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An x ray with a wavelength of 0.100 nm collides with an electron that is initially at rest. The x ray's final wavelength is 0.110 nm. What is the final kinetic energy of the electron?

Short Answer

Expert verified
The electron's final kinetic energy is the difference between the initial and final x-ray energies.

Step by step solution

01

Understanding the Problem

This problem involves Compton scattering, where an x-ray photon collides with a stationary electron, and the wavelength of the photon increases after the collision. We need to find the kinetic energy of the electron after the collision.
02

Identifying Given Values and Formulas

We have the initial wavelength of the x-ray, \(\lambda_i = 0.100\, \text{nm}\), and the final wavelength of the x-ray, \(\lambda_f = 0.110\, \text{nm}\). The change in wavelength \(\Delta \lambda\) is given by the formula: \[ \Delta \lambda = \lambda_f - \lambda_i = 0.110\, \text{nm} - 0.100\, \text{nm} = 0.010\, \text{nm} = 0.010 \times 10^{-9}\, \text{m}.\]
03

Using Compton's Wavelength Shift Formula

Compton's formula for the change in wavelength is: \[ \Delta \lambda = \frac{h}{m_e c} (1 - \cos \theta), \] where \(h\) is Planck's constant, \(m_e\) is the electron's rest mass, and \(c\) is the speed of light. Substituting the values, \(\Delta \lambda = 0.010 \times 10^{-9} \text{ m}\).
04

Solving for the Scattering Angle \(\theta\)

Using \( \Delta \lambda = 0.010 \times 10^{-9} \text{ m} = \frac{h}{m_e c} (1 - \cos \theta) \), we need to determine \(\theta\) first. However, solving for \(\theta\) usually isn't necessary if directly targeting kinetic energy. Let's use the energy perspective next.
05

Calculating the Energy Change of the Photon

The energy of a photon is given by \( E = \frac{hc}{\lambda} \). The initial energy of the x-ray is \( E_i = \frac{hc}{\lambda_i} \) and the final energy is \( E_f = \frac{hc}{\lambda_f} \). Substitute \(h = 6.626 \times 10^{-34} \text{ Js}\), \(c = 3 \times 10^8 \text{ m/s}\) to calculate these energies.
06

Calculate the Initial and Final Photon Energies

The initial energy of the photon: \( E_i = \frac{6.626 \times 10^{-34} \times 3 \times 10^8}{0.100 \times 10^{-9}} \text{ J}. \)The final energy of the photon: \( E_f = \frac{6.626 \times 10^{-34} \times 3 \times 10^8}{0.110 \times 10^{-9}} \text{ J}. \)
07

Calculate the Change in Photon's Energy

The change in energy \( \Delta E = E_i - E_f \). Compute this energy difference to determine the kinetic energy gained by the electron, since energy is transferred from photon to electron.
08

Converting Energy to Electron's Kinetic Energy

The kinetic energy of the electron is equivalent to the decrease in the x-ray photon energy: \( KE = \Delta E \). Calculate \(\Delta E\) using the results from Step 6.

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Key Concepts

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

Wavelength Shift
In the context of Compton scattering, the wavelength shift refers to the change in wavelength of a photon, such as an x-ray, after it scatters off an electron. When the photon collides with a stationary electron, part of its energy is transferred to the electron.
This causes the photon to lose some of its initial energy, leading to an increased wavelength. This phenomenon is quantified using the change in wavelength, \( \Delta \lambda \).
The formula for the wavelength shift is: \[ \Delta \lambda = \lambda_f - \lambda_i \] where \( \lambda_i \) is the initial wavelength, and \( \lambda_f \) is the final wavelength of the photon.
In Compton's formula, the shift is given by: \[ \Delta \lambda = \frac{h}{m_e c} (1 - \cos \theta) \] where \( h \) is Planck's constant, \( m_e \) is the electron rest mass, \( c \) is the speed of light, and \( \theta \) is the scattering angle.
This shift directly correlates to the energy transferred to the electron, which is key to determining the electron's kinetic energy after such a collision.
Kinetic Energy
Kinetic energy is the energy an object possesses due to its motion. In the case of Compton scattering, the electron initially at rest gains kinetic energy from the x-ray photon. This transfer of energy results from the reduction in the photon's energy, which is then utilized to move the electron.
To find the kinetic energy of the electron, note that it is equivalent to the energy lost by the photon. The energy of a photon is inversely proportional to its wavelength, so when the photon loses energy, its wavelength increases.
The change in the photon's energy, \( \Delta E \), corresponds directly to the kinetic energy gained by the electron. By calculating the initial \( E_i \) and final \( E_f \) energies of the photon using their respective wavelengths, you can determine the kinetic energy as follows: \[ KE = \Delta E = E_i - E_f \]
This relationship highlights the fundamental principles of energy conservation in particle physics, where the lost photon energy becomes the kinetic energy of the electron.
Photon Energy
The energy of a photon is a crucial aspect of understanding Compton scattering. Photons are packets of light energy, and their energy is directly related to their wavelength. The energy, \( E \), of a photon is expressed using Planck's principle: \[ E = \frac{hc}{\lambda} \]
Here, \( h \) is Planck's constant, and \( \lambda \) is the wavelength of the photon, while \( c \) stands for the speed of light. Since photon energy is inversely proportional to wavelength, a shorter wavelength means higher energy, and vice versa.
During Compton scattering, the x-ray photon initially has a high energy and short wavelength (\( \lambda_i \)). After colliding with an electron, some of this energy is lost, resulting in a longer wavelength (\( \lambda_f \)). By calculating the initial and final energies: \[ E_i = \frac{hc}{\lambda_i} \] \[ E_f = \frac{hc}{\lambda_f} \]
We can find the change in energy \( \Delta E = E_i - E_f \), which represents the amount of energy transferred to the electron.
Planck's Constant
Planck's constant is a fundamental physical constant that plays a central role in quantum mechanics. Denoted by \( h \), its value is approximately \( 6.626 \times 10^{-34} \) joule seconds. This constant is crucial in explaining how energy is quantized, particularly in the realm of particles such as photons.
In Compton scattering, Planck's constant relates the energy of a photon to its frequency or its wavelength. The energy relationship is expressed as: \[ E = \frac{hc}{\lambda} \]
This dependency indicates that small changes in wavelength result in significant changes in energy at the quantum level. Understanding this relationship helps illustrate why photons, which follow the principles outlined by Planck's constant, behave the way they do in scattering interactions.
As photons scatter, and their energy changes, Planck's constant ensures that these changes follow a predictable and quantifiable pattern. This keeps the behavior of light consistent with observed quantum phenomena.

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Most popular questions from this chapter

Consider Compton scattering of a photon by a \(moving\) electron. Before the collision the photon has wavelength \(\lambda\) and is moving in the +\(x\)-direction, and the electron is moving in the -\(x\)-direction with total energy \(E\) (including its rest energy \(mc^2\)). The photon and electron collide head-on. After the collision, both are moving in the -\(x\)-direction (that is, the photon has been scattered by 180\(^\circ\)). (a) Derive an expression for the wavelength \(\lambda'\) of the scattered photon. Show that if \(E \gg mc^2\), where m is the rest mass of the electron, your result reduces to $$\lambda' = {hc \over E} (1 + {m^2c^4\lambda \over 4hcE}) $$ (b) A beam of infrared radiation from a CO\(_2\) laser (\(\lambda = 10.6 \mu{m}\)) collides head-on with a beam of electrons, each of total energy \(E\) = 10.0 GeV (1 GeV = 10\(^9\) eV). Calculate the wavelength \(\lambda'\) of the scattered photons, assuming a 180\(^\circ\) scattering angle. (c) What kind of scattered photons are these (infrared, microwave, ultraviolet, etc.)? Can you think of an application of this effect?

Protons are accelerated from rest by a potential difference of 4.00 kV and strike a metal target. If a proton produces one photon on impact, what is the minimum wavelength of the resulting x rays? How does your answer compare to the minimum wavelength if 4.00-keV electrons are used instead? Why do x-ray tubes use electrons rather than protons to produce x rays?

If a photon of wavelength 0.04250 nm strikes a free electron and is scattered at an angle of 35.0\(^\circ\) from its original direction, find (a) the change in the wavelength of this photon; (b) the wavelength of the scattered light; (c) the change in energy of the photon (is it a loss or a gain?); (d) the energy gained by the electron.

Higher-energy photons might be desirable for the treatment of certain tumors. Which of these actions would generate higher-energy photons in this linear accelerator? (a) Increasing the number of electrons that hit the tungsten target; (b) accelerating the electrons through a higher potential difference; (c) both (a) and (b); (d) none of these.

(a) If the average frequency emitted by a 120-W light bulb is 5.00 \(\times\) 10\(^{14}\) Hz and 10.0\(\%\) of the input power is emitted as visible light, approximately how many visible-light photons are emitted per second? (b) At what distance would this correspond to 1.00 \(\times\) 10\(^{11}\) visible-light photons per cm\(^2\) per second if the light is emitted uniformly in all directions?

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