Optics Wave Behavior in Optics - De Anza...

OpticsWave Behavior in Optics

Lana Sheridan

De Anza College

June 19, 2017

Last time

• mirrors

• image terminology

• images formed by spherical mirrors

• images formed by refraction

• images formed by lenses

• (images formed by lens combinations)

Overview

• Huygen’s Principle

• Interference of light: the Double-Slit experiment

• diffraction gratings

• diffraction patterns

• diffraction and interference

• resolution and Raleigh’s criterion

Moving beyond Ray Optics

Ray optics can tell us about the formation of images, but it cannottell us about the behavior of light that is specific to waves.

The ray approximation assumes that light will travel out from asource in straight lines, unless it encounters a change of medium.

However light does also behave a wave and can change direction atapertures: diffraction and interference.

Huygens’ Principle

This is a geometric principle to construct a wavefront at a laterpoint in time from a wavefront at an earlier one.

35.6 Huygens’s Principle 1071

Finalize Knowing the apex angle F of the prism and measuring dmin, you can calculate the index of refraction of the prism material. Furthermore, a hollow prism can be used to determine the values of n for various liquids filling the prism.

Pitfall Prevention 35.4Of What Use Is Huygens’s Princi-ple? At this point, the importance of Huygens’s principle may not be evident. Predicting the position of a future wave front may not seem to be very critical. We will use Huygens’s principle here to generate the laws of reflection and refraction and in later chapters to explain additional wave phenom-ena for light.

35.6 Huygens’s PrincipleThe laws of reflection and refraction were stated earlier in this chapter without proof. In this section, we develop these laws by using a geometric method proposed by Huy-gens in 1678. Huygens’s principle is a geometric construction for using knowledge of an earlier wave front to determine the position of a new wave front at some instant:

All points on a given wave front are taken as point sources for the produc-tion of spherical secondary waves, called wavelets, that propagate outward through a medium with speeds characteristic of waves in that medium. After some time interval has passed, the new position of the wave front is the sur-face tangent to the wavelets.

First, consider a plane wave moving through free space as shown in Figure 35.18a. At t 5 0, the wave front is indicated by the plane labeled AA9. In Huygens’s construc-tion, each point on this wave front is considered a point source. For clarity, only three point sources on AA9 are shown. With these sources for the wavelets, we draw circular arcs, each of radius c Dt, where c is the speed of light in vacuum and Dt is some time interval during which the wave propagates. The surface drawn tangent to these wave-lets is the plane BB9, which is the wave front at a later time, and is parallel to AA9. In a similar manner, Figure 35.18b shows Huygens’s construction for a spherical wave.

Huygens’s Principle Applied to Reflection and RefractionWe now derive the laws of reflection and refraction, using Huygens’s principle. For the law of reflection, refer to Figure 35.19. The line AB represents a plane wave front of the incident light just as ray 1 strikes the surface. At this instant, the wave at A sends out a Huygens wavelet (appearing at a later time as the light brown circular arc passing through D); the reflected light makes an angle g9 with the surface. At the

Old wavefront

New wavefront

A B

Old wavefront

New wavefront

A! B!

c "t

c "t

a b

The new wave front is drawn tangent to the circular wavelets radiating from the point sources on the original wave front.

Figure 35.18 Huygens’s construction for (a) a plane wave propagating to the right and (b) a spherical wave propagating to the right.

▸ 35.5 c o n t i n u e d

A C

B D

1

2

gg!

u1

This wavelet was sent out by wave 1 from point A.

This wavelet was sent out at the same time by wave 2 from point B.

u!1

Figure 35.19 Huygens’s con-struction for proving the law of reflection.









Old wavefront

New wavefront

A B

Old wavefront

New wavefront

A! B!

c "t

c "t

a b



▸ 35.5 c o n t i n u e d

A C

B D

1

2

gg!

u1



u!1



Every point on a propagating wavefront can be thought of as thesource of a new spherical secondary wavelet. The wavefrontformed at a later time is the surface tangent (or envelope) of allthese wavelets.

Huygens’ PrincipleHuygens’ motivation for this principle was the idea of the existenceof an ether: each part of the light wave would interact withparticles composing the ether.

Now we know there is no ether.

This principle is still useful, since it gives us the correct idea ofwhat happens in various circumstances, including diffraction.

35.4 Analysis Model: Wave Under Reflection 1061

35.3 The Ray Approximation in Ray OpticsThe field of ray optics (sometimes called geometric optics) involves the study of the propagation of light. Ray optics assumes light travels in a fixed direction in a straight line as it passes through a uniform medium and changes its direction when it meets the surface of a different medium or if the optical properties of the medium are nonuniform in either space or time. In our study of ray optics here and in Chapter 36, we use what is called the ray approximation. To understand this approximation, first notice that the rays of a given wave are straight lines perpendicular to the wave fronts as illustrated in Figure 35.3 for a plane wave. In the ray approximation, a wave moving through a medium travels in a straight line in the direction of its rays. If the wave meets a barrier in which there is a circular opening whose diameter is much larger than the wavelength as in Figure 35.4a, the wave emerging from the opening continues to move in a straight line (apart from some small edge effects); hence, the ray approximation is valid. If the diameter of the opening is on the order of the wavelength as in Figure 35.4b, the waves spread out from the opening in all directions. This effect, called diffraction, will be studied in Chapter 37. Finally, if the opening is much smaller than the wavelength, the opening can be approxi-mated as a point source of waves as shown in Fig. 35.4c. Similar effects are seen when waves encounter an opaque object of dimension d. In that case, when l ,, d, the object casts a sharp shadow. The ray approximation and the assumption that l ,, d are used in this chapter and in Chapter 36, both of which deal with ray optics. This approximation is very good for the study of mirrors, lenses, prisms, and associated optical instruments such as telescopes, cameras, and eyeglasses.

35.4 Analysis Model: Wave Under ReflectionWe introduced the concept of reflection of waves in a discussion of waves on strings in Section 16.4. As with waves on strings, when a light ray traveling in one medium encounters a boundary with another medium, part of the incident light

From the particle under constant speed model, find the speed of the pulse of light:

c 52dDt

52 17 500 m 2

5.05 3 1025 s5 2.97 3 108 m/s

Finalize This result is very close to the actual value of the speed of light.

Rays

Wave fronts

The rays, which always point in the direction of the wave propagation, are straight lines perpendicular to the wave fronts.

Figure 35.3 A plane wave prop-agating to the right.

d

l ,, d l .. d

a b c

l ! d

When l ,, d, the rays continue in a straight-line path and the ray approximation remains valid.

When l ! d, the rays spread out after passing through the opening.

When l .. d, the opening behaves as a point source emitting spherical waves.

Figure 35.4 A plane wave of wavelength l is incident on a bar-rier in which there is an opening of diameter d.

▸ 35.1 c o n t i n u e d

1See page in the textbook for a derivation of Snell’s Law from Huygens’Principle.

Huygens-Fresnel Principle

Fresnel added the concept of interference to Huygens’ Principle,which explained the paths that rays of light seem to take.

Kirchhoff then showed that this new Huygens-Frensel Principle wasa consequence of the wave equation, so it can be expressed in arigorous mathematical way.

In fact, working from Kirchhoff’s mathematical approach, this ideacan be used to relate wavefronts at a light source to an image on ascreen using Fourier Transforms.

Young’s Double-Slit ExperimentThomas Young in 1801 did the first experiment that conclusivelyshowed the interference of light from 2 sources.

He filtered sunlight to make as source of red light, then shone thelight through a series of narrow apertures (slits).

The first screen blocks all but tiny source of light. This is calledthe collimating slit, and ensure the light reaching the other twoslits will be coherent.

1http://www.lightandmatter.com/

Young’s Double-Slit ExperimentThe filtered coherent light then goes through two slits cut from thesame mask. The light from these two sources interferes.

The light strikes a screen where bright and dark areas can be seen.

Young’s Double-Slit Experiment

If light could be modeled as a particle, then one would expect tosee two bright patches, one for each slit.

This is not what Young observed.

1http://www.studyphysics.ca

Young’s Double-Slit Experiment

A pattern of light and dark “fringes” (stripes of light and darkness)appear on the screen.

Zoomed in view:

Young’s Experiment: Interference

1136 Chapter 37 Wave Optics

the upper one by exactly one wavelength, they still arrive in phase at P and a sec-ond bright fringe appears at this location. At point R in Figure 37.3c, however, between points O and P, the lower wave has fallen half a wavelength behind the upper wave and a crest of the upper wave overlaps a trough of the lower wave, giv-ing rise to destructive interference at point R. A dark fringe is therefore observed at this location. If two lightbulbs are placed side by side so that light from both bulbs combines, no interference effects are observed because the light waves from one bulb are emitted independently of those from the other bulb. The emissions from the two lightbulbs do not maintain a constant phase relationship with each other over time. Light waves from an ordinary source such as a lightbulb undergo random phase changes in time intervals of less than a nanosecond. Therefore, the conditions for constructive interference, destructive interference, or some intermediate state are maintained only for such short time intervals. Because the eye cannot follow such rapid changes, no interference effects are observed. Such light sources are said to be incoherent. To observe interference of waves from two sources, the following conditions must be met:

The sources must be coherent; that is, they must maintain a constant phase with respect to each other.

The sources should be monochromatic; that is, they should be of a single wavelength.

As an example, single-frequency sound waves emitted by two side-by-side loud-speakers driven by a single amplifier can interfere with each other because the two speakers are coherent. In other words, they respond to the amplifier in the same way at the same time. A common method for producing two coherent light sources is to use a mono-chromatic source to illuminate a barrier containing two small openings, usually in the shape of slits, as in the case of Young’s experiment illustrated in Figure 37.1. The light emerging from the two slits is coherent because a single source produces the original light beam and the two slits serve only to separate the original beam into two parts (which, after all, is what is done to the sound signal from two side-by-side loudspeakers). Any random change in the light emitted by the source occurs in both beams at the same time. As a result, interference effects can be observed when the light from the two slits arrives at a viewing screen. If the light traveled only in its original direction after passing through the slits as shown in Figure 37.4a, the waves would not overlap and no interference pattern would be seen. Instead, as we have discussed in our treatment of Huygens’s prin-ciple (Section 35.6), the waves spread out from the slits as shown in Figure 37.4b. In other words, the light deviates from a straight-line path and enters the region that

Conditions for interference X

b

Constructive interference also occurs at point P.

Brightfringe

S1

S2

O

P

c

Destructive interference occurs at point R when the two waves combine because the lower wave falls one-half a wavelength behind the upper wave.

Darkfringe

P

R

O

S1

S2

a

Constructive interference occurs at point O when the waves combine.

Brightfringe

S1

S2

O

Viewing screen

Figure 37.3 Waves leave the slits and combine at various points on the viewing screen. (All figures not to scale.)

In places where the path lengths differ by a whole number ofwavelengths (mλ) there is constructive interference.

1Serway & Jewett.

Young’s Experiment: Finding the Maxima

Consider light that is diffracted through each slit and an angle ≈ θ.

37.2 Analysis Model: Waves in Interference 1137

would otherwise be shadowed. As noted in Section 35.3, this divergence of light from its initial line of travel is called diffraction.

37.2 Analysis Model: Waves in InterferenceWe discussed the superposition principle for waves on strings in Section 18.1, lead-ing to a one-dimensional version of the waves in interference analysis model. In Example 18.1 on page 537, we briefly discussed a two-dimensional interference phenomenon for sound from two loudspeakers. In walking from point O to point P in Figure 18.5, the listener experienced a maximum in sound intensity at O and a minimum at P. This experience is exactly analogous to an observer looking at point O in Figure 37.3 and seeing a bright fringe and then sweeping his eyes upward to point R, where there is a minimum in light intensity. Let’s look in more detail at the two-dimensional nature of Young’s experiment with the help of Figure 37.5. The viewing screen is located a perpendicular distance L from the barrier containing two slits, S1 and S2 (Fig. 37.5a). These slits are separated by a distance d, and the source is monochromatic. To reach any arbitrary point P in the upper half of the screen, a wave from the lower slit must travel farther than a wave from the upper slit. The extra distance traveled from the lower slit is the path differ-ence d (Greek letter delta). If we assume the rays labeled r1 and r2 are parallel (Fig. 37.5b), which is approximately true if L is much greater than d, then d is given by

d 5 r2 2 r1 5 d sin u (37.1)

The value of d determines whether the two waves are in phase when they arrive at point P. If d is either zero or some integer multiple of the wavelength, the two waves

a b

When we assume r1 is parallel to r2, the path difference between the two rays is r2 ! r1 " d sin u.

d " r2 ! r1 " d sin u

S1

S2

d

r2

r1

d

S1

S2 d

Q

LViewing screen

P

O

y

r1

r2u u u

Figure 37.5 (a) Geometric construction for describing Young’s double-slit experiment (not to scale). (b) The slits are represented as sources, and the outgoing light rays are assumed to be parallel as they travel to P. To achieve that in practice, it is essen-tial that L .. d.

a

Light passing through narrow slits does not behave this way.

b

Light passing through narrow slits diffracts.

