Review the key concepts, formulae, and examples before starting your quiz.
🔑Concepts
Bohr's second postulate states that the angular momentum of an electron orbiting the nucleus is quantized and can only take values that are integral multiples of .
Louis de Broglie provided a theoretical basis for this postulate by proposing that electrons in atoms behave like standing waves (stationary waves).
For an electron wave to be stable in a circular orbit of radius , the circumference of the orbit must be an integral multiple of its de Broglie wavelength .
If the circumference is not equal to , the wave would interfere with itself upon successive revolutions and eventually average out to zero.
The condition for a standing wave is , where represents the principal quantum number.
Substituting the de Broglie relation into the standing wave condition yields the quantization of angular momentum: .
📐Formulae
💡Examples
Problem 1:
Determine the number of de Broglie wavelengths associated with an electron revolving in the orbit of a hydrogen atom.
Solution:
According to de Broglie's explanation of Bohr's second postulate, the condition for a stable orbit is given by: For the orbit, the principal quantum number is . Substituting into the equation: Therefore, there are de Broglie wavelengths in the orbit.
Explanation:
In any orbit, the number of complete de Broglie wavelengths that fit into the circumference of the orbit is exactly equal to the principal quantum number .
Problem 2:
Show how the de Broglie hypothesis leads to the quantization of angular momentum for an electron in a circular orbit of radius .
Solution:
- Start with the standing wave condition for a circular orbit:
- Use the de Broglie relation for wavelength:
- Substitute the expression for into the first equation:
- Rearrange the terms to isolate angular momentum ():
- This is Bohr's quantization condition, where (with ).
Explanation:
By treating the electron as a wave, the requirement for constructive interference (standing wave) naturally results in the restriction of angular momentum to discrete values.