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An excited hydrogen atom emits a photon with an energy of \(1.133 \mathrm{eV}\). What were the initial and final states of the hydrogen atom before and after emitting the photon?

Short Answer

Expert verified
Answer: The initial state is 3, and the final state is 2.

Step by step solution

01

Recall the formula for energy levels in the hydrogen atom

The energy levels of the hydrogen atom can be determined using the following formula: \(E_n = -\dfrac{13.6 \mathrm{eV}}{n^2}\), where \(n\) is the principal quantum number (state) and \(E_n\) denotes the energy of the nth state.
02

Calculate the energy difference

The energy of the emitted photon is the difference in energy between the initial and final states of the atom. Thus, we can write the energy difference as: \(\Delta E = E_{initial} - E_{final} = 1.133 \mathrm{eV}\)
03

Use the formula for energy levels to find the possible state transitions

Since the energy difference is caused by a transition between two energy states, we can set up an equation to find the possible initial and final states: \(E_{initial} - E_{final} = \dfrac{13.6}{n^2_{final}} - \dfrac{13.6}{n^2_{initial}} = 1.133 \mathrm{eV}\)
04

Find the ratio of initial and final states

To simplify our calculation, let's call this ratio \(k\): \(k = \dfrac{1}{n^2_{initial}} - \dfrac{1}{n^2_{final}}\). Now, we can rewrite our equation as: \(13.6 \times k = 1.133 \mathrm{eV}\) Solving for \(k\), we get: \(k =\dfrac{1.133}{13.6} = 0.0833\)
05

Find the initial and final states that satisfy this ratio

Since \(n_{initial}\) and \(n_{final}\) are integers and \(n_{initial}>n_{final}\), we can find pairs of values \((n_{initial}, n_{final})\) that satisfy the condition \(k = \dfrac{1}{n^2_{initial}} - \dfrac{1}{n^2_{final}}\). After checking possible energy state transitions, we find that only the following pair of states satisfies the obtained ratio: \((n_{initial}, n_{final}) = (3, 2)\)
06

Conclude the initial and final states

Based on our calculations, the initial and final states of the hydrogen atom before and after emitting the photon are: Initial state: \(n_{initial} = 3\) Final state: \(n_{final} = 2\)

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Most popular questions from this chapter

An electron in a hydrogen atom is in the ground state (1s). Calculate the probability of finding the electron within a Bohr radius \(\left(a_{0}=0.05295 \mathrm{nm}\right)\) of the proton. The ground state wave function for hydrogen is: \(\psi_{1 s}(r)=A_{1 s} e^{-r / a_{0}}=e^{-r / a_{0}} / \sqrt{\pi a_{0}^{3}}\).

Find the energy difference between the ground state of hydrogen and deuterium (hydrogen with an extra neutron in the nucleus)

The radius of the \(n=1\) orbit in the hydrogen atom is $$ a_{0}=0.053 \mathrm{nm} $$ a) Compute the radius of the \(n=6\) orbit. How many times larger is this compared to the \(n=1\) radius? b) If an \(n=6\) electron relaxes to an \(n=1\) orbit (ground state), what is the frequency and wavelength of the emitted radiation? What kind of radiation was emitted (visible, infrared, etc.)? c) How would your answer in (a) change if the atom was a singly ionized helium atom \(\left(\mathrm{He}^{+}\right),\) instead?

What is the shortest possible wavelength of the Lyman series in hydrogen?

The binding energy of an extra electron when As atoms are doped in a Si crystal may be approximately calculated by considering the Bohr model of a hydrogen atom. a) Show the ground energy of hydrogen-like atoms in terms of the dielectric constant and the ground state energy of a hydrogen atom. b) Calculate the binding energy of the extra electron in a Si crystal. (The dielectric constant of Si is about 10.0 , and the effective mass of extra electrons in a Si crystal is about \(20.0 \%\) of that of free electrons.)

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