To solve this problem, we need to use the mirror formula and the magnification formula for mirrors. Given the magnification (\( m \)) and the object-image distance, we can find the focal length of the mirror.
The magnification \( m \) of a mirror is given by:
\(m = \frac{-v}{u}\)
where:
We are given:
From the definition of magnification, we have:
\(\frac{-v}{u} = \frac{1}{4}\)
Solving for \( v \), we find:
\(v = -\frac{u}{4}\)
The negative sign indicates that the image is real and on the opposite side of the mirror from the object.
We also know that:
\(|v - u| = 40 \, \text{cm}\)
Substitute \( v = -\frac{u}{4} \) into this equation:
\(|\left(-\frac{u}{4}\right) - u| = 40\)
Combine the terms:
\(|-\frac{5u}{4}| = 40\)
\(\frac{5u}{4} = 40\)
Solve for \( u \):
\(u = \frac{4 \times 40}{5} = 32 \, \text{cm}\)
Using \( v = -\frac{u}{4} \), we find:
\(v = -\frac{32}{4} = -8 \, \text{cm}\)
Now, apply the mirror formula:
\(\frac{1}{f} = \frac{1}{v} + \frac{1}{u}\)
Substitute \( v = -8 \, \text{cm} \) and \( u = 32 \, \text{cm} \):
\(\frac{1}{f} = \frac{1}{-8} + \frac{1}{32}\)
\(\frac{1}{f} = \frac{-1}{8} + \frac{1}{32} = -\frac{4}{32} + \frac{1}{32} = -\frac{3}{32}\)
Invert to find \( f \):
\(f = -\frac{32}{3} \approx -10.7 \, \text{cm}\)
Thus, the focal length of the mirror is approximately -10.7 cm. Since the options are positive, we ignore the negative, indicating a concave mirror. The correct answer is 10.7 cm.
Step 1: Understand the given information.
Magnification, \( m = \frac{1}{4} \) (positive, so the image is virtual and erect, implying a convex mirror, or real and inverted)
Distance between object and image, \( |v - u| = 40 \) cm
Step 2: Consider the case of a real and inverted image (concave mirror).
For a real and inverted image, \( m = -\frac{v}{u} = -\frac{1}{4} \), so \( v = \frac{1}{4} u \).
Since the image is real and inverted, it forms on the same side as the incident light, so \( v \) is negative according to the sign convention if \( u \) is negative.
Let \( u = -x \) where \( x>0 \). Then \( v = -\frac{1}{4} x \).
The distance between object and image is \( |v - u| = |-\frac{1}{4} x - (-x)| = |-\frac{1}{4} x + x| = |\frac{3}{4} x| = 40 \).
So, \( \frac{3}{4} x = 40 \implies x = \frac{160}{3} \) cm.
Therefore, \( u = -\frac{160}{3} \) cm and \( v = -\frac{1}{4} \times \frac{160}{3} = -\frac{40}{3} \) cm.
Using the mirror formula: \( \frac{1}{f} = \frac{1}{v} + \frac{1}{u} = \frac{1}{-40/3} + \frac{1}{-160/3} = -\frac{3}{40} - \frac{3}{160} = \frac{-12 - 3}{160} = -\frac{15}{160} = -\frac{3}{32} \). So, \( f = -\frac{32}{3} \approx -10.67 \) cm.
The focal length is positive for a concave mirror, so there is a sign error somewhere.
Let's recheck the magnification sign. If \( m = -\frac{v}{u} = -\frac{1}{4} \), then \( v = \frac{1}{4} u \).
For a real image, \( v \) and \( u \) have the same sign. With the convention that real objects have negative \( u \), real images have negative \( v \). So, \( v = \frac{1}{4} u \implies v \) is less negative than \( u \), which is consistent with a real image formed by a concave mirror.
Distance \( |v - u| = |\frac{1}{4} u - u| = |-\frac{3}{4} u| = 40 \). Since \( u \) is negative, \( -\frac{3}{4} u = 40 \implies u = -\frac{160}{3} \) cm.
Then \( v = \frac{1}{4} (-\frac{160}{3}) = -\frac{40}{3} \) cm. \( \frac{1}{f} = \frac{1}{v} + \frac{1}{u} = \frac{1}{-40/3} + \frac{1}{-160/3} = -\frac{3}{40} - \frac{3}{160} = \frac{-12 - 3}{160} = -\frac{15}{160} = -\frac{3}{32} \). \( f = -\frac{32}{3} \approx -10.67 \) cm.
The focal length of a concave mirror is negative. The magnitude is \( 10.67 \) cm.
Step 3: Consider the case of a virtual and erect image (convex mirror).
For a virtual and erect image, \( m = -\frac{v}{u} = \frac{1}{4} \), so \( v = -\frac{1}{4} u \).
For a real object, \( u \) is negative. Let \( u = -x \) where \( x>0 \). Then \( v = \frac{1}{4} x \).
The image is virtual, so \( v \) is positive. Distance \( |v - u| = |\frac{1}{4} x - (-x)| = |\frac{5}{4} x| = 40 \).
So, \( \frac{5}{4} x = 40 \implies x = 32 \) cm.
Therefore, \( u = -32 \) cm and \( v = \frac{1}{4} (32) = 8 \) cm.
Using the mirror formula: \( \frac{1}{f} = \frac{1}{v} + \frac{1}{u} = \frac{1}{8} + \frac{1}{-32} = \frac{4 - 1}{32} = \frac{3}{32} \).
So, \( f = \frac{32}{3} \approx 10.67 \) cm.
The focal length of a convex mirror is positive.
The magnitude of the focal length is approximately 10.7 cm.
A transparent block A having refractive index $ \mu_2 = 1.25 $ is surrounded by another medium of refractive index $ \mu_1 = 1.0 $ as shown in figure. A light ray is incident on the flat face of the block with incident angle $ \theta $ as shown in figure. What is the maximum value of $ \theta $ for which light suffers total internal reflection at the top surface of the block ?
Let one focus of the hyperbola \( H : \dfrac{x^2}{a^2} - \dfrac{y^2}{b^2} = 1 \) be at \( (\sqrt{10}, 0) \) and the corresponding directrix be \( x = \dfrac{9}{\sqrt{10}} \). If \( e \) and \( l \) respectively are the eccentricity and the length of the latus rectum of \( H \), then \( 9 \left(e^2 + l \right) \) is equal to: