Let the object distance be \(u\), and the image distance be \(v\). Since the magnification \(m = -\frac{v}{u} = 3\), we have:
\[ v = 3u \]
From the lens formula:
\[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \]
Substituting \(v = 3u\):
\[ \frac{1}{f} = \frac{1}{3u} - \frac{1}{u} \]
Simplifying:
\[ \frac{1}{f} = \frac{1 - 3}{3u} = -\frac{2}{3u} \]
Now, since \(u = 10 \, \text{cm}\), we get:
\[ f = 15 \, \text{cm} \]
Thus, the correct answer is 15.
Let a line passing through the point $ (4,1,0) $ intersect the line $ L_1: \frac{x - 1}{2} = \frac{y - 2}{3} = \frac{z - 3}{4} $ at the point $ A(\alpha, \beta, \gamma) $ and the line $ L_2: x - 6 = y = -z + 4 $ at the point $ B(a, b, c) $. Then $ \begin{vmatrix} 1 & 0 & 1 \\ \alpha & \beta & \gamma \\ a & b & c \end{vmatrix} \text{ is equal to} $
Resonance in X$_2$Y can be represented as
The enthalpy of formation of X$_2$Y is 80 kJ mol$^{-1}$, and the magnitude of resonance energy of X$_2$Y is: