Given Information:
$P_{eq} = 2P_l + P_m$
$-\frac{1}{f_{eq}} = \frac{2}{f_l} - \frac{1}{f_m}$
$\frac{4(\mu-1)}{R} - \frac{2}{-R} = \frac{1}{R}(4\mu - 4 + 2)$
Explanation of Steps: Step 1: Simplify the third equation
$\frac{4(\mu-1)}{R} - \frac{2}{-R} = \frac{1}{R}(4\mu - 4 + 2)$
$\frac{4\mu - 4}{R} + \frac{2}{R} = \frac{4\mu - 2}{R}$
$\frac{4\mu - 4 + 2}{R} = \frac{4\mu - 2}{R}$
$\frac{4\mu - 2}{R} = \frac{4\mu - 2}{R}$
Explanation: Here, we expand the terms and simplify the equation. This step shows that the equation holds true.
Step 2: Substitute into the second equation
From the given information, we have: $-\frac{1}{f_{eq}} = \frac{2}{f_l} - \frac{1}{f_m}$ We are given that $\frac{2}{f_l} - \frac{1}{f_m} = \frac{4\mu - 2}{R}$ from the third equation. Substituting this into the second equation: $-\frac{1}{f_{eq}} = \frac{4\mu - 2}{R}$
Explanation: This step substitutes the simplified expression from the third equation into the second equation to relate the equivalent focal length to $\mu$ and $R$.
Step 3: Solve for $f_{eq}$
Multiply both sides by -1: $\frac{1}{f_{eq}} = -\frac{4\mu - 2}{R}$
Take the reciprocal of both sides: $f_{eq} = -\frac{R}{4\mu - 2}$ Also,
we are given $R = 2f_{eq}$, so $f_{eq} = \frac{R}{2}$. Substituting $f_{eq} = \frac{R}{2}$ into $R = -f_{eq}(4\mu - 2)$: $R = -\frac{R}{2}(4\mu - 2)$
$R = 2f_{eq} = -2 \left( \frac{R}{4\mu - 2} \right) = \frac{-R}{2\mu - 1}$
$1 = \frac{-1}{2\mu - 1}$
$2\mu - 1 = -1$
$2\mu = 0$
$\mu = 0$ The final expression is: $R = \frac{-R}{2\mu - 1}$
Final Result: $R = \frac{-R}{2\mu - 1}$
In the diagram given below, there are three lenses formed. Considering negligible thickness of each of them as compared to \( R_1 \) and \( R_2 \), i.e., the radii of curvature for upper and lower surfaces of the glass lens, the power of the combination is:
The steam volatile compounds among the following are: