A slanted object AB is placed on one side of convex lens as shown in the diagram. The image is formed on the opposite side. Angle made by the image with principal axis is: 
The location of the image of A can be found using the lens formula: \[ \frac{1}{v} - \frac{1}{u} = \frac{1}{f} \] where \( f = 20 \, \text{cm} \), \( u = -30 \, \text{cm} \), and \( v = 60 \, \text{cm} \). Using the magnification formula: \[ m = \frac{v}{u} = \frac{60}{-30} = -2 \] Since the object size is small with respect to the location, we can calculate the small change \( dv \) in the image: \[ dv = m^2 du = 4 \times 1 = 4 \, \text{cm} \] This gives us the size of the image at \( P \) as \( h_i = m h_o = 2 \times 2 = 4 \, \text{cm} \).
The angle made by the image with the principal axis is \( -45^\circ \), which corresponds to the correct answer.
The problem asks for the angle made by the image of a slanted object AB with the principal axis. The object is placed in front of a convex lens. We can solve this by finding the coordinates of the images of the endpoints A and B of the object and then determining the slope of the line connecting these image points.
The solution relies on the thin lens formula and the lateral magnification formula.
Step 1: Determine the coordinates of the endpoints of the object (A and B).
Let the optical center of the convex lens be the origin (0, 0). The principal axis is the x-axis. According to the sign convention and the diagram:
Step 2: Find the coordinates of the image of point A (let's call it A').
For point A, the object distance is \( u_A = -30 \, \text{cm} \). Using the lens formula to find the image distance \( v_A \):
\[ \frac{1}{v_A} - \frac{1}{-30} = \frac{1}{20} \] \[ \frac{1}{v_A} = \frac{1}{20} - \frac{1}{30} = \frac{3 - 2}{60} = \frac{1}{60} \] \[ v_A = +60 \, \text{cm} \]
Since point A is on the principal axis, its image A' will also be on the principal axis. The coordinates of A' are \( (60, 0) \).
Step 3: Find the coordinates of the image of point B (let's call it B').
For point B, the object distance is \( u_B = -29 \, \text{cm} \) and the object height is \( h_{oB} = 2 \, \text{cm} \). First, we find the image distance \( v_B \) using the lens formula:
\[ \frac{1}{v_B} - \frac{1}{-29} = \frac{1}{20} \] \[ \frac{1}{v_B} = \frac{1}{20} - \frac{1}{29} = \frac{29 - 20}{20 \times 29} = \frac{9}{580} \] \[ v_B = \frac{580}{9} \, \text{cm} \]
Now, we find the height of the image of B (\( h_{iB} \)) using the lateral magnification formula:
\[ m_B = \frac{v_B}{u_B} = \frac{580/9}{-29} = -\frac{580}{9 \times 29} = -\frac{20}{9} \] \[ h_{iB} = m_B \times h_{oB} = \left(-\frac{20}{9}\right) \times 2 = -\frac{40}{9} \, \text{cm} \]
The coordinates of B' are \( \left(\frac{580}{9}, -\frac{40}{9}\right) \).
Step 4: Calculate the slope of the image A'B' to find the angle.
The image is the line segment connecting A'(60, 0) and B'\( \left(\frac{580}{9}, -\frac{40}{9}\right) \). Let \( \beta \) be the angle the image makes with the principal axis. The tangent of this angle is the slope of the line A'B'.
\[ \tan(\beta) = \frac{\Delta y}{\Delta x} = \frac{y_{B'} - y_{A'}}{x_{B'} - x_{A'}} \] \[ \tan(\beta) = \frac{-\frac{40}{9} - 0}{\frac{580}{9} - 60} = \frac{-\frac{40}{9}}{\frac{580 - 540}{9}} = \frac{-\frac{40}{9}}{\frac{40}{9}} = -1 \]
The tangent of the angle made by the image with the principal axis is -1.
\[ \tan(\beta) = -1 \]
This means the angle of inclination with the positive x-axis is \( 135^\circ \). The question asks for the angle made by the image with the principal axis, which is typically the acute angle. The magnitude of the angle is:
\[ \beta = \tan^{-1}(|-1|) =- 45^\circ \]
The angle made by the image with the principal axis is - 45°.
Light from a point source in air falls on a spherical glass surface (refractive index, \( \mu = 1.5 \) and radius of curvature \( R = 50 \) cm). The image is formed at a distance of 200 cm from the glass surface inside the glass. The magnitude of distance of the light source from the glass surface is 1cm.
A symmetric thin biconvex lens is cut into four equal parts by two planes AB and CD as shown in the figure. If the power of the original lens is 4D, then the power of a part of the divided lens is:

If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:
The major product (A) formed in the following reaction sequence is
