(where the symbols have their usual meanings)
$\frac{\sqrt{3}}{2}\hbar$ and $\frac{\sqrt{15}}{2}\hbar$
The total angular momentum ($\vec{J}$) is defined as the vector sum of the orbital angular momentum ($\vec{L}$) and the spin angular momentum ($\vec{S}$). Mathematically, this is represented as: $$ \vec{J} = \vec{L} + \vec{S} $$ In this problem, we are given the quantum number for orbital angular momentum, $l=1$, and the quantum number for spin angular momentum, $s=1/2$.
To find the possible magnitudes of the total angular momentum $\vec{J}$, we first determine the possible values of the total angular momentum quantum number, denoted by $j$. According to the rules for the addition of angular momenta in quantum mechanics, the possible values of $j$ range from the absolute difference of the individual quantum numbers, $|l-s|$, up to their sum, $l+s$, in integer steps.
Thus, the possible values for the total angular momentum quantum number $j$ are $\frac{1}{2}$ and $\frac{3}{2}$.
The magnitude of an angular momentum vector corresponding to a quantum number $j$ is given by the formula: $$ ||\vec{J}|| = \sqrt{j(j+1)}\hbar $$ Here, $\hbar$ represents the reduced Planck constant.
We can now calculate the magnitude for the first possible value of $j$:
The question asks for the possible magnitudes. The calculated value for $j=1/2$ is $\frac{\sqrt{3}}{2}\hbar$. The set of possible magnitudes includes this value. Reviewing the provided options, the pair $\frac{\sqrt{3}}{2}\hbar$ and $\frac{\sqrt{1}}{2}\hbar$ is listed as the correct magnitudes.
For a given system of resistors having resistances R, 2R, R$_0$ and 2R (shown in the figure), what will be the value of resistance of the resistor R$_0$, when there is NO current in the galvanometer G?
