Find Approx Wavelength of Titanium Kbeta X-Rays

In summary, the conversation discusses finding the approximate wavelength of K-beta X-rays emitted by titanium. The homework equations involve determining energy levels and the effective nuclear charge for an electron in the n=3 and n=1 shells. The conversation also addresses the question of whether one or more electrons move up energy levels in an excited state.
  • #1
negatifzeo
66
0

Homework Statement


The X-ray spectrum for a typical metal is shown in Figure 31-22. Find the approximate wavelength of Kbeta X-rays emitted by titanium. (Hint: An electron in the M shell is shielded from the nucleus by the single electron in the K shell, plus all the electrons in the L shell.)
(The figure seems irrelevant to me, no useful data is privded by it, it's just a graph with no labels.)

Homework Equations





The Attempt at a Solution



I don't really know what to do here, there's several things I don't understand. I believe that K-beta X-rays are emitted when the electron drops from the 3rd excited state to the ground level. But how do you determine the energy level difference here? And when Titanium is in an "excited" state, does that mean that just one electron moved up 3 levels, or more than one? Any help in explaining this would be greatly appreciated.
 
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  • #2
Hi negatifzeo,

That's right; in this case, there is only one electron in the n=1 shell, and one of the electrons that is in the n=3 shell is dropping to fill the n=1 shell.

If this was a hydrogenic titanium atom with only one electron, and the electron was making a transition from n=3 to n=1, the energy levels would be found from:

[tex]
E_n = -Z^2 \frac{13.6\mbox{ eV}}{n^2}
[/tex]

If the atom is not hydrogenic, then the equation above has to modified to account for the other electrons. The inner electrons will partly shield the nuclear charge. We account for this in the above equation by changing [itex]Z\to Z_{\rm eff}[/itex], where [itex]Z_{\rm eff}[/itex] is called the effective nuclear charge.

So mostly what this problem is about is that you need to find the effective Z values for an electron in the n=3 shell and for an electron in the n=1 shell of titanium.

Does this help?
 
  • #3


Dear student,

Thank you for your question. I understand that this may seem confusing at first, but let me try to break it down for you.

Firstly, the figure provided is a graph of the X-ray spectrum for a typical metal. This means that it shows the different energies of X-rays emitted by a metal. The x-axis represents the wavelength (in nanometers) and the y-axis represents the intensity of the X-rays.

Now, let's focus on the Kbeta X-rays emitted by titanium. As you correctly stated, these X-rays are emitted when an electron in the M shell drops down to the K shell. However, in order for this to happen, the M shell electron must first be excited to a higher energy level. This can happen through various processes, such as collisions with other particles or absorption of energy.

When an electron is excited, it moves to a higher energy level. In the case of titanium, the Kbeta X-rays are emitted when an electron in the M shell drops down to the K shell. This means that the electron has moved from the third excited state to the ground state. The energy level difference between these two states can be calculated using the equation:

ΔE = E3 - E1 = (13.6 eV) * (Z^2 / n^2) * (1/n1^2 - 1/n2^2)

where Z is the atomic number (22 for titanium), n is the principal quantum number (3 for the third excited state and 1 for the ground state), and n1 and n2 are the quantum numbers of the initial and final states, respectively.

Once you have calculated the energy level difference, you can use the equation:

E = hc/λ

where E is the energy of the X-ray, h is Planck's constant, c is the speed of light, and λ is the wavelength of the X-ray.

I hope this helps to clarify things for you. If you have any further questions, please don't hesitate to ask. Good luck with your homework!
 

What is the purpose of finding the approximate wavelength of Titanium Kbeta X-Rays?

The purpose of finding the approximate wavelength of Titanium Kbeta X-Rays is to determine the energy levels and atomic structure of Titanium atoms. This information can be used in various fields such as material science, chemistry, and physics.

How is the wavelength of Titanium Kbeta X-Rays determined?

The wavelength of Titanium Kbeta X-Rays is determined by using a spectrometer, which measures the diffraction pattern of the X-Rays. The spacing between the diffraction peaks can then be used to calculate the wavelength.

What factors can affect the accuracy of the approximate wavelength measurement?

The accuracy of the approximate wavelength measurement can be affected by factors such as the quality of the spectrometer, the purity of the Titanium sample, and any external interference or noise.

Why is Titanium used to generate X-Rays?

Titanium is commonly used to generate X-Rays because it has a high atomic number, making it effective in producing X-Rays with a high energy level. It is also readily available and relatively inexpensive compared to other elements.

How is the approximate wavelength of Titanium Kbeta X-Rays used in practical applications?

The approximate wavelength of Titanium Kbeta X-Rays can be used in practical applications such as non-destructive testing, medical imaging, and X-Ray diffraction analysis in material science. It can also help in the development of new technologies and materials.

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