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 bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :