| Class XII |
Mathematics |
Mathematics Part-II |
7 |
® 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 |
Mathematics |
Mathematics Part-II |
7 |
of probability lies in the correspondence between two great men of the seventeenth century, Pascal (1623-1662) and Pierre de Fermat (1601-1665). A ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
Chapter Nine RAY OPTICS AND OPTICAL INSTRUMENTS 9.1 I NTRODUCTION Nature has endowed the human eye (retina) with the sensitivity to detect electrom... |
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| Class XII |
Physics |
Physics Part-II |
1 |
reflecting and refracting surfaces. We then go on to describe the construction and working of some important optical instruments, including the hum... |
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| Class XII |
Physics |
Physics Part-II |
1 |
follow the Cartesian sign convention. According to this convention, all distances are measured fromthepoleofthemirrorortheoptical centre of the len... |
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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 |
of a concave mirror of radius of curvature 15 cm. Find the position, nature, and magnification of the image in each case. Solution The focal length... |
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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 |
2 |
Wave Optics Chapter Ten WAVE OPTICS 10.1 I NTRODUCTION In 1637 Descartes gave the corpuscular model of light and derived Snell’s law.Itexplainedthe... |
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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 |
few 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 ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
material of the prism must be less than 45°. We see from Table 9.1 that this is true for both FIGURE 9.12 Observing total internal crown glass and ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
used as a ‘light pipe’ to facilitate visual examination of internal organs like esophagus, stomach and intestines. You might have seen a commonly a... |
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| Class XII |
Physics |
Physics Part-II |
1 |
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 serves as ... |
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| Class XII |
Physics |
Physics Part-II |
1 |
which should be spherical. Applying the formula for image formation by a single spherical surface successively at the two surfaces of a lens, we sh... |
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| Class XII |
Physics |
Physics Part-II |
1 |
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 of the... |
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| Class XII |
Physics |
Physics Part-II |
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 point where i... |
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| Class XII |
Physics |
Physics Part-II |
1 |
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 virtual images. It i... |
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| Class XII |
Physics |
Physics Part-II |
1 |
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 through the sa... |
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| Class XII |
Physics |
Physics Part-II |
1 |
angle by which it converges or diverges a beam of light parallel to the principal axis falling at unit distance from the optical centre (Fig. 9.18)... |
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