Chapter #23 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. On the surface of the earth we receive about 1.37 kW of energy per square meter from the sun. Calculate the electric field associated with the sunlight (on the surface of the earth) assuming that it is essentially monochromatic with l= 6000Å.[Ans. ~1000 V/m] Get solution

2. (a) On the surface of the earth we receive about 1370 W m-2 of energy. Show that the radiation pressure is about 4.6 μPa (1 Pa = 10-5 N m-2 ).(b) A 100 W sodium lamp (λ ≈ 5890 Å) is assumed to emit waves uniformly in all directions. What is the radiation pressure on a plane mirror at distance of 10 m from the bulb? Get solution

3. A 1 kW transmitter is emitting electromagnetic waves of (of wavelength 40 m) uniformly in all directions. Calculate the electric field at a distance of 1 km from the transmitter. Get solution

4. Ocean water can be assumed to be a non –magnetic dielectric with ... and ...mhos/m. (a) Calculate the frequency at which the penetration depth will be 10 cm. (b) Show that for frequencies less than 108 s-1, it can be considered as a good conductor.[Ans (a) ~6×106 s–1] Get solution

5. For silver one may assume ...and ...mhos/m. Calculate the skin depth at 108 s–1.[Ans. ...cm] Get solution

6. Show that for frequencies ≲ 108 sec-1, a sample of silicon will act like a good conductor. For silicon one may assume ...and ...mhos/cm. Also calculate the penetration depth for this sample at .... Get solution

7. In a conducting medium show that H also satisfies an equation similar to Eq. (94). Get solution

8. Using the analysis given in Sec. 23.7 and assuming ... (which is valid for an insulator) show that... and... where... Get solution

9. For the glass used in a typical optical fiber at ...Å, ......mhos/m. Calculate ...and show that we can use the formulae given in the previous problem. Calculate β and loss in dB/km. [Hint : the power would decrease as exp (–2 βz); loss in dB/km is defined in Sec. 24.8][Ans. ...m-1 ; loss ≈ 3.7 dB/km] Get solution


Chapter #22 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. Discuss the state of polarization when the x and y components of the electric field are given by the following equations:(a) ... (b) ...(c) ... (d)   ... In each case, plot the rotation of the tip of the electric vector on the plane z = 0.[Ans: (a) Linearly polarized, (b) Right-circularly polarized, (c) Left-circularly polarized, and (d) Left-elliptically polarized.] Get solution

2. The electric field components of a plane electromagnetic wave are Ex = 2E0 cos (ωt – kz + ϕ) ; Ey = E0 sin (ωt – kz)Draw the diagram showing the state of polarization (i.e., circular, plane, elliptical or unpolarized) when (a) ϕ = 0  (b) ϕ = π/2  (c) ϕ = π/4 Get solution

3.  Using the data given in Table 22.1, calculate the thickness of quartz half wave plate for λ0 = 5890Å.            [Ans: 32.34 μm] Get solution

4. A right-circularly polarized beam is incident on a calcite half-wave plate. Show that the emergent beam will be left-circularly polarized. Get solution

5. What will be the Brewster angle for a glass slab (n = 1.5) immersed in water (n = 4/3).          [Ans: 48.4°] Get solution

6. Consider the normal incidence of a plane wave on a quartz quarter wave plate whose optic axis is parallel to the surface (see Fig. 22.24). Thus the optic axis is along the z-axis and the propagation is along the x-axis. Show that Ey propagates as an o-wave and Ez as an e-wave.(a) Assuming... at x = 0 show that the emergent light would be right circularly polarized.(b) On the other hand, if one assumes... at x = 0 show that the emergent beam is linearly polarized. Get solution

7. Show that the angle between the vectors D and E is the same as between the Poynting vector S and the propagation vector k. Get solution

8. Consider the propagation of an extra-ordinary wave through a KDP crystal. If the wave vector is at an angle of 45° to the optic axis, calculate the angle between S and k. Repeat the calculation for LiNbO3. The values of no and ne for KDP and LiNbO3 are given in Table 22.1.        [Ans: 1.56° and 2.25°] Get solution

9. Prove that when the angle of incidence corresponds to the Brewster angle, the reflected and refracted rays are at right angles to each other. Get solution

10. (a) Consider two crossed polaroids placed in the path of an unpolarized beam of intensity I0 (see Fig. 22.6). If we place a third polaroid in between the two then, in general, some light will be transmitted through. Explain this phenomenon. (b) Assuming the pass axis of the third polaroid to be at 45° to the pass axis of either of the polaroids, calculate the intensity of the transmitted beam. Assume that all the polaroids are perfect.          [Ans: 1/8 I0] Get solution

11. A quarter-wave plate is rotated between two crossed polaroids. If an unpolarized beam is incident on the first polaroid, discuss the variation of intensity of the emergent beam as the quarter-wave plate is rotated. What will happen if we have a half-wave instead of a quarter-wave plate? Get solution

12. In Problem 22.11, if the optic axis of the quarter-wave plate makes an angle of 45° with the pass axis of either polaroid, show that only a quarter of the incident intensity will be transmitted. If the quarter-wave plate is replaced by a half-wave plate, show that half of the incident intensity will be transmitted through. Get solution

13. ...For calcite, the values of no and ne for λ0 = 4046Å are 1.68134 and 1.49694 respectively; corresponding to λ0 = 7065Å the values are 1.65207 and 1.48359 respectively. We have a calcite quarter-wave plate corresponding to λ0 = 4046Å. A left-circularly polarized beam of λ0 = 7065Å is incident on this plate. Obtain the state of polarization of the emergent beam. Get solution

14. A HWP (half wave plate) is introduced between two crossed polaroids P1 and P2. The optic axis makes an angle 15° with the pass axis of P1 as shown in Fig. 22.39(a) and (b). If an unpolarized beam of intensity I0 is normally incident on P1 and if I1, I2, and I3 are the intensities after P1, after HWP and after P2 respectively then calculate I1/I0, I2/I0 and I3/I0.[Ans: ½, ½, ⅛] Get solution

15. Two prisms of calcite (no > ne) are cemented together as shown in Fig. 22.40, so as to form a cube. Lines and dots show the direction of the optic axis. A beam of unpolarized light is incident normally from region I. Assume the angle of the prism to be 12°. Determine the path of rays in regions II, III & IV indicating the direction of vibrations (i.e., the direction of ).... Get solution

16. A λ/6 plate is introduced in between the two crossed polarizers in such a way that the optic axis of the λ/6 plate makes an angle of 45° with the pass axis of the first polarizer (see Fig. 22.41). Consider an unpolarized beam of intensity I0 to be incident normally on the polarizer. Assume the optic axis to be along the z-axis and the propagation along the x-axis. Write the y and z components of the electric fields (and the corresponding total intensities) after passing through (i) P1 (ii) λ/6 plate and (iii) P2 .... Get solution

17. A beam of light is passed through a polarizer. If the polarizer is rotated with the beam as an axis, the intensity I of the emergent beam does not vary. What are the possible states of polarization of the incident beam? How to ascertain its state of polarization with the help of the given polarizer and a QWP? Get solution

18. Consider a Wollaston prism consisting of two similar prisms of calcite (no = 1.66 and ne = 1.49) as shown in Fig. 22.29, with angle of prism now equal to 25°. Calculate the angular divergence of the two emerging beams. Get solution

19. (a) Consider a plane wave incident normally on a calcite crystal with its optic axis making an angle of 20° with the normal [see Fig. 19.18(a)]. Thus ψ = 20°. Calculate the angle that the Poynting vector will make with the normal to the surface. Assume no ≈ 1.66 and ne ≈ 1.49. (b) In the above problem assume the crystal to be quartz with no ≈ 1.544 and ne ≈ 1.553.         [Ans: (a) 4.31°] Get solution

20. Consider the incidence of he following REP beam on a sugar solution at z = 0:Ex = 5 cos ωt ; Ey = 4 sin ωt with λ = 6328Å. Assume  nl – nr = 10 –5 and nl = 4/3 study the evolution of the SOP of the beam. Get solution

21. Consider the incidence of the above REP beam on an elliptic core fiber with  ... 1.506845 and ... 1.507716 Calculate the SOP at z = 0.25 Lb, 0.5 Lb, 0.75 Lb and Lb. Get solution

22. When the optic axis lies on the surface of the crystal and in the plane of incidence, show (by geometrical considerations) that the angles of refraction of the ordinary and the extra-ordinary rays (which we denote by ro and re respectively) are related through the following equation:  ... Get solution

11&12. Get solution


Chapter #21 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. Consider the reconstruction of the hologram as formed in the configuration of Example 21.2 by a plane wave traveling along a direction parallel to the z-axis. Show the formation of a virtual and a real image. Get solution

2. In continuation of Example 21.2, calculate the interference pattern when the incident plane wave makes an angle θ with the z-axis [see Fig. 14. 13]. Assume B ≈ A/d.[Ans: ...] Get solution

3. Figure 21.6 corresponds to the reconstruction of a doubly exposed hologram, the objects corresponding to the unstrained and strained positions of an aluminum bar of width 4 cm, thickness 0.2 cm and length 12 cm. If the strained position corresponds to a load of 1 gm force applied at the end of the bar, calculate the Young’s modulus of aluminum. Assume θ1 ≈ θ2 ≈ 0 and λ = 6328 Å. [Hint: N represents the number of fringes produced over the length of the cantilever.][Ans: 0.7 × 10 11 N/m2] Get solution


Chapter #20 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. Consider a plane wave of wavelength 6 × 10-5 cm incident normally on a circular aperture of radius 0.01 cm. Calculate the positions of the brightest and the darkest points on the axis. Get solution

2. What would happen if the circular aperture in Problem 20.1 is replaced by a circular disc of the same radius? Get solution

3. A plane wave (λ = 6 × 10-5 cm) is incident normally on a circular aperture of radius a.(a) Assume a = 1 mm. Calculate the values of z (on the axis) for which maximum intensity will occur. Plot the intensity as a function of z and interpret physically. Repeat the calculations for λ = 5 × 10-5 cm and discuss chromatic aberration of a zone plate.(b) Assume z = 50 cm. Calculate the values of a for which minimum intensity will occur on the axial point. Plot the intensity variation as a function of a and interpret physically. Get solution

4. Consider a circular aperture of diameter 2 mm illuminated by a plane wave. The most intense point on the axis is at a distance of 200 cm from the aperture. Calculate the wavelength.     [Ans: 5 × 10-5 cm] Get solution

5. If a zone-plate has to have a principle focal length of 50 cm corresponding to λ = 6 × 10-5 cm, obtain an expression for the radii of different zones. What would be its principle focal length for λ = 5 × 10-5 cm? [...mm, 60 cm] Get solution

6. In a zone-plate, the second, fourth, sixth…zones are blackened; what would happen if instead the 1st, 3rd, 5th, etc., zones were blackened? Get solution

7. (a) A plane wave is incident normally on a straight edge (see Fig. 20.24). Show that the field at an arbitrary point P is given by...where ....(b) Assume λ0 = 5000 Å and d = 100 cm. Write approximately the values of I/I0 at the points O, P (y = 0.5 mm), Q (y = 1 mm) and R (y = -1 mm) where O is at the edge of the geometrical shadow.... Get solution

8. Consider a straight edge being illuminated by a parallel beam of light with λ = 6 × 10-5 cm. Calculate the positions of the first two maxima and minima on a screen at a distance of 50 cm from the edge. Get solution

9. In a straight edge diffraction pattern, one observes that the most intense maximum occurs at a distance of 1 mm from the edge of the geometrical shadow. Calculate the wavelength of light, if the distance between the screen and the straight edge is 300 cm.   [Ans. ≈ 4480 Å] Get solution

10. In a straight edge diffraction pattern, if the wavelength of the light used is 6000 Å and if the distance between the screen and the straight edge is 100 cm, calculate the distance between the most intense maximum and the next maximum. Find approximately the distance in centimeters inside the geometrical shadow where I /I0 = 0.1.[Ans.y ≈ 0.027 cm] Get solution

11. Consider a plane wave falling normally on a narrow slit of width 0.5 mm. If the wavelength of light is 6 × 10-5 cm, calculate the distance between the slit and the screen so that the value of v1 would be 0.5, 1.0, 1.5 and 5.0 (see Fig. 20.19 – 20.22). Discuss the transition to the Fraunhofer region. Get solution

12. Consider the Fresnel diffraction pattern produced by a plane wave incident normally on a slit of width b. Assume λ = 5 × 10-5 cm, d = 100 cm. Using Table 20.1, approximately calculate the intensity values (for b = 0.1 cm) at y = 0, ± 0.05 cm, ± 0.1 cm. Repeat theanalysis for b = 5 cm. Get solution

13. In Sec. 19.7 we obtained the diffraction pattern of a circular aperture of radius a. Obtain the diffraction pattern of an annular aperture bounded by circles of radii a1 and a2 (> a1). [This Problem is already given as Problem 19.5]. Get solution

14. Consider a rectangular aperture of dimensions 0.2 mm × 0.3 mm. Obtain the positions of the first few maxima and minima in the Fraunhofer diffraction pattern along directions parallel to the length and breadth of the rectangle. Assume λ = 5 × 10-5 cm and that the diffraction pattern is produced at the focal plane of a lens of focal length 20 cm. Get solution

15. The Fraunhofer diffraction pattern of a circular aperture (of radius 0.5 mm) is observed on the focal plane of a convex lens of focal length 20 cm. Calculate the radii of the first and the second dark rings. Assume λ = 5.5 × 10-5 cm.[Ans. 0.13 mm, 0.18 mm] Get solution

16. In the above problem, calculate the area of the patch (on focal plane) which will contain 95% of the total energy. Get solution

17. (a) The output of a He-Ne laser (λ = 6328 Å) can be assumed to be Gaussian with plane phase front. For w0 = 1 mm and w0 = 0.2 mm, calculate the beam diameter at z = 20 m.(b) Repeat the calculation for λ = 5000 Å and interpret the results physically. Get solution

18. A Gaussian beam is coming out of a laser. Assume λ = 6000 Å and that at z = 0, the beam width is 1 mm and the phase front is plane. After traversing 10 m through vacuum what will be (a) the beam width and (b) the radius of curvature of the phase front.... Get solution

19. A plane wave of intensity I0 is incident normally on a circular aperture as shown in Fig. 20.25. What will be the intensity on the axial point P? [Hint: You may use Eq. (25)] Get solution

20. Show that a phase variation of the type ...represents a diverging spherical wave of radius R. Get solution

21. Consider a resonator consisting of a plane mirror and a concave mirror of radius of curvature R (see Fig. 20.26). Assume λ = 1 μm, R = 100 cm and the distance between the 2 mirrors to be 50 cm. Calculate the spot size of the Gaussian beam.... Get solution

22. The output of a semiconductor laser can be approximated described by a Gaussian function with two different widths along the transverse (wT) and lateral (wL) directions as...where x and y represent axes parallel and perpendicular to the junction plane. Typically wT ≈ 0.5 μm and wL = 2 μm. Discuss the far field of this beam (see Fig. 20.27).... Get solution


Chapter #19 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. Consider a rectangular aperture of dimensions 0.2 mm × 0.3 mm with a screen placed at a distance of 100 cm from the aperture. Assume a plane wave with λ = 5 × 10-5 cm incident normally on the aperture. Calculate the positions of maxima and minima in a region 0.2 cm × 0.2 cm of the screen. Show that both Fresnel and Fraunhofer approximations are satisfied. Get solution

2. In Problem 19.1 assume a convex lens (of focal length 20 cm) placed immediately after the aperture. Calculate the positions of the first three maxima and minima on the x-axis (implying ϕ = 0) and also on the y-axis (implying θ = 0). Get solution

3. The Fraunhofer diffraction pattern of a circular aperture (of radius 0.5 mm) is observed on the focal plane of a convex lens of focal length 20 cm. Calculate the radii of the first and the second dark rings. Assume λ = 5.5 × 10-5 cm.[Ans. 0.13 mm, 0.18 mm] Get solution

4. In Problem 19.3, calculate the area of the patch (on focal plane) which will contain 95% of the total energy. Get solution

5. Obtain the diffraction pattern of an annular aperture bounded by circles of radii a1 and a2 (> a1). [Hint: The integration limits of ρ in Eq. (35) must be a1 and a2] Get solution


Chapter #18 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. A plane wave (λ = 5000 Å) falls normally on a long narrow slit of width 0.5 mm. Calculate the angles of diffraction corresponding to the first three minima. Repeat the calculations corresponding to a slit width of 0.1 mm. Interpret physically the change in the diffraction pattern[ Ans. 0.057°, 0.115°, 0.17°; 0.29°, 0.57°, 0.86°] Get solution

2. A convex lens of focal length 20 cm is placed after a slit of width 0.6 mm. If a plane wave of wavelength 6000 Å falls normally on the slit, calculate the separation between the second minima on either side of the central maximum.[ Ans. ≈ 0.08cm] Get solution

3. In Problem 18.2 calculate the ratio of the intensity of the principal maximum to the first maximum on either side of the principal maximum.[ Ans. ~ 21] Get solution

4. Consider a laser beam of circular cross-section of diameter 3 cm and of wavelength 5×10-5 cm. Calculate the order of the beam diameter after it has traversed a distance of 3 km.[ Ans. ~ 14 cm. This shows the high directionality of laser beams] Get solution

5. A circular aperture of radius 0.01 cm is placed in front of a convex lens of focal length of 25 cm and illuminated by a parallel beam of light of wavelength 5×10-5 cm. Calculate the radii of the first three dark rings.[Ans. 0.76, 1.4, 2.02 mm] Get solution