Figure 37.4 (a) If light waves did not spread out after passing through the slits, no interference would occur. (b) The light waves from the two slits overlap as they spread out, filling what we expect to be shadowed regions with light and producing interference fringes on a screen placed to the right of the slits.


If the distance to the screen is very much larger that the distancebetween the slits (it will be), then φ is very small.

d

S1

S2 d

Q

LViewing screen

P

O

y

r1

r2u u

cosφ ≈ 1 and r1 = r2 − δ. The path difference is δ!


Effectively, the two rays are parallel.




d 5 r2 2 r1 5 d sin u (37.1)


a b


d " r2 ! r1 " d sin u

S1

S2

d

r2

r1

d

S1

S2 d

Q

LViewing screen

P

O

y

r1

r2u u u


a


b



Looking at the right triangle with hypotenuse d (the slit separationdistance): δ = d sin θ.

Young’s Experiment: Finding the Angles of theMaxima

Maxima (bright fringes) occur when

d sin θmax = mλ where m ∈ Z

Minima (dark fringes) occur when

d sin θmin =

(m +

1

2

)λ where m ∈ Z

These expressions give us the angles (measured outward from theaxis that passes through the midpoint of the slits) where the brightand dark fringes occur.

Order Number

m is the order number. The central bright fringe is the “0th orderfringe”, the neighboring ones are the “1st order fringes”, etc.

1Figure from Quantum Mechanics and the Multiverse by Thomas D. Le.

Young’s Experiment: Finding the Position of theMaxima

We can also predict the distance from the center of the screen, y ,in terms of the distance from the slits to the screen, L.




d 5 r2 2 r1 5 d sin u (37.1)


a b


d " r2 ! r1 " d sin u

S1

S2

d

r2

r1

d

S1

S2 d

Q

LViewing screen

P

O

y

r1

r2u u u


a


b



tan θ =y

L


Maxima (bright fringes) occur at

ymax = L tan θmax

Minima (dark fringes) occur at

ymin = L tan θmin


When θ is also small, sin θ ≈ tan θ, and we can use our earlierexpressions for the fringe angles.

Maxima (bright fringes) occur at

ymax = Lmλ

d(small θ)

Minima (dark fringes) occur at

ymin = L

(m + 1

2

)λ

d(small θ)

Young’s Experiment Question

Quick Quiz 37.11 Which of the following causes the fringes in atwo-slit interference pattern to move farther apart?

(A) decreasing the wavelength of the light

(B) decreasing the screen distance L

(C) decreasing the slit spacing d

(D) immersing the entire apparatus in water

1Serway & Jewett, page 1138.

Double-Slit Fringes of Two Wavelengths, Ex 37.2

A light source emits visible light of two wavelengths: λ = 430 nmand λ ′ = 510 nm. The source is used in a double-slit interferenceexperiment in which L = 1.50 m and d = 0.0250 mm.

Find the separation distance between the third-order bright fringesfor the two wavelengths.

Young’s Experiment: Intensity DistributionConsider the electric field at a certain point P on the screen fromeach slit:

E1 = E0 sin(ωt)

E2 = E0 sin(ωt + φ)

Using

sinα+ sinβ = 2 cos

(α− β

2

)sin

(α+ β

2

)We see that the net E-field at that point P is:

EP = E1 + E2

=

[2E0 cos

(φ

2

)]sin

(ωt +

φ

2

)Amplitude Time-fluctuation

Young’s Experiment: Intensity Distribution

EP,max = 2E0 cos

(φ

2

)Relating E-field to intensity, recall (Ch. 34):

I ∝ E 2P,max

So,

I = Imax cos2(φ

2

)The phase difference is related to δ, the path difference by:

