The photoelectric effect and the Compton effect both demonstrate the particle characteristics of a photon supporting the notion of wave-particle duality.  A natural consequence of this is to ask if a particle, such as an electron, could behave like a wave.  Louis de Broglie introduced this idea in 1923.  He proposed, based on Compton's findings, that matter-possessing momentum has a characteristic wavelength according to .

For an electron travelling much less than the speed of light, this equation becomes .

The first evidence of matter waves came several years later when physicists C.J. Davison and L.H. Germer accidentally discovered that a beam of electrons can create an interference pattern.  Ultimately, this discovery contributed to the development of the modern electron microscope.

 


Watch This
Watch the following short video of de Broglie's work. de Broglie Particle Wave Duality


Read
Read "Then, Now and Future, The Electron Microscope" on page 727 and "De Broglie's Wave Hypothesis: Strange but True!" on page 729 of your physics textbook.


As you discovered in the reading about electron microscopes, the magnification of a microscope depends on the inverse of the wavelength that produces the image.  The electron microscope is able to generate matter waves with wavelengths much smaller than that of visible light, leading to greater magnification as you can see in the picture of the fly's eye to the right.

 

Example Problem 1.  

What is the wavelength of an electron with a speed of 5.50 × 10 6  m/s?  How many times smaller is this wavelength compared to a 400-nm violet light?

 

Hint:  When asked to compare two quantities, answer by stating how many times larger or smaller one quantity is relative to the other.

© Musem of Science, Boston

Given

 

Required

the wavelength of the electron and the ratio of the wavelengths of the electron and violet light

 

Analysis and Solution

 

Paraphrase

The wavelength of the electron is 1.32 × 10 -10 m, and it is 3.03 × 10 3 times smaller than the wavelength of violet light.

Example Problem 2

What is the wavelength of an electron that has a kinetic energy of 3.10 × 10 -16 J?


Given

 

Required

the wavelength of the electron

 

Analysis and Solution

 

Paraphrase
The wavelength of the electron is 2.79 × 10 -11 m.

 

 
Self-Check

Answer the following self-check (SC) questions then click the "Check your work" bar to assess your responses.

 

 

SC 3.

What is the wavelength of an electron that has a speed of 2.25 × 10 7 m/s?

 

SC 4. 

What is the wavelength of an electron that has a kinetic energy of 7.2 × 10 -4 MeV?

 

SC 5.

What is the speed of an electron that has a wavelength of 7.00 pm?

 

SC 6.
What is the wavelength of an electron that is accelerated from rest through a potential difference of 1000 V?

 

   Self-Check Answer

Contact your teacher if your answers vary significantly from the answers provided here.

 

SC 3.

 

Given

 

Required

the wavelength of the electron

 

Analysis and Solution

 

Paraphrase

The wavelength of the electron is 3.23 × 10 -11  m.

 

SC 4.

 

Given

 

Required

the wavelength of the electron

 

Analysis and Solution

Change the energy in eV to J

 

 

Use the kinetic energy to find the velocity.

 

 

Use the velocity to find the wavelength.

 

 

Paraphrase

The wavelength of the electron is 4.58 × 10 -11  m.

 

SC 5.

 

Given

 

Required

the velocity of the electron

 

Analysis and Solution

 

Paraphrase

The speed of the electron is 1.04 × 10 8  m/s.

 

SC 6


Given

V  = 1000 V

 

Required

the wavelength of the electron

 

Analysis and Solution

Calculate the change in energy (or work done) of the electron.

 

 

Calculate the velocity using  Ek=12mv2 .

 

 

Calculate the wavelength.

 

 

Paraphrase

The wavelength of the electron is 3.88 × 10 -11  m.



Read
Read "De Broglie's Hypothesis-A Key Concept of Quantum Physics" and "Heisenberg's Uncertainty Principle" on pages 730 to 735 of the textbook.



Heisenberg's uncertainty principle:  a principle stating that it is impossible to know both the position and momentum of a particle with unlimited precision at the same time