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Schaum’s Outline of College Physics

Eugene Hecht

Chapter 43

The Hydrogen Atom - all with Video Answers

Educators


Chapter Questions

01:44

Problem 1

What wavelength does a hydrogen atom emit as its excited electron descends from the $n=5$ state to the $n=2$ state? Give your answer to three significant figures.
From the Bohr model we know that the energy levels of the hydrogen atom are given by $\mathrm{E}_{n}=-13.6 / \mathrm{n}^{2} \mathrm{eV}$, and therefore
$$
\mathrm{E} 5=-0.54 \mathrm{eV} \quad \text { and } \quad \mathrm{E} 2=-3.40 \mathrm{eV}
$$
The energy difference between these states is $3.40-0.54=2.86$ $\mathrm{eV}$. Because $1240 \mathrm{~nm}$ corresponds to $1.00 \mathrm{eV}$ in an inverse proportion (i.e., the more energetic the photon, the shorter the wavelength), we have, for the wavelength of the emitted photon,
$$
\lambda=\left(\frac{1.00 \mathrm{eV}}{2.86 \mathrm{eV}}\right)(1240 \mathrm{~nm})=434 \mathrm{~nm}
$$

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04:40

Problem 2

When a hydrogen atom is bombarded, the atom may be raised into a higher energy state. As the excited electron falls back to the lower energy levels, light is emitted. What are the three longestwavelength spectral lines emitted by the hydrogen atom as it returns to the $n=1$ state from higher energy states? Give your answers to three significant figures.
We are interested in the following transitions (see Fig. $43-1$ ):
$$
\begin{array}{ll}
n=2 \rightarrow n=1: & \Delta \mathrm{E}_{2,1}=-3.4-(-13.6)=10.2 \mathrm{eV} \\
n=3 \rightarrow n=1: & \Delta \mathrm{E}_{3,1}=-1.5-(-13.6)=12.1 \mathrm{eV} \\
n=4 \rightarrow n=1: & \Delta \mathrm{E}_{4,1}=-0.85-(-13.6)=12.8 \mathrm{eV}
\end{array}
$$
To find the corresponding wavelengths, proceed as in Problem 43.1, or use $\Delta \mathrm{E}=h f=h c / \lambda$. For example, for the $n=2$ to $n=1$ transition,
$$
\lambda=\frac{h c}{\Delta E_{2,1}}=\frac{\left(6.63 \times 10^{-34} \mathrm{~J} \cdot \mathrm{s}\right)\left(2.998 \times 10^{8} \mathrm{~m} / \mathrm{s}\right)}{(10.2 \mathrm{eV})\left(1.60 \times 10^{-19} \mathrm{~J} / \mathrm{eV}\right)}=1.22 \mathrm{~nm}
$$
The other lines are found in the same way to be $102 \mathrm{~nm}$ and $96.9$ $\mathrm{nm}$. These are the first three lines of the Lyman series.

Amit Srivastava
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02:11

Problem 3

The series limit wavelength of the Balmer series is emitted as the electron in the hydrogen atom falls from the $n=\infty$ state to the $n=$ 2 state. What is the wavelength of this line (to three significant figures)?
From $\underline{\text { Fig. } 43-1,} \Delta \mathrm{E}=3.40-0=3.40 \mathrm{eV}$. We find the corresponding wavelength in the usual way from $\Delta \mathrm{E}=h c / \lambda .$ The result is $365 \mathrm{~nm}$.

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02:07

Problem 4

What is the greatest wavelength (lowest frequency) of radiation that will ionize unexcited hydrogen atoms?
The incident photons must have enough energy to raise the atom from the $n=1$ level to the $n=\infty$ level when absorbed by the atom. Because $\mathrm{E}_{\infty}-\mathrm{E}_{1}=13.6 \mathrm{eV}$, we can use $\mathrm{E} \infty-\mathrm{E}_{1}=h c / \lambda$, to find the wavelength as $91.2 \mathrm{~nm}$. Wavelengths shorter than this would not only remove the electron from the atom but would add $\mathrm{KE}$ to the removed electron.

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03:49

Problem 5

The energy levels for singly ionized helium atoms (atoms from which one of the two electrons has been removed) are given by $\mathrm{E}_{n}$ $=\left(-54.4 / n^{2}\right) \mathrm{eV}$. Construct the energy-level diagram for this system.

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03:45

Problem 6

What are the two longest wavelengths of the Balmer series for singly ionized helium atoms?
The pertinent energy-level diagram is shown in Fig. 43-3. Recall that the Balmer series corresponds to transitions from higher states to the $n=2$ state. From the diagram, the two smallest-energy transitions to the $n=2$ states are
$$
\begin{array}{ll}
n=3 \rightarrow n=2 & \Delta \mathrm{E}_{3,2}=13.6-6.04=7.6 \mathrm{eV} \\
n=4 \rightarrow n=2 & \Delta \mathrm{E}_{4,2}=13.6-3.4=10.2 \mathrm{eV}
\end{array}
$$
Using the fact that $1 \mathrm{eV}$ corresponds to $1240 \mathrm{~nm}$, we find the corresponding wavelengths to be $163 \mathrm{~nm}$ and $122 \mathrm{~nm}$; both wavelengths are in the far ultraviolet or long X-ray region.

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02:20

Problem 7

Unexcited hydrogen atoms are bombarded with electrons that have been accelerated through $12.0 \mathrm{~V}$. What wavelengths will the atoms emit?
When an atom in the ground state is given $12.0 \mathrm{eV}$ of energy, the most these electrons can supply, the atom can be excited no higher than $12.0 \mathrm{eV}$ above the ground state. Only one state exists in this energy region, the $n=2$ state. Hence, the only transition possible is
$$
n=2 \rightarrow n=1: \quad \Delta \mathrm{E}_{2,1}=13.6-3.4=10.2 \mathrm{eV}
$$
The only emitted wavelength will be
$$
\lambda=(1240 \mathrm{~nm})\left(\frac{1.00 \mathrm{eV}}{10.2 \mathrm{eV}}\right)=122 \mathrm{~nm}
$$
which is the longest-wavelength line in the Lyman series.

Amit Srivastava
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01:27

Problem 8

Unexcited hydrogen gas is an electrical insulator because it contains no free electrons. What maximum-wavelength photon beam incident on the gas can cause the gas to conduct electricity?
The photons in the beam must ionize the atom so as to produce free electrons. (This is called the atomic photoelectric effect.) To do this, the photon energy must be at least $13.6 \mathrm{eV}$, and so the maximum wavelength is
$$
\lambda=(1240 \mathrm{~nm})\left(\frac{1.00 \mathrm{eV}}{13.6 \mathrm{eV}}\right)=91.2 \mathrm{~nm}
$$
which is the series limit for the Lyman series.

Amit Srivastava
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01:30

Problem 9

A bright yellow sodium emission line has a wavelength of $587.561$ $8 \mathrm{~nm} .$ Determine the difference between the atom's two energy levels defining the transition. Give your answer in $\mathrm{eV}$ to four significant figures.

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01:22

Problem 10

Molecules have low-energy vibration modes, and they can make transitions from one such state to another that result in the emission of infrared radiant energy. Suppose two such states are separated by $0.015 \mathrm{eV}$, and the molecule descends in energy from the higher to the lower. Determine the wavelength of the photon that would be emitted.

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03:15

Problem 11

Derive the expression
$$
r_{n}=n^{2} \hbar^{2} / m_{e} k_{0} e^{2} \quad n=1,2,3, \ldots
$$
for the radius of the $n$ th electron orbit where $h=\mathrm{h} / 2 \pi$. [Hint: Study Eqs. (43.1) and (43.2).]

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01:59

Problem 12

When $n=1$ in Eq. (43.9), we get the radius of the lowest energy orbit (the ground state orbit) called the Bohr radius. Numerically that's
$$
r_{1}=0.0529177 \mathrm{~nm}
$$
Using Eq. (43.9), show that the diameter of a hydrogen atom is just about $0.10 \mathrm{~nm}$, thereby confirming Eq. (43.10) to four significant figures.

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01:14

Problem 13

Show that for the hydrogen atom as described by the Bohr model, the allowed orbital radii are given by
$$
r_{n}=n^{2} r_{1} \quad n=1,2,3, \ldots
$$
By the way, here $n$ is known as the principal quantum number. [Hint: Study the previous two problems.]

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02:18

Problem 14

Show that for the hydrogen atom as described by the Bohr model, the classical KE of the electron $\left(\frac{1}{2} m_{e} v_{n}^{2}\right)$ is given by
$$
\mathrm{KE}_{\mathrm{e}}=k_{0} e^{2} / 2 r_{n} \quad n=1,2,3, \ldots
$$
[Hint: Study Eq. (43.2).]

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01:23

Problem 15

In the Bohr theory the total energy of the orbiting electron, $\mathrm{E}_{n}$, equals the sum of the electron's KE plus its PE, where from Coulomb's Law, $\mathrm{PE}=-\mathrm{k}_{0} e^{2} / r_{n} .$ Show that
$$
\mathrm{E}_{n}=-k_{0} e^{2} / 2 r_{n} \quad n=1,2,3, \ldots
$$
The minus sign arises because this is a bound state and the PE is negative. [Hint: Study the previous problem.]

Amit Srivastava
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03:02

Problem 16

In the Bohr theory the total energy of the orbiting electron is $\mathrm{E}_{n}$. Show that
$$
\mathrm{E}_{n}=-2 \pi^{2} k_{0}^{2} e^{4} m_{e} / h^{2} n^{2} \quad n=1,2,3, \ldots
$$
The minus sign arises because this is a bound state and the $\mathrm{PE}$ is negative. [Hint: Study the previous problem.]

Amit Srivastava
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02:37

Problem 17

Verify Eq. (43.3). [Hint: Use Eq. (43.14).]

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01:32

Problem 18

How much energy should be pumped into a hydrogen atom to raise it from its ground state into its 2nd excited state? [Hint: The 2nd excited state corresponds to $n=3$; examine Fig. 43-1.]

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01:20

Problem 19

A hydrogen atom in its 1 st excited state drops down to its ground state emitting a photon in the process. Find the energy of that photon. [Hint: Study Eq. (43.5).]

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01:19

Problem 20

A hydrogen atom in its 1 st excited state drops down to its ground state emitting a photon in the process. Calculate the wavelength of that photon. [Hint: Study Eq. (43.5).]

Amit Srivastava
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00:47

Problem 21

One spectral line in the hydrogen spectrum has a wavelength of $821 \mathrm{~nm}$. What is the energy difference between the two states that gives rise to this line?

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04:00

Problem 22

What are the energies of the two longest-wavelength lines in the Paschen series for hydrogen? What are the corresponding wavelengths? Give your answers to two significant figures.

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02:05

Problem 23

What is the wavelength of the series limit line for the hydrogen Paschen series? Consult Problem $43.3$ for an explanation of "series limit."

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01:03

Problem 24

The lithium atom has a nuclear charge of $+3 e$. Find the energy required to remove the third electron from a lithium atom that has already lost two of its electrons. Assume the third electron to be initially in the ground state.

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01:28

Problem 25

Electrons in an electron beam are accelerated through a potential difference $V$ and are incident on hydrogen atoms in their ground state. What is the maximum value for $V$ if the collisions are to be perfectly elastic?

Amit Srivastava
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02:22

Problem 26

What are the three longest photon wavelengths that singly ionized helium atoms (in their ground state) will absorb strongly? (See $\underline{\text { Fig. } 43-3 .}$.)

Amit Srivastava
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01:34

Problem 27

How much energy is required to remove the second electron from a singly ionized helium atom? What is the maximum wavelength of an incident photon that could tear this electron from the ion?

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01:18

Problem 28

In the spectrum of singly ionized helium, what is the series limit for its Balmer series?

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