6. Consider a plane wave incident on a convex lens of diameter 5 cm and of focal length 10 cm. If the wavelength of the incident light is 6000 Å, calculate the radius of the first dark ring on the focal plane of the lens. Repeat the calculations for a lens of same focal length but diameter 15 cm. Interpret the results physically.[Ans. 1.46 × 10-4 cm, 4.88 × 10-5 cm] Get solution

7. Consider a set of two slits each of width b = 5 × 10-2 cm and separated by a distance d = 0.1 cm, illuminated by a monochromatic light of wavelength 6.328 × 10-5 cm. If a a convex lens of focal length 10 cm is placed beyond the double slit arrangement, calculate the positions of the maxima inside the first diffraction minimum.[Ans. 0.0316 mm, 0.094 mm] Get solution

8. Show that when b = d, the resulting diffraction pattern corresponds to a slit of width 2b. Get solution

9. Show that the first order and second order spectra will never overlap when the grating is used for studying a light beam containing wavelength components from 4000 Å to 7000Å. Get solution

10. Consider a diffraction grating of width 5 cm with slits of width 0.0001 cm separated by a distance of 0.0002 cm. What is the corresponding grating element? How many orders would be observable at λ = 5.5 × 10-5 cm? Calculate the width of principal maximum. Would there be any missing orders? Get solution

11. For the diffraction grating of Problem 16.10, calculate the dispersion in the different orders. What will be the resolving power in each order? Get solution

12. A grating (with 15,000 lines per inch) is illuminated by white light. assuming that white light consist of wavelengths lying between 4000 and 7000 Å, calculate the angular widths of first and the second order spectra. [ Hint : You should not use Eq. (65); why] Get solution

13. A grating (with 15,000 lines per inch) is illuminated by sodium light. The grating spectrum is observed on the focal plane of a convex lens of focal length 10 cm. Calculate the separation between the D1 and D2 lines of sodium. (The wavelengths of D1 and D2 lines are 5890 and 5896 Å respectively.) [Hint : You may use Eq. (65).] Get solution

14. Calculate the resolving power in the second order spectrum of a 1 inch grating having 15,000 lines. Get solution

15. Consider a wire grating of width 1 cm having 1000 wires. Calculate the angular width of the second order principal maximum and compare the value with the one corresponding to a grating having 5000 lines in 1 cm. Assume λ = 5.5 × 10-5 cm Get solution

16. In the minimum deviation position of a diffraction grating the first order spectrum corresponds to an angular deviation of 30°. If λ = 6 × 10-5 cm, calculate the grating element. Get solution

17. Calculate the diameter of a telescope lens if a resolution of 0.1 seconds of arc is required at λ = 6 × 10-5 cm. Get solution

18. Assuming that the resolving power of the eye is determined by diffraction effects only, calculate the maximum distance at which two objects separated by a distance of 2 m can be resolved by the eye. (Assume pupil diameter to be 2 mm and λ = 6000 Å.) Get solution

19. (a) A pinhole camera is essentially a rectangular box with a tiny pinhole in front. An inversted image of the object is formed on the rear of the box. Consider a parallel beam of light incident normally on the pinhole. If we neglect diffraction effects then the diameter of the image will increase linearly with the diameter of the pinhole. On the other hand, if we assume Fraunhofer diffraction, then the diameter of the first dark ring will go on increasing as we reduce the diameter of the pinhole. Find the pinhole diameter for which the diameter of the geometrical image is approximately equal to the diameter of the first dark ring in the Airy pattern. Assume λ = 6000 Å and a separation of 15 cm between the pinhole and the rear of the box.[Ans. (a) 0.47mm] Get solution

20. Copper is an FCC structure with lattice constant 3.615 Å. An X-ray powder photograph of copper is taken. The X-ray beam consists of wavelengths 1.540 Å and 1.544 Å. Show that diffraction maxima will be observed at θ = (21.64°, 21.70°), (25.21°, 25.28°), (37.05°, 37.16°), (44.94°, 45.09°), (47.55°, 47.71°), (58.43°, 58.67°), (68.20°, 68.58°), (72.29°, 72.76°). Get solution

21. Tungsten is a BCC structure with lattice constant 3.1648 Å. Show that in the powder photograph of tungsten (corresponding to an X-ray wavelength of 1.542 Å) one would observe diffraction maxima at θ = 20.15°, 29.17°, 36.64°, 43.56°, 50.39°, 57.55°, 65.74° and 77.03°. Get solution

22. (a) In the simple cubic structure if we alternately place Na and Cl atoms we would obtain the NaCl structure. Show that the Na atoms (and the Cl atoms) independently form FCC structures. The lattice constant associated with each FCC structure is 5.6402 Å. Corresponding to the X-ray wavelength 1.542 Å, show that the diffraction maxima will be observed at θ = 13.69°, 15.86°, 22.75°, 26.95°, 28.97°, 33.15°, 36.57°, 37.69°, 42.05°, 45.26°, 50.66°, 53.98°, 55.10°, 59.84°, 63.69°, 65.06°, 71.27°, 77.45° and 80.66°.(b) Show that if we treat NaCl as a simple cubic structure with lattice parameter 2.82 Å then the maxima at θ = 13.69°, 26.95°, 36.57°, 45.26°, 53.98°, 63.69° and 77.45° will not be observed. Indeed in the X-ray diffraction pattern of NaCl, the maxima corresponding to these angles will be very weak. Get solution

23. Show that the mth order reflection from the planes characterized by (hkl) can be considered as the same as the first order reflection from the planes characterized by (mh mk ml). Get solution

24. Calculate the Fraunhofer diffraction pattern produced by a double slit arrangement with slits of widths b and 3b, with their centers separated by a distance 6b. Get solution

25. Consider the propagation of a 1 kW laser beam (λ = 6943 Å, beam diameter ≈ 1 cm) in CS2. Calculate fd and fnl and discuss the defocusing (or focusing) of the beam. Repeat the calculations corresponding to a 1000 kW beam and discuss any qualitative differences that exist between the two cases. The data for n0 and n2 are given in Sec. 18.11. Get solution

26. The values of ...and ... for benzene are 1.5 and 0.6 ×10-10 C.G.S. units respectively. Obtain an approximate expression for the critical power. Get solution


Chapter #17 Solutions - Optics - Ajoy Ghatak - 1st Edition

1. The orange Krypton like (λ = 6058 Å) has a coherence length of ~20 cm. Calculate the line width and the frequency stability.[ Ans. ~ 0.01 Å, ~ 1.5 × 10-6] Get solution

2. Laser linewidths as low as 20Hz have been obtained. Calculate the coherence length and the frequency stability. Assume λ = 6328 Å. Get solution

3. In Sec. 17.4 we had mentioned that the lateral coherence width of a circular source is 1.22λ/θ. It can be shown that for good coherence (i.e. for a visibility of 0.88 or better), the coherence width should be ƒ 0.3λ/θ. Assuming that the angular diameter of the sun is about 30′, calculate the distance between two pinholes which would produce a clear interference pattern.[ Ans. ~ 0.02 mm] Get solution

4. Calculate the distance at which a source of diameter 1 mm should be kept from a screen so that two points separated by a distance of 0.5 mm may be said to be coherent. Assume λ = 6×10-5 cm. Get solution

5. In a Michelson interferometer experiment, it is found that for a source S, as one of the mirrors is moved away from the equal path length position by a distance of about 5 cm, the fringes disappear. What is the coherence time of the radiation emerging from the source? Get solution

6. If we perform the Young’s double-hole experiment using white light, then only a few coloured fringes are visible. Assuming that the visible spectrum extends from 4000 to 7000 Å, explain this phenomenon qualitatively on the basis of coherence length. Get solution

7. Using the stellar interferometer, Michelson observed for the star Betelgeuse, that the fringes disappear when the distance between the movable mirrors is 25 inches. Assuming λ ≈6×10-5 cm, calculate the angular diameter of the star. Get solution

8. Consider Young’s double-hole experiment as shown in Fig. 17.5. The distance SS1 ≈ 1 m. Calculate the angular diameter of the hole S which will produce a good interference pattern on the screen. Assume λ = 6000 Å. Get solution

9. Assume a Gaussian pulse of form... Show that the Fourier transform is given by... You will have to use the following integral [see Appendix A]...Show that the temporal coherence is ~τ. Assume τ >> (1/ω0), plot the Fourier transform A(ω) [as a function of ω] and interpret it physically. Show that the frequency spread Δω ~1/τ. Get solution

10. In Problem 17.9, assume λ0 = 6×10-5 cm and τ ~10-9 sec. Calculate the frequency components predominantly present in the pulse and compare it with the case corresponding to τ ~10-6 sec. Get solution


Chapter #30 Solutions - Optics - Ajoy Ghatak - 1st Edition

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