| List-I (Element) | List-II (Electronic Configuration) |
|---|---|
| A. N | I. [Ar] 3d10 4s2 4p5 |
| B. S | II. [Ne] 3s2 3p4 |
| C. Br | III. [He] 2s2 2p3 |
| D. Kr | IV. [Ar] 3d10 4s2 4p6 |
The question requires matching elements with their respective electronic configurations. Let's analyze each element's correct electronic configuration to identify the correct match.
From the analysis above, the correct matching is:
| List-I (Element) | List-II (Electronic Configuration) |
|---|---|
| A. N | III. [He] 2s2 2p3 |
| B. S | II. [Ne] 3s2 3p4 |
| C. Br | I. [Ar] 3d10 4s2 4p5 |
| D. Kr | IV. [Ar] 3d10 4s2 4p6 |
Thus, the correct answer is: A-III, B-II, C-I, D-IV.
Let us match the electronic configurations:
A. N (Nitrogen):} Nitrogen has the electronic configuration $1s^2 2s^2 2p^3$, which corresponds to configuration III.
B. S (Sulfur):} Sulfur has the electronic configuration $[\text{Ne}] 3s^2 3p^4$, which corresponds to configuration II.
C. Br (Bromine):} Bromine has the electronic configuration $[\text{Ar}] 3d^{10} 4s^2 4p^5$, which corresponds to configuration I.
D. Kr (Krypton):} Krypton has the electronic configuration $[\text{Ar}] 3d^{10} 4s^2 4p^6$, which corresponds to configuration IV.
Thus, the correct match is A-III, B-II, C-I, D-IV. Hence, the answer is (2).
Rods $x$ and $y$ of equal dimensions but of different materials are joined as shown in figure. Temperatures of end points $A$ and $F$ are maintained at $100^\circ$C and $40^\circ$C respectively. Given the thermal conductivity of rod $x$ is three times of that of rod $y$, the temperature at junction points $B$ and $E$ are (close to): 
\(XPQY\) is a vertical smooth long loop having a total resistance \(R\), where \(PX\) is parallel to \(QY\) and the separation between them is \(l\). A constant magnetic field \(B\) perpendicular to the plane of the loop exists in the entire space. A rod \(CD\) of length \(L\,(L>l)\) and mass \(m\) is made to slide down from rest under gravity as shown. The terminal speed acquired by the rod is _______ m/s. 
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 