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Question

(a) Derive an expression for the angle between the vector representing angular momentum l with z-component m1=+lm_{1}=+l (that is, its maximum value) and the z-axis. What is this angle for l = 1 and for l = 5? (b) Derive an expression for the angle between the vector representing angular momentum l with z-component m1=+lm_{1}=+l and the z-axis. What value does this angle take in the limit that l becomes very large? Interpret your result in the light of the correspondence principle.

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(a)\textbf{(a)}

Expression for the angle between the vector representing angular momentum ll with z - component ml=+lm_l = + l (i.e. its maximum value) can be obtained from equation that defines angular momentum:

l=l(l+1)\begin{equation}|\vec{l}| = \sqrt{l (l + 1)}\hbar\end{equation}

and its projection on z - axis:

lz=ml,\begin{equation}l_z = m_l \hbar, \end{equation}

where ll is orbital quantum number (l=0,1,2,...n1l = 0,1,2,...n-1; n is principal quantum number), mlm_l magnetic orbital quantum number (ml=0,±1,±2,....,±lm_l = 0, \pm 1, \pm 2, ....,\pm l), =h2π\hbar = \dfrac{h}{2 \pi} (hh is Planck constant).

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