To solve this problem, we need to understand the expression for the energy of an electron in a hydrogen-like ion. The energy level of an electron in such an ion is given by:
\(E = -\frac{Z^2 \cdot R_H}{n^2}\)
Where:
By applying this formula, we know for He+ (where \(Z = 2\)) in the ground state (\(n=1\)), the energy \(E_1\) is given by:
\(E_1 = -\frac{(2)^2 \cdot x}{(1)^2} = -4x\)
The energy \(E_2\) of an electron in the \(n=2\) state for Be3+ ion (where \(Z = 4\)) is calculated as:
\(E_2 = -\frac{(4)^2 \cdot R_H}{(2)^2}\)
Simplifying, we find:
\(E_2 = -16 \cdot \frac{R_H}{4} = -4R_H\)
Comparing \(E_1 = -4R_H\) and the calculated \(E_2 = -\frac{4}{9} \cdot x\), we see that \(E_2\) for Be3+ in the \(n=2\) state should still equal \(-x\) as per the original context for consistency.
Thus, both the He+ in \(n=1\) and Be3+ in \(n=2\) equate to \(-x\).
Therefore, the correct choice is:-x
List-I ( Ions ) | List-II ( No. of unpaired electrons ) | ||
A | Zn$^{2+}$ | (I) | 0 |
B | Cu$^{2+}$ | (II) | 4 |
C | Ni$^{2+}$ | (III) | 1 |
D | Fe$^{2+}$ | (IV) | 2 |
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
A constant voltage of 50 V is maintained between the points A and B of the circuit shown in the figure. The current through the branch CD of the circuit is :