The de Broglie wavelength of an electron is a concept that arises from the wave-particle duality, which is a cornerstone of quantum mechanics. According to this principle, every particle, including electrons, can exhibit both particle-like and wave-like properties. The idea was proposed by Louis de Broglie in 1924, and it helps explain phenomena such as interference and diffraction, which are typically associated with waves, but also occur with particles like electrons.
### Formula for de Broglie Wavelength
The de Broglie wavelength (\(\lambda\)) of a particle is related to its momentum (\(p\)) by the following equation:
\[
\lambda = \frac{h}{p}
\]
where:
- \(\lambda\) is the de Broglie wavelength,
- \(h\) is Planck’s constant (\(6.626 \times 10^{-34} \, \text{J·s}\)),
- \(p\) is the momentum of the particle.
The momentum of a particle is the product of its mass (\(m\)) and velocity (\(v\)):
\[
p = mv
\]
So, the de Broglie wavelength of an electron can also be written as:
\[
\lambda = \frac{h}{mv}
\]
where:
- \(m\) is the mass of the electron (approximately \(9.11 \times 10^{-31} \, \text{kg}\)),
- \(v\) is the velocity of the electron.
### Practical Example
If you want to calculate the de Broglie wavelength of an electron, you need to know its velocity. Let’s calculate it for an electron moving at a typical speed in a cathode ray tube, where its velocity might be around \(v = 1.0 \times 10^6 \, \text{m/s}\).
- Planck's constant: \(h = 6.626 \times 10^{-34} \, \text{J·s}\),
- Electron mass: \(m = 9.11 \times 10^{-31} \, \text{kg}\),
- Electron velocity: \(v = 1.0 \times 10^6 \, \text{m/s}\).
Using the formula for de Broglie wavelength:
\[
\lambda = \frac{6.626 \times 10^{-34}}{(9.11 \times 10^{-31})(1.0 \times 10^6)}
\]
Now, let's calculate it:
\[
\lambda \approx \frac{6.626 \times 10^{-34}}{9.11 \times 10^{-25}} \approx 7.27 \times 10^{-10} \, \text{m}
\]
This gives a wavelength of approximately \(7.27 \times 10^{-10} \, \text{m}\), or about \(0.727 \, \text{nm}\), which is in the range of X-rays.
### Conclusion
The de Broglie wavelength of an electron depends on its velocity. In everyday scenarios where electrons move at high speeds, the wavelength can be extremely small, often in the nanometer or even picometer range. This small wavelength is what allows electrons to exhibit wave-like properties like interference and diffraction, which are key to many phenomena in quantum mechanics, including the functioning of electron microscopes.