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The sodium D-lines, two very distinct lines of yellow light emitted by heated sodium metal, are often used in the calibration of spectrometers. The wavelength of one of these lines is \(5890 \AA\). How much energy does an electron emit (or absorb) in undergoing the electronic transition associated with this line?

Short Answer

Expert verified
The energy emitted or absorbed by an electron during the electronic transition associated with the given sodium D-line is approximately \(3.377 \times 10^{-19}\) joules.

Step by step solution

01

Convert given wavelength to meters

The provided wavelength is in angstroms (Å). We need to convert it to meters to work with SI units: 1 Å = \(1 \times 10^{-10}\) m Given wavelength λ = 5890 Å = \(5890 \times 10^{-10}\) m
02

Calculate frequency

Using the speed of light formula, we solve for frequency: \(c = \lambda \cdot f\) Rearrange the formula for frequency (f): \(f = \frac{c}{\lambda}\) Plugging in the values: - Speed of light (c) = \(3.0 \times 10^8\) m/s - Wavelength (λ) = \(5890 \times 10^{-10}\) m \(f = \frac{3.0 \times 10^8}{5890 \times 10^{-10}}\) Frequency (f) = \(5.093 \times 10^{14}\) Hz
03

Calculate energy difference

Now that we have the frequency, we can calculate the energy difference using the energy formula: \(E = h \cdot f\) Plugging in the values: - Planck's constant (h) = \(6.626 \times 10^{-34}\) J·s - Frequency (f) = \(5.093 \times 10^{14}\) Hz \(E = (6.626 \times 10^{-34}) (5.093 \times 10^{14})\) Energy (E) = \(3.377 \times 10^{-19}\) J The energy emitted or absorbed by an electron during the electronic transition associated with the given sodium D-line is approximately \(3.377 \times 10^{-19}\) joules.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Spectrometer Calibration
Calibration of a spectrometer is crucial to ensure its measurements are accurate and reliable. When using sodium D-lines, these lines are distinct and occur naturally at specific known wavelengths. This is why they serve as ideal reference points for calibration.
The sodium D-line at 5890 Å is particularly useful. By calibrating a spectrometer with this specific line, the device can maintain a high level of precision in identifying other spectral lines.
  • Provides benchmark for accurate measurement
  • Ensures data reliability in experiments
  • Makes identification of unknown lines more precise

Precision in calibration ultimately affects the outcomes of any experiment relying on spectrometer readings, ensuring that scientists and researchers can trust the data they collect.
Wavelength Conversion
Converting wavelength measurements from angstroms to meters is necessary for working within the International System of Units (SI). Angstroms are often used for their convenience at the atomic scale, but meters are the standard.
To convert the sodium D-line from angstroms (Å) to meters (m), you remember that \(1 \, \text{Å} = 1 \times 10^{-10} \, \text{m}\). Thus, 5890 Å becomes \(5890 \times 10^{-10}\ m\).
  • Helps use consistent units in calculations
  • Ensures compatibility with other measurement units
  • Aligns with standard scientific practices

This conversion makes it easier to apply physical constants like the speed of light \(c = 3.0 \times 10^8\, \text{m/s}\).
Frequency Calculation
Frequency represents how often a wave passes a specific point in one second and is calculated using the speed of light and the wavelength. This involves the formula:\[f = \frac{c}{\lambda}\]
Here, the speed of light \(c\) is \(3.0 \times 10^8\, \text{m/s}\) and \(\lambda\) is \(5890 \times 10^{-10}\, \text{m}\). Solving gives a frequency \(f\) of \(5.093 \times 10^{14}\, \text{Hz}\).
  • Indicates light's cycles per second
  • Crucial for further energy calculations
  • Related directly to energy in quantum mechanics

Converting between wavelength and frequency is vital in many areas of science, such as quantum mechanics and optics.
Energy Transition
In atomic physics, energy transitions indicate an electron moving between energy levels, emitting or absorbing energy. For the sodium D-line, the energy difference can be calculated with:\[E = h \cdot f\]
This uses Planck's constant \(h = 6.626 \times 10^{-34}\, \text{J·s}\), and the frequency \(f = 5.093 \times 10^{14}\, \text{Hz}\), giving energy \(E = 3.377 \times 10^{-19}\, \text{J}\).
  • Explains phenomena like light emission and absorption
  • Shows quantum level energy interactions
  • Key in understanding spectroscopic data

Energy transitions provide the foundation for interpreting spectral lines in terms of underlying atomic processes.
Planck's Constant
Planck's constant is a fundamental physical constant essential for describing the particles at the quantum level. It bridges the concepts of wave and particle nature of light and relates to energy (\(E\)) and frequency (\(f\)) through\[E = h \cdot f\].
It is valued at \(6.626 \times 10^{-34}\, \text{J·s}\), illustrating how small energy quantities are involved at the atomic level.
  • Key to quantum mechanics
  • Used in calculations of photon energy
  • Integral in wave-particle duality discussion

Ultimately, Planck's constant helps provide a deeper understanding of how energy operates within the quantum realm, reinforcing the discrete nature of electronic transitions.

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Most popular questions from this chapter

The Rydberg - Ritz equation governing the spectral lines of hydrogen is \((1 / \lambda)=\mathrm{R}\left[\left(1 / \mathrm{n}_{1}{ }^{2}\right)-\left(1 / \mathrm{n}_{2}{ }^{2}\right)\right]\), where \(\mathrm{R}\) is the Rydberg constant, \(\mathrm{n}_{1}\) indexes the series under consideration \(\left(\mathrm{n}_{1}=1\right.\) for the Lyman series, \(\mathrm{n}_{1}=2\) for the Balmer series, \(\mathrm{n}_{1}=3\) for the Paschen series \(), \mathrm{n}_{2}=\mathrm{n}_{1}+1, \mathrm{n}_{1}+2, \mathrm{n}_{1}+3, \ldots\) indexes the successive lines in a series, and \(\lambda\) is the wave- length of the line corresponding to index \(\mathrm{n}_{2}\). Thus, for the Lyman series, \(\mathrm{n}_{1}=1\) and the first two lines are \(1215.56 \AA\left(\mathrm{n}_{2}=\mathrm{n}_{1}+1=2\right)\) and \(1025.83 \AA\left(\mathrm{n}_{2}=\mathrm{n}_{1}+2=3\right)\) Using these two lines, calculate two separate values of the Rydberg constant. The actual value of this constant is \(\mathrm{R}=109678 \mathrm{~cm}^{-1}\)

Consider an atom containing one electron and having an atomic number \(Z\). It is observed that light of a wavelength of \(0.1 \mathrm{~nm}\) will excite this atom from the ground state to infinite ionization. Determine the value of \(Z\).

The flame test for barium involves placing a barium-containing compound in a Bunsen burner flame. The barium compound then decomposes to give barium atoms which subsequently undergo an electronic transition of energy \(3.62 \times 10^{-12} \mathrm{erg} .\) What color flame would this give rise to?

Wave number ( \(\mathrm{v}\) ) are the reciprocals of wavelengths, \(\lambda\) and are given by the expression \(\bar{v}=1 / \lambda\). For the hydrogen atom, the Bohr theory predicts that the wave number for the emission line associated with an electronic transition from the energy level having principal quantum number \(\mathrm{n}_{2}\) to that with principal quantum number \(\mathrm{n}_{1}\) is \(\bar{v}=R_{H}\left[\left(1 / n_{1}^{2}\right)-\left(1 / n_{2}^{2}\right)\right]\) where \(\mathrm{R}_{\mathrm{H}}\) is the Rydberg constant. In what region of the electromagnetic spectrum would there appear a spectral line resulting from the transition from the tenth to the fifth electronic level in hydrogen?

The atomic radius of hydrogen is \(0.037 \mathrm{~nm}\), Compare this figure with the length of the first Bohr radius. Explain any differences.

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