Optics
A man wearing glasses of focal length $$+ 1 \mathrm { m }$$ cannot clearly see beyond $$1\mathrm { m }$$
Find the magnification of a Keplerian telescope adjusted to infinity if the mounting of the objective has a diameter $$ D $$ and the image of that mounting formed by the telescope's ocular has a diameter $$ d $$.
In the Kelplerian telescope, in normal adjustment , the distance between the objective and eyepiece is $$f_0+f_e$$. The image of the mounting produced by the eyepiece is formed at a distance $$v$$ to the right where
$$\dfrac{1}{s'}-\dfrac{1}{s}=\dfrac{1}{f_e}$$
But $$s=-(f_0+f_e),$$
so $$\dfrac{1}{s'}=\dfrac{1}{f_e}-\dfrac{1}{f_0+f_e}=\dfrac{f_0}{f_e(f_0+f_e)}$$
The linear magnification produced by the eyepiece of the mounting is, in magnitude
$$|\beta|=|\dfrac{s'}{s}|=\dfrac{f_e}{f_0}$$
This equals $$\dfrac{d}{D}$$ according to the problem so
$$I'=\dfrac{f_e}{f_e}=\dfrac{D}{d}$$
A man wearing glasses of focal length $$+ 1 \mathrm { m }$$ cannot clearly see beyond $$1\mathrm { m }$$
A lens forms a sharp image of a real object on screen. On inserting a parallel slide between the lens and the screen with its thickness along the principal axis of the lens, it is found necessary to shift the screen parallel to itself distance $$d$$ away from the lens for getting image sharply focussed on it. If the refractive index of the glass relative to air is $$\mu$$, the thickness of the slab is :
If David is observing his image in plane mirror. The distance between the mirror and his image is 4 m. If he moves 1 m towards the mirror, then the distance between David and his image will be :
Light from a point source in air falls on a spherical glass surface whose radius of curvature and refractive index are 20 cm and 1.5 respectively. If the distance of light source from the glass surface is 100 cm, then at which position image will be formed?
There are two thin symmetrical lenses: one is converging, with refractive index $$ n_{1}=1.70, $$, and the other is diverging with refractive index $$ n_{2}=1.51. $$ Both lenses have the same curvature radius of their surfaces equal to $$ R=10 \mathrm{cm} . $$ The lenses were put close together and submerged into water. What is the focal length of this system in the water?
On passing through a telescope a flux of light increases its intensity $$ \eta=4.0 \times 10^{4} $$ times. Find the angular dimension of a distant object if its image formed by that telescope has an angular dimension $$ \psi^{\prime}=2.0^{\circ} $$
An illuminated slide is held $$44$$ cm from a screen. How far from the slide must a lens of focal length $$11$$ cm be placed (between the slide and the screen) to form an image of the slide’s picture on the screen?
Figure(a) shows the basic structure of an old film camera. A lens can be moved forward or back to produce an image on film at the back of the camera. For a certain camera, with the distance, i between the lens and the film set at $$f=5.0\,cm$$, parallel light rays from a very distant object O converge to a point image on the film, as shown. The object is now brought closer, to a distance of $$p = 100\,cm$$, and the lens–film distance is adjusted so that an inverted real image forms on the film. (a) What is the lens–film distance i now? (b) By how much was distance i changed?
The graph shows the variation of magnification $$m$$ produced by convex lens with image distance $$ \vartheta$$. The focal length of the lens used is :
A convex lens of focal length $$f$$ is placed somewhere in between the object and a screen. The distance between object and screen is $$x$$. If magnification produced is $$m$$, the focal length of the lens is: