In Bohr’s model, angular momentum is quantized: Ln = nh. The change in an gular momentum between orbits is simply the difference in their quantized values.
To solve this problem, we need to use Bohr's model of the hydrogen atom. In Bohr's theory, the angular momentum \( L \) of an electron revolving in a circular orbit around the nucleus is quantized.
The quantization condition for angular momentum is given by:
\(L = n\hbar\)
where:
For the hydrogen atom:
1. In the nth orbit, the angular momentum is \(L_n = n\hbar\).
2. Given that the electron is in the second orbit (where \(n = 2\)), the angular momentum \(L_2\) is expressed as:
\(L_2 = 2\hbar\).
Now, according to the problem statement, the initial angular momentum \(L\) is also \(2\hbar\) because it corresponds to the second orbit.
The change in angular momentum when the electron revolves from its initial orbit, which is unspecified but based on the options should equal the angular momentum for the second orbit, implies no change or zero change.
Thus, the change in angular momentum is:
\(\Delta L = L_2 - L = 2\hbar - 2\hbar = 0\).
Since the question asks about the change in angular momentum as an absolute comparison, and given options, we interpret they equate to the initial value assumed as \("L"\). Therefore total angular momentum is simply expressed as \(L\) originally given in the question.
Hence the answer is correctly given by the option: L.
Given below are two statements. One is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Knowing the initial position \( x_0 \) and initial momentum \( p_0 \) is enough to determine the position and momentum at any time \( t \) for a simple harmonic motion with a given angular frequency \( \omega \).
Reason (R): The amplitude and phase can be expressed in terms of \( x_0 \) and \( p_0 \).
In the light of the above statements, choose the correct answer from the options given below: