\(\frac{nh}{2πr}\)
\(\frac{nh}{2r}\)
\(\frac{nh}{2\pi}\)
\(\frac{2πr}{nh}\)
To find the expression for the momentum of an electron revolving in the nth orbit, we start by understanding the basic principles of atomic structure, particularly focusing on Bohr's model of the atom.
According to Bohr's postulate for quantized angular momentum, the angular momentum (L) of an electron in the nth orbit is given by:
L = n\hbar
where \hbar is the reduced Planck's constant: \hbar = \frac{h}{2\pi}, and n is the principal quantum number.
Since the angular momentum (L) is also expressed as the product of linear momentum (p) and radius (r) of the orbit, we have:
L = p \cdot r
Equating the two expressions for angular momentum, we get:
p \cdot r = n\hbar
Substituting the value of \hbar, we get:
p \cdot r = n \cdot \frac{h}{2\pi}
Solving for the linear momentum (p):
p = \frac{n \cdot h}{2\pi r}
This shows that the momentum of an electron revolving in the nth orbit is given by: \(\frac{nh}{2\pi r}\), which matches the correct answer option.
Conclusion: The correct expression for the momentum of an electron in the nth orbit is \(\frac{nh}{2\pi r}\). This expression adheres to the Bohr model by quantifying the orbit characteristics and aligning with the angular momentum quantization rule.
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: