Правка разделов «Solution», «Answer»

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правка #20494 предыдущая #17968 ← раньше
@@ -4,12 +4,28 @@Statement
### Solution
−![For problem $13.1.13$ |1488x2105, 31%](../../img/13.1.13/scan-1.png)
+![|589x684, 50%](../../img/13.1.13/парвпрваопропр.png)
−![For problem $13.1.13$ |1488x2105, 31%](../../img/13.1.13/scan-0.png)
+Consider a ray parallel to the principal optical axis incident on a spherical mirror at point $A$.
−Here it was used that h' = 0, no matter what the original h value is. Since the incident height does not change where the ray converges. I would also like to note, that I made a small error, For a light ray travelling at an angle, I wrote sin(β), it is supposed to be tan(β), but we can still use the small angle approximation. So it doesn't change the result.
+The radius of the mirror $OA = R$ is the normal to the surface at the point of incidence. According to the law of reflection, the angle of incidence equals the angle of reflection: $\angle (\text{incident ray}, OA) = \angle OAF = \alpha$.
+Since the incident ray is parallel to the principal optical axis $OC$, the alternate interior angle $\angle AOF$ is also equal to $\alpha$.
+
+Therefore, triangle $\triangle AOF$ is isosceles, which implies:
+$$ |OF| = |AF| $$
+
+Let us drop a perpendicular from point $F$ to the segment $OA$. In an isosceles triangle, this perpendicular also acts as a median, hence:
+$$ |OF| \cos \alpha = \frac{R}{2} \implies |OF| = \frac{R}{2 \cos \alpha} $$
+
+The distance from the pole of the mirror $C$ to the focus $F$ (the focal length) is given by:
+$$ F = |OC| - |OF| = R - \frac{R}{2 \cos \alpha} $$
+
+For paraxial rays, which form a sharp image, the angle $\alpha$ is small ($\alpha \to 0$). In this approximation, $\cos \alpha \approx 1$.
+
+Taking this limit, we obtain the focal length of the spherical mirror:
+$$ F = R - \frac{R}{2} = \frac{R}{2} $$
+
#### Answer
−[R/2]
+$$ F = \frac{R}{2} $$