| Class XII |
Mathematics |
Mathematics Part-II |
7 |
0 ® P (E ∩ F) = P (F) P (E|F), P (F) ≠ 0 ® If E and F are independent, then P (E ∩ F) = P (E) P (F) P (E|F) = P (E), P (F) ≠ 0 P (F|E) = P (F), P(E... |
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| Class XII |
Physics |
Physics Part-II |
1 |
the mirror. The geometry of reflection of an incident ray is shown in Fig. 9.4. Let C be the centre of curvature of the mirror. Consider a ray para... |
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| Class XII |
Physics |
Physics Part-II |
1 |
(i) The ray from the point which is parallel to the principal axis. The reflected ray goes through the focus of the mirror. (ii) The ray passing th... |
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| Class XII |
Physics |
Physics Part-II |
1 |
get B′F B′P –FP B′P FP = FP = BP (9.6) Equation (9.6) is a relation involving magnitude of distances. We now apply the sign convention. We note tha... |
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| Class XII |
Physics |
Physics Part-II |
1 |
by a concave and convex mirror. You should verify that Eqs. (9.7) and (9.9) are valid for these cases as well. FIGURE 9.6 Image formation by (a) a ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
(for u = –39 + 5 = –34) is (34/35 )m. 4 Reprint 2026-27 Physics The shift in the position of image in 1 s is 39 − 34 = 1365 −360 = 5 = 1 m 40 35 14... |
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| Class XII |
Physics |
Physics Part-II |
1 |
is constant. Remember that the angles of incidence (i) and refraction (r ) are the angles that the incident and its refracted ray make with the nor... |
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| Class XII |
Physics |
Physics Part-II |
1 |
index of medium 3 with respect to medium 2 then n 32= n × n , where n is the refractive index of 31 12 31 medium 3 with respect to medium 1. Some e... |
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| Class XII |
Physics |
Physics Part-II |
1 |
If the angle of incidence isincreasedstillfurther(e.g.,therayAO ),4 refractionisnotpossible,andtheincident ray is totally reflected. This is called... |
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| Class XII |
Physics |
Physics Part-II |
1 |
drops of milk or any other suspension to water and stir so that water becomes a little turbid. Take a laser pointer and shine its beam through the ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
of which should be spherical. Applying the formula for image formation by a single spherical surface successively at the two surfaces of a lens, we... |
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| Class XII |
Physics |
Physics Part-II |
1 |
v u R Equation (9.16) gives us a relation between object and image distance in terms of refractive index of the medium and the radius of curvature ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
DI BC 1 DC 2 Suppose the object is at infinity, i.e., OB and DI = f, Eq. (9.19) gives n1 1 1 = (n2−n )1 + (9.20) f BC 1 DC 2 The poin... |
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| Class XII |
Physics |
Physics Part-II |
1 |
we derived it for a real image formed by a convex lens, the formula is valid for both convex as well as concave lenses and for both real and virtua... |
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| Class XII |
Physics |
Physics Part-II |
1 |
holds good for all cases. Here again it must be remembered that each point on an object gives out infinite number of rays. All these rays will pass... |
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| Class XII |
Physics |
Physics Part-II |
1 |
tangent of the angle by which it converges or diverges a beam of light parallel to the principal axis falling at unit distance from the optical cen... |
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| Class XII |
Physics |
Physics Part-II |
1 |
we have 1 1 1 =(n−1 ) − 12 10 −15 This gives n = 1.5. (iii) For a glass lens in air, n = 1.5, n = 1, f = +20 cm. Hence, the lens 2 1 form... |
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| Class XII |
Physics |
Physics Part-II |
1 |
(9.28) 1 2 Adding Eqs. (9.27) and (9.28), we get 1 1 1 1 v − u = f + f (9.29) 1 2 If the two lens-system is regarded as equivalent to a single lens... |
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| Class XII |
Physics |
Physics Part-II |
1 |
. v1 u 1 f1 L 1 1 1 P v − −30 10 A 1 X or v1= 15 cm 238 E Reprint 2026-27 Ray Optics and Optical Instruments The image formed by the first lens ser... |
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| Class XII |
Physics |
Physics Part-II |
1 |
these two equations, we get r1+ r2= A (9.34) The total deviationd is the sum of deviations at the two faces, d= (i – 1 ) + (e 2 r ) that is, d = i ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
(n 21)A It implies that, thin prisms do not deviate light much. 9.7 O PTICAL INSTRUMENTS A number of optical devices and instruments have been desi... |
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| Class XII |
Physics |
Physics Part-II |
1 |
near point (distance D @ 25 cm), it causes some strain on the eye. Therefore, the image formed at infinity is often considered most suitable for vi... |
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| Class XII |
Physics |
Physics Part-II |
1 |
closer for image formation at the near point. Clearly, m p l s the final image is inverted with respect to the original object. We now obtain the m... |
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| Class XII |
Physics |
Physics Part-II |
1 |
In practice, it is difficult to make the focal length much smaller than 1 cm. Also large lenses are required to make L large. For example, with an ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
whose objective has a focal length of 100 cm and the eyepiece a focal length of 1 cm. The magnifying power of this telescope is m = 100/1 = 100. Le... |
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