De Broglie proposed that electrons travel through space as a wave
This would explain why they can exhibit behaviour such as diffraction
He therefore suggested that electrons must also hold wave properties, such as wavelength
This became known as the de Broglie wavelength
However, he realised all particles can show wave-like properties, not just electrons
So, the de Broglie wavelength can be defined as:
The wavelength associated with a moving particle
The majority of the time, and for everyday objects travelling at normal speeds, the de Broglie wavelength is far too small for any quantum effects to be observed
A typical electron in a metal has a de Broglie wavelength of about 10 nm
Therefore, quantum mechanical effects will only be observable when the width of the sample is around that value
The electron diffraction tube can be used to investigate how the wavelength of electrons depends on their speed
The smaller the radius of the rings, the smaller the de Broglie wavelength of the electrons
As the voltage is increased:
The energy of the electrons increases
The radius of the diffraction pattern decreases
This shows as the speed of the electrons increases, the de Broglie wavelength of the electrons decreases
Calculating de Broglie Wavelength
Using ideas based upon the quantum theory and Einstein’s theory of relativity, de Broglie suggested that the momentum (p) of a particle and its associated wavelength (λ) are related by the equation:
Since momentum p = mv, the de Broglie wavelength can be related to the speed of a moving particle (v) by the equation:
Since kinetic energy E = ½ mv2
Momentum and kinetic energy can be related by:
Combining this with the de Broglie equation gives a form which relates the de Broglie wavelength of a particle to its kinetic energy:
Where:
λ = the de Broglie wavelength (m)
h = Planck’s constant (J s)
p = momentum of the particle (kg m s-1)
E = kinetic energy of the particle (J)
m = mass of the particle (kg)
v = speed of the particle (m s-1)
Worked Example
A proton and an electron are each accelerated from rest through the same potential difference.