φ

2π=δ

λ

So, using δ = d sin θ (and φ = 2πd sin θ/λ)

I = Imax cos2(πd sin θ

λ

)


I = Imax cos2(πd sin θ

λ

)


where Imax is the maximum intensity on the screen and the expression represents the time average. Substituting the value for f given by Equation 37.10 into this expression gives

I 5 Imax cos2 apd sin ul

b (37.14)

Alternatively, because sin u < y/L for small values of u in Figure 37.5, we can write Equation 37.14 in the form

I 5 Imax cos2 apdlL

yb 1small angles 2 (37.15)

Constructive interference, which produces light intensity maxima, occurs when the quantity pdy/lL is an integral multiple of p, corresponding to y 5 (lL/d)m, where m is the order number. This result is consistent with Equation 37.7. A plot of light intensity versus d sin u is given in Figure 37.6. The interference pat-tern consists of equally spaced fringes of equal intensity. Figure 37.7 shows similar plots of light intensity versus d sin u for light passing through multiple slits. For more than two slits, we would add together more electric field magnitudes than the two in Equation 37.9. In this case, the pattern contains primary and secondary maxima. For three slits, notice that the primary maxima are nine times more intense than the secondary maxima as measured by the height of the curve because the intensity varies as E 2. For N slits, the intensity of the primary maxima is N 2 times greater than that for the secondary maxima. As the number of slits increases, the primary maxima increase in intensity and become narrower, while the secondary maxima decrease in intensity relative to the primary maxima. Figure 37.7 also shows that as the number of slits increases, the number of sec-ondary maxima also increases. In fact, the number of secondary maxima is always N 2 2, where N is the number of slits. In Section 38.4, we shall investigate the pat-tern for a very large number of slits in a device called a diffraction grating.

Q uick Quiz 37.2 Using Figure 37.7 as a model, sketch the interference pattern from six slits.

N ! 2

0

Primary maximumSecondary maximum

IImax

d sin u"2l 2ll

For any value of N, the decrease in intensity in maxima to the left and right of the central maximum, indicated by the blue dashed arcs, is due to diffraction patterns from the individual slits, which are discussed in Chapter 38.

N ! 3

N ! 4

N ! 5

N ! 10 "l

Figure 37.7 Multiple-slit interference patterns. As N, the number of slits, is increased, the primary maxima (the tallest peaks in each graph) become narrower but remain fixed in position and the number of secondary maxima increases.

Figure 37.6 Light intensity versus d sin u for a double-slit interference pattern when the screen is far from the two slits (L .. d).

I

"2l 2l0

Imax

ld sin u

"l


E = 2E0 cos

(φ

2

)97135-6 I NTE N S ITY I N DOU B LE-S LIT I NTE R FE R E NCE

PART 4

Proof of Eqs. 35-22 and 35-23We shall combine the electric field components E1 and E2, given by Eqs. 35-20and 35-21, respectively, by the method of phasors as is discussed in Section 16-11.In Fig. 35-13a, the waves with components E1 and E2 are represented by phasorsof magnitude E0 that rotate around the origin at angular speed v. The valuesof E1 and E2 at any time are the projections of the corresponding phasors on thevertical axis. Figure 35-13a shows the phasors and their projections at an arbitrarytime t. Consistent with Eqs. 35-20 and 35-21, the phasor for E1 has a rotationangle vt and the phasor for E2 has a rotation angle vt ! f (it is phase-shiftedahead of E1). As each phasor rotates, its projection on the vertcal axis varies withtime in the same way that the sinusoidal functions of Eqs. 35-20 and 35-21 varywith time.

To combine the field components E1 and E2 at any point P in Fig. 35-10, weadd their phasors vectorially, as shown in Fig. 35-13b.The magnitude of the vectorsum is the amplitude E of the resultant wave at point P, and that wave has a cer-tain phase constant b.To find the amplitude E in Fig. 35-13b, we first note that thetwo angles marked b are equal because they are opposite equal-length sides ofa triangle. From the theorem (for triangles) that an exterior angle (here f, asshown in Fig. 35-13b) is equal to the sum of the two opposite interior angles (herethat sum is b ! b), we see that .Thus, we have

(35-28)

If we square each side of this relation, we obtain

(35-29)

Now, from Eq. 33-24, we know that the intensity of an electromagnetic wave isproportional to the square of its amplitude.Therefore, the waves we are combiningin Fig. 35-13b, whose amplitudes are E0, each has an intensity I0 that is proportionalto , and the resultant wave, with amplitude E, has an intensity I that is propor-tional to E2.Thus,

Substituting Eq. 35-29 into this equation and rearranging then yield

which is Eq. 35-22, which we set out to prove.We still must prove Eq. 35-23, which relates the phase difference f between

the waves arriving at any point P on the screen of Fig. 35-10 to the angle u thatserves as a locator of that point.

The phase difference f in Eq. 35-21 is associated with the path length differ-ence S1b in Fig. 35-10b. If S1b is , then f is p ; if S1b is l, then f is 2p, and so on.This suggests

(35-30)

The path length difference S1b in Fig. 35-10b is d sin u ; so Eq. 35-30 for the phasedifference between the two waves arriving at point P on the screen becomes

which is Eq. 35-23, the other equation that we set out to prove to relate f to theangle u that locates P.

" #2$d

% sin &,

! phasedifference" #

2$

% !path length

difference ".

12 %

I # 4I0 cos2 12 ",

II0

#E 2

E 02 .

E 02

E 2 # 4E 02 cos2 12 ".

# 2E0 cos 12 ".

E # 2(E0 cos ')

' # 12 "

Fig. 35-13 (a) Phasors representing, attime t, the electric field components givenby Eqs. 35-20 and 35-21. Both phasors havemagnitude E0 and rotate with angularspeed v.Their phase difference is f. (b)Vector addition of the two phasors givesthe phasor representing the resultant wave,with amplitude E and phase constant b.

(a)

E1 E0

ω t

ω E0

E2

φ

(b)

E1E0

ωt

E

E2

φβ

β

E0

ω

Phasors that representwaves can be added tofind the net wave.

halliday_c35_958-989hr.qxd 4-01-2010 10:02 Page 971

→

97135-6 I NTE N S ITY I N DOU B LE-S LIT I NTE R FE R E NCEPART 4

Proof of Eqs. 35-22 and 35-23We shall combine the electric field components E1 and E2, given by Eqs. 35-20and 35-21, respectively, by the method of phasors as is discussed in Section 16-11.In Fig. 35-13a, the waves with components E1 and E2 are represented by phasorsof magnitude E0 that rotate around the origin at angular speed v. The valuesof E1 and E2 at any time are the projections of the corresponding phasors on thevertical axis. Figure 35-13a shows the phasors and their projections at an arbitrarytime t. Consistent with Eqs. 35-20 and 35-21, the phasor for E1 has a rotationangle vt and the phasor for E2 has a rotation angle vt ! f (it is phase-shiftedahead of E1). As each phasor rotates, its projection on the vertcal axis varies withtime in the same way that the sinusoidal functions of Eqs. 35-20 and 35-21 varywith time.

To combine the field components E1 and E2 at any point P in Fig. 35-10, weadd their phasors vectorially, as shown in Fig. 35-13b.The magnitude of the vectorsum is the amplitude E of the resultant wave at point P, and that wave has a cer-tain phase constant b.To find the amplitude E in Fig. 35-13b, we first note that thetwo angles marked b are equal because they are opposite equal-length sides ofa triangle. From the theorem (for triangles) that an exterior angle (here f, asshown in Fig. 35-13b) is equal to the sum of the two opposite interior angles (herethat sum is b ! b), we see that .Thus, we have

(35-28)

If we square each side of this relation, we obtain

(35-29)

Now, from Eq. 33-24, we know that the intensity of an electromagnetic wave isproportional to the square of its amplitude.Therefore, the waves we are combiningin Fig. 35-13b, whose amplitudes are E0, each has an intensity I0 that is proportionalto , and the resultant wave, with amplitude E, has an intensity I that is propor-tional to E2.Thus,

Substituting Eq. 35-29 into this equation and rearranging then yield

which is Eq. 35-22, which we set out to prove.We still must prove Eq. 35-23, which relates the phase difference f between

the waves arriving at any point P on the screen of Fig. 35-10 to the angle u thatserves as a locator of that point.

The phase difference f in Eq. 35-21 is associated with the path length differ-ence S1b in Fig. 35-10b. If S1b is , then f is p ; if S1b is l, then f is 2p, and so on.This suggests

(35-30)

The path length difference S1b in Fig. 35-10b is d sin u ; so Eq. 35-30 for the phasedifference between the two waves arriving at point P on the screen becomes

which is Eq. 35-23, the other equation that we set out to prove to relate f to theangle u that locates P.

" #2$d

% sin &,

! phasedifference" #

2$

% !path length

difference ".

12 %

I # 4I0 cos2 12 ",

II0

#E 2

E 02 .

E 02

E 2 # 4E 02 cos2 12 ".

# 2E0 cos 12 ".

E # 2(E0 cos ')

' # 12 "

Fig. 35-13 (a) Phasors representing, attime t, the electric field components givenby Eqs. 35-20 and 35-21. Both phasors havemagnitude E0 and rotate with angularspeed v.Their phase difference is f. (b)Vector addition of the two phasors givesthe phasor representing the resultant wave,with amplitude E and phase constant b.

(a)

E1 E0

ω t

ω E0

E2

φ

(b)

E1E0

ωt

E

E2

φβ

β

E0

ω

Phasors that representwaves can be added tofind the net wave.


I = Imax cos2(φ

2

)

Interference with Three Slits

E1 = E0 sin(ωt) , E2 = E0 sin(ωt + φ) , E3 = E0 sin(ωt + 2φ)

Interference with Three Slits


where Imax is the maximum intensity on the screen and the expression represents the time average. Substituting the value for f given by Equation 37.10 into this expression gives

I 5 Imax cos2 apd sin ul

b (37.14)

Alternatively, because sin u < y/L for small values of u in Figure 37.5, we can write Equation 37.14 in the form

I 5 Imax cos2 apdlL

yb 1small angles 2 (37.15)

Constructive interference, which produces light intensity maxima, occurs when the quantity pdy/lL is an integral multiple of p, corresponding to y 5 (lL/d)m, where m is the order number. This result is consistent with Equation 37.7. A plot of light intensity versus d sin u is given in Figure 37.6. The interference pat-tern consists of equally spaced fringes of equal intensity. Figure 37.7 shows similar plots of light intensity versus d sin u for light passing through multiple slits. For more than two slits, we would add together more electric field magnitudes than the two in Equation 37.9. In this case, the pattern contains primary and secondary maxima. For three slits, notice that the primary maxima are nine times more intense than the secondary maxima as measured by the height of the curve because the intensity varies as E 2. For N slits, the intensity of the primary maxima is N 2 times greater than that for the secondary maxima. As the number of slits increases, the primary maxima increase in intensity and become narrower, while the secondary maxima decrease in intensity relative to the primary maxima. Figure 37.7 also shows that as the number of slits increases, the number of sec-ondary maxima also increases. In fact, the number of secondary maxima is always N 2 2, where N is the number of slits. In Section 38.4, we shall investigate the pat-tern for a very large number of slits in a device called a diffraction grating.

Q uick Quiz 37.2 Using Figure 37.7 as a model, sketch the interference pattern from six slits.

N ! 2

0


IImax

d sin u"2l 2ll

For any value of N, the decrease in intensity in maxima to the left and right of the central maximum, indicated by the blue dashed arcs, is due to diffraction patterns from the individual slits, which are discussed in Chapter 38.

N ! 3

N ! 4

N ! 5

N ! 10 "l

Figure 37.7 Multiple-slit interference patterns. As N, the number of slits, is increased, the primary maxima (the tallest peaks in each graph) become narrower but remain fixed in position and the number of secondary maxima increases.

Figure 37.6 Light intensity versus d sin u for a double-slit interference pattern when the screen is far from the two slits (L .. d).

I

"2l 2l0

Imax

ld sin u

"l

Interference Patterns from Many Slits

N ! 2

0


IImax

d sin u"2l 2ll

For any value of intensity in maxima to the left and right of the central maximum, indicated by the blue dashed arcs, is due to diffraction patternsthe individual slits, which are discussed in Chapter 38.

N ! 3

N ! 4

N ! 5

N ! 10 "l

Diffraction Grating

A diffraction grating is a device that works in a similar way toYoung’s two slits, but produces a brighter set of fringes for thesame source, and the bright fringes are narrower.

It breaks the light from a source up into very, very many coherentsources. (Young’s slit does the same, but only breaks the light into2 sources.)

It is used mainly for spectroscopy (determining the spectrum of atype of atom or molecule) and in monochromators (devices thatselect a particular frequency of light).

Interference Pattern from a Diffraction Grating

A diffraction grating has so many slits that effectively N →∞.

With monochromatic light, the peaks are sharp and well-separated.

1170 Chapter 38 Diffraction Patterns and Polarization

We can use this expression to calculate the wavelength if we know the grating spacing d and the angle ubright. If the incident radiation contains several wave-lengths, the mth-order maximum for each wavelength occurs at a specific angle. All wavelengths are seen at u 5 0, corresponding to m 5 0, the zeroth-order maximum. The first-order maximum (m 5 1) is observed at an angle that satisfies the relation-ship sin ubright 5 l/d, the second-order maximum (m 5 2) is observed at a larger angle ubright, and so on. For the small values of d typical in a diffraction grating, the angles ubright are large, as we see in Example 38.5. The intensity distribution for a diffraction grating obtained with the use of a monochromatic source is shown in Figure 38.13. Notice the sharpness of the principal maxima and the broadness of the dark areas compared with the broad bright fringes characteristic of the two-slit interference pattern (see Fig. 37.6). You should also review Figure 37.7, which shows that the width of the intensity maxima decreases as the number of slits increases. Because the principal maxima are so sharp, they are much brighter than two-slit interference maxima.

Q uick Quiz 38.5 Ultraviolet light of wavelength 350 nm is incident on a diffrac-tion grating with slit spacing d and forms an interference pattern on a screen a distance L away. The angular positions ubright of the interference maxima are large. The locations of the bright fringes are marked on the screen. Now red light of wavelength 700 nm is used with a diffraction grating to form another diffraction pattern on the screen. Will the bright fringes of this pattern be located at the marks on the screen if (a) the screen is moved to a distance 2L from the grating, (b) the screen is moved to a distance L/2 from the grating, (c) the grating is replaced with one of slit spacing 2d, (d) the grating is replaced with one of slit spacing d/2, or (e) nothing is changed?

d

P

Incoming planewave of light

First-ordermaximum(m ! 1)

First-ordermaximum(m ! "1)

Central orzeroth-ordermaximum(m ! 0)

Diffractiongrating

P

u u

d ! d sin u

Figure 38.12 Side view of a dif-fraction grating. The slit separa-tion is d, and the path difference between adjacent slits is d sin u.

0

m

2ld" d" d

2ld

llsin u

"2 "1 0 1 2

Figure 38.13 Intensity versus sin u for a diffraction grating. The zeroth-, first-, and second-order maxima are shown.

Conceptual Example 38.4 A Compact Disc Is a Diffraction Grating

Light reflected from the surface of a compact disc is multicolored as shown in Figure 38.14. The colors and their intensities depend on the orientation of the CD relative to the eye and rela-tive to the light source. Explain how that works.

The surface of a CD has a spiral grooved track (with adjacent grooves having a separation on

S O L U T I O N

Carlo

s E.

Sant

a M

aria

/Shu

tter

stoc

k.co

m

Figure 38.14 (Conceptual Example 38.4) A compact disc observed under white light. The colors observed in the reflected light and their intensities depend on the orientation of the CD relative to the eye and relative to the light source.

For light that is composed of several frequencies, the peaks foreach will be separated out.

Diffraction Gratings

There are two types of diffraction grating.Transmission gratings:

P





Diffractiongrating

P

Many slits allow light to pass through.

Diffraction Gratings

Reflection gratings:

Light reflects off of a series of mirrored surfaces.

1http://exoplanet.as.arizona.edu/∼lclose/a302/lecture14/lecture 14.html

Diffraction GratingWe can find the maxima (bright fringes) of the pattern produced ina diffraction grating in exactly the same way we did for Young’sslits.


We can use this expression to calculate the wavelength if we know the grating spacing d and the angle ubright. If the incident radiation contains several wave-lengths, the mth-order maximum for each wavelength occurs at a specific angle. All wavelengths are seen at u 5 0, corresponding to m 5 0, the zeroth-order maximum. