Let the total resistance of the wire be $ R $.
Equilateral Triangle Analysis:
Each of the three sides of the equilateral triangle possesses a resistance of $ \frac{R}{3} $. When considering two vertices of a single side:
These two resistance paths are connected in parallel, yielding the equivalent resistance of the triangle:
$$ R_{\text{triangle}} = \frac{\left(\frac{R}{3}\right)\left(\frac{2R}{3}\right)}{\frac{R}{3} + \frac{2R}{3}} = \frac{\frac{2R^2}{9}}{R} = \frac{2R}{9} $$
Square Analysis:
Each of the four sides of the square has a resistance of $ \frac{R}{4} $. When considering two vertices of a single side:
These two resistance paths are connected in parallel, yielding the equivalent resistance of the square:
$$ R_{\text{square}} = \frac{\left(\frac{R}{4}\right)\left(\frac{3R}{4}\right)}{\frac{R}{4} + \frac{3R}{4}} = \frac{\frac{3R^2}{16}}{R} = \frac{3R}{16} $$
Ratio Calculation:
The ratio of the resistance of the triangle to that of the square is computed as follows:
$$ \frac{R_{\text{triangle}}}{R_{\text{square}}} = \frac{\frac{2R}{9}}{\frac{3R}{16}} = \frac{2R}{9} \times \frac{16}{3R} = \frac{32}{27} $$
Conclusion:
The final calculated ratio is $ \frac{32}{27} $.
Two charges \( +q \) and \( -q \) are placed at points \( A \) and \( B \) respectively which are at a distance \( 2L \) apart. \( C \) is the midpoint of \( AB \). The work done in moving a charge \( +Q \) along the semicircle CSD (\( W_1 \)) and along the line CBD (\( W_2 \)) are 
Find work done in bringing charge q = 3nC from infinity to point A as shown in the figure : 