Problem 20
Question
If energy is absorbed by a hydrogen atom in its ground state, the atom is excited to a higher energy state. For example, the excitation of an electron from \(n=1\) to \(n=3\) requires radiation with a wavelength of \(102.6 \mathrm{nm}\) Which of the following transitions would require radiation of longer wavelength than this? (a) \(n=2\) to \(n=4\) (b) \(n=1\) to \(n=4\) (c) \(n=1\) to \(n=5\) (d) \(n=3\) to \(n=5\)
Step-by-Step Solution
Verified Answer
Transitions n=2 to n=4 and n=3 to n=5 require longer wavelengths.
1Step 1: Understanding Energy and Wavelength
In this problem, we are dealing with transitions between different energy levels of a hydrogen atom. The energy difference between two energy levels determines the wavelength of radiation required for transition. Since energy and wavelength are inversely related (according to the equation \( E = \frac{hc}{\lambda} \)), higher energy transitions correspond to shorter wavelengths and vice versa.
2Step 2: Energy Level Transitions
The energy levels of a hydrogen atom are quantized and calculated using the formula: \( E_n = -\frac{13.6}{n^2} \text{ eV} \), where \( n \) is the principal quantum number. To compare wavelengths for different transitions, calculate the energy differences \( \Delta E \) for each transition provided.
3Step 3: Calculate Energy Difference for n=1 to n=3
The energy difference from \( n=1 \) to \( n=3 \) is given as corresponding to a wavelength of \( 102.6 \text{ nm} \). Calculate \( E_3 - E_1 \) as follows: \[ \Delta E_{1-3} = E_3 - E_1 = -\frac{13.6}{3^2} - \left(-\frac{13.6}{1^2} \right) = 12.09 \text{ eV} \]
4Step 4: Calculate Energy Difference for Other Transitions
Calculate the energy difference for each option: - **(a)** \( n=2 \) to \( n=4 \): \[ \Delta E_{2-4} = E_4 - E_2 = -\frac{13.6}{4^2} - -\frac{13.6}{2^2} = -0.85 \text{ eV} \] - **(b)** \( n=1 \) to \( n=4 \): \[ \Delta E_{1-4} = E_4 - E_1 = -\frac{13.6}{4^2} - -\frac{13.6}{1^2} = 12.75 \text{ eV} \] - **(c)** \( n=1 \) to \( n=5 \): \[ \Delta E_{1-5} = E_5 - E_1 = -\frac{13.6}{5^2} - -\frac{13.6}{1^2} = 13.06 \text{ eV} \] - **(d)** \( n=3 \) to \( n=5 \): \[ \Delta E_{3-5} = E_5 - E_3 = -\frac{13.6}{5^2} - -\frac{13.6}{3^2} = 1.55 \text{ eV} \]
5Step 5: Compare Energy Differences
To determine which transition requires a longer wavelength than \( 102.6 \text{ nm} \), find which has an energy difference smaller than \( 12.09 \text{ eV} \) (as longer wavelength means less energy). Transitions \( n=2 \) to \( n=4 \) and \( n=3 \) to \( n=5 \) have smaller energy differences (\( 0.85 \text{ eV} \) and \( 1.55 \text{ eV} \) respectively) than \( n=1 \) to \( n=3 \).
Key Concepts
Wavelength and Energy RelationshipQuantum TransitionsEnergy Level Calculations
Wavelength and Energy Relationship
Understanding the connection between wavelength and energy is essential when studying transitions in a hydrogen atom. In physics, energy (E) and wavelength (\lambda) are inversely related. This means that as the energy of a photon increases, its wavelength decreases, and vice versa. This relationship is mathematically described by the equation:
\[E = \frac{hc}{\lambda}\]where:
\[E = \frac{hc}{\lambda}\]where:
- \(E\) is the energy of the photon (in electron volts, eV).
- \(h\) is Planck's constant (6.626 \times 10^{-34} \text{ Js}).
- \(c\) is the speed of light in a vacuum (3.00 \times 10^8 \text{ m/s}).
- \(\lambda\) is the wavelength of the light (in meters).
Quantum Transitions
Quantum transitions in a hydrogen atom involve an electron moving between different energy levels. Each energy level is identified by a principal quantum number (
n
), which determines the size and energy of the orbital where the electron is likely to be found.
Electrons in the hydrogen atom can absorb or emit photons, allowing them to transition upward or downward between these quantized energy states. When a photon is absorbed, an electron jumps to a higher energy level; while when a photon is emitted, the electron drops to a lower energy level.
For example, moving an electron from the first energy level ( n=1 ) to the third ( n=3 ) requires energy absorption equaling the difference between these two states. Quantum theory describes this phenomenon with precise calculations, allowing us to predict which transitions would require shorter or longer wavelength radiation based on the energy differences.
Electrons in the hydrogen atom can absorb or emit photons, allowing them to transition upward or downward between these quantized energy states. When a photon is absorbed, an electron jumps to a higher energy level; while when a photon is emitted, the electron drops to a lower energy level.
For example, moving an electron from the first energy level ( n=1 ) to the third ( n=3 ) requires energy absorption equaling the difference between these two states. Quantum theory describes this phenomenon with precise calculations, allowing us to predict which transitions would require shorter or longer wavelength radiation based on the energy differences.
Energy Level Calculations
Calculating energy levels in a hydrogen atom involves understanding how much energy is associated with each quantum state. Each state is defined by its principal quantum number (n), and the energy for each level can be calculated using the formula:
\[E_n = -\frac{13.6}{n^2} \text{ eV}\]This formula highlights:
For example, for a transition from n=1 to n=3, we calculate:\[\Delta E_{1-3} = E_3 - E_1 = -\frac{13.6}{3^2} - \left(-\frac{13.6}{1^2} \right) = 12.09 \text{ eV}\]Understanding these calculations allows you to determine how much energy and what wavelength of radiation is necessary for specific electron transitions.
\[E_n = -\frac{13.6}{n^2} \text{ eV}\]This formula highlights:
- The energy of an electron at a given level (n) is negative—this reflects that energy must be added to free the electron.
- The lower the value of (n), the closer the electron is to the nucleus, and the more negative (or lower) the energy value becomes.
For example, for a transition from n=1 to n=3, we calculate:\[\Delta E_{1-3} = E_3 - E_1 = -\frac{13.6}{3^2} - \left(-\frac{13.6}{1^2} \right) = 12.09 \text{ eV}\]Understanding these calculations allows you to determine how much energy and what wavelength of radiation is necessary for specific electron transitions.
Other exercises in this chapter
Problem 17
Consider only transitions involving the \(n=1\) through \(n=5\) energy levels for the \(\mathrm{H}\) atom (see Figures 6.7 and 6.10) (a) How many emission lines
View solution Problem 19
The energy emitted when an electron moves from a higher energy state to a lower energy state in any atom can be observed as electromagnetic radiation. (a) Which
View solution Problem 21
Calculate the wavelength and frequency of light emitted when an electron changes from \(n=3\) to \(n=1\) in the H atom. In what region of the spectrum is this r
View solution Problem 22
Calculate the wavelength and frequency of light emitted when an electron changes from \(n=4\) to \(n=3\) in the H atom. In what region of the spectrum is this r
View solution