Question 1:
Both – diffraction from each slit and interference of the waves coming from the two slits.
Question 18:
The two beams are incoherent, because each has as its source an incandescent light bulb, so that there is no particular phase relationship between light from each bulb (short coherence length). Thus, no interference pattern is visible, since coherence is a necessary condition for interference patterns.
Exercise 3:
Δy = λ D / d = 5.12*10-7m 5.4m /
1.2*10-3m = 2.3 mm
Exercise
7 :
ym =
mλD/d
ym(2)
– ym(1) = (λ2 – λ1)mD/d
è y3(2) – y3(1)
= (6.12-4.80)10-7m * 3 *1.36m / 5.22*10-3 m = 0.103 mm
Exercise
28 :
2d = (m+1/2)λfilm = (m+1/2)λair / nfilm for maxima
2d = mλfilm = mλair / nfilm for minima
λmax
= 600 nm = 2 d n / (m+1/2)
λmin = 450 nm = 2 d n / m
λmax / λmin = m / (m+1/2) = 4/3 è m = -2
Using |m|= 2
d = λmin |m| / (2n) = ¾ 450 nm = 338 nm
Exercise 40:
Each fringe corresponds to one-half wavelength.
Thus, 5cm*(nair-1)
= 60 (5.00*10-5cm) / 2 è nair = 6*5.00*10-5 + 1 =
1.0003
Problem 2 :
The optical pathlength difference (n-1)t corresponds to a change in λ of 7λ.
è (n-1)t = 7λ è t = 7λ/(n-1) = 7*5.50*10-7m / 0.58 = 6.64 μm
Problem 4:
Here (n1-1)t – (n2-1)t = (5-0) λ
è (n1-n2)t = 5 λ
è t = 5λ / (n1-n2) = 5*4.80*10-7m / (1.7-1.4) = 8.00 μm
Problem 5:
Using Φ = 2π d sinθ/ λ so ΔΦ = 2π d Δ(sinθ)/ λ = 2π d cosθ Δθ / λ
Choose first minimum, so that m=1, since the width of the fringes is the same.
Then 2π d cosθ Δθ / λ = π è Δθ = λ / (2 d cosθ)
For small θ: cosθ
≈ 1 è
Δθ = λ / (2 d)