom of the conduction electrons change?
(d) Did the number of degrees of freedom of the whole system increase or decrease?
(e) On a microscopic scale, what happens to the energy put into the iron to melt it?

CA
Chi-Chung Ai
Numerade Educator
00:53

Problem 16

The heat capacities of some diatomic gas molecules show that they have three degrees of freedom at very low temperatures, five degrees of freedom at intermediate temperatures, and seven degrees of freedom at very high temperatures. How would you explain this?

Rashmi Gondi
Rashmi Gondi
Numerade Educator
02:14

Problem 17

Estimate the molar heat capacity of a diatomic gas with five degrees of freedom per molecule, by calculating how many joules of energy must be added to raise the temperature by $1^{\circ} \mathrm{C}$. (Assume that the volume is constant, so that only heat is added and no work is done.)

Dominador Tan
Dominador Tan
Numerade Educator
02:02

Problem 18

(a) Make an estimate of $u_0$ (in eV ) for a water molecule in the liquid state at $100^{\circ} \mathrm{C}$. Assume that there are six degrees of freedom per molecule in both the liquid and the vapor states and that 2260 kJ of energy per kg are released when it condenses. Ignore any work done on the molecule due to the change in volume.
(b) What is the average thermal energy per molecule?
(c) What is the average total energy per molecule for liquid water at $100^{\circ} \mathrm{C}$ ?

Manish Jain
Manish Jain
Numerade Educator
02:58

Problem 19

At $0^{\circ} \mathrm{C}$, a water molecule in both ice and liquid water has six degrees of freedom. One mole of water has mass 18 grams and a latent heat of fusion equal to 6025 joules per mole. Given this information, calculate the following in units of eV :
(a) the average thermal energy per molecule in liquid water at $0^{\circ} \mathrm{C}$ and in ice at $0^{\circ} \mathrm{C}$,
(b) the amount of energy per molecule added in making the phase change,
(c) the change in the potential energy reference level $u_0$ in going from the solid to the liquid state.
Does the water's thermal energy increase, decrease, or remain the same as ice melts?

Keshav Singh
Keshav Singh
Numerade Educator
04:09

Problem 20

Using equipartition, calculate the root mean square value of the following quantities in a gas at room temperature ( 295 K ).
(a) The speed of a nitrogen molecule ( $m=4.68 \times 10^{-26} \mathrm{~kg}$ ).
(b) The speed of a hydrogen molecule ( $m=3.34 \times 10^{-27} \mathrm{~kg}$ ).
(c) The angular momentum of a diatomic oxygen molecule around one of the two rotational axes, for which its moment of inertia is $1.95 \times 10^{-46} \mathrm{~kg} \mathrm{~m}^2$.
(d) If the axis in part (c) is the $z$-axis, what would be the root mean square value of the quantum number $l_z$ ?

Jordan Vanevery
Jordan Vanevery
Numerade Educator
01:19

Problem 21

What is the total thermal energy at room temperature ( 293 K ) in a gram of (a) lead, (b) dry air $\left(78 \% \mathrm{~N}_2, 21 \% \mathrm{O}_2, 1 \% \mathrm{Ar}\right)$ ?

Jerrah Biggerstaff
Jerrah Biggerstaff
Numerade Educator
04:01

Problem 22

You are climbing a mountain and you and your equipment weigh 700 N . Suppose that of the food energy you use, one quarter goes into work (getting you up the mountain) and three quarters into waste heat. Half the waste heat goes into evaporating sweat. For every kilometer of elevation that you gain, how many kilograms of food do you burn, and how many kilograms of water do you lose? (Very roughly, food provides $4 \times 10^6 \mathrm{~J} / \mathrm{kg}$, and the latent heat of evaporation at the ambient temperature is about $2.5 \times 10^6 \mathrm{~J} / \mathrm{kg}$.)

Vishal Gupta
Vishal Gupta
Numerade Educator