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 current element X is connected across an AC source of emf \(V = V_0\ sin\ 2πνt\). It is found that the voltage leads the current in phase by \(\frac{π}{ 2}\) radian. If element X was replaced by element Y, the voltage lags behind the current in phase by \(\frac{π}{ 2}\) radian.
(I) Identify elements X and Y by drawing phasor diagrams.
(II) Obtain the condition of resonance when both elements X and Y are connected in series to the source and obtain expression for resonant frequency. What is the impedance value in this case?