Step 1: Understanding the Concept:
This question relates to Bohr's model of the hydrogen atom, specifically his second postulate, which deals with the quantization of angular momentum. According to Bohr, an electron can only revolve in certain stable orbits where its angular momentum is an integral multiple of a fundamental unit.
Step 2: Key Formula or Approach:
Bohr's quantization condition for the angular momentum (\(L_n\)) of an electron in the \(n^{th}\) orbit is given by:
\[ L_n = n \frac{h}{2\pi} \]
where \(n\) is the principal quantum number (\(n = 1, 2, 3, \ldots\)) and \(h\) is Planck's constant.
Step 3: Detailed Explanation:
We need to find the difference in angular momentum between two successive orbits. Let's consider two consecutive orbits with principal quantum numbers \(n\) and \(n+1\).
The angular momentum in the \((n+1)^{th}\) orbit is:
\[ L_{n+1} = (n+1) \frac{h}{2\pi} \]
The angular momentum in the \(n^{th}\) orbit is:
\[ L_n = n \frac{h}{2\pi} \]
The difference (\(\Delta L\)) between them is:
\[ \Delta L = L_{n+1} - L_n = (n+1) \frac{h}{2\pi} - n \frac{h}{2\pi} \]
\[ \Delta L = \left( (n+1) - n \right) \frac{h}{2\pi} \]
\[ \Delta L = (1) \frac{h}{2\pi} = \frac{h}{2\pi} \]
The difference is constant and independent of \(n\).
Step 4: Final Answer:
The difference in angular momentum between any two successive orbits is \(\frac{h}{2\pi}\). This is also often written as \(\hbar\) (h-bar). Therefore, option (A) is correct.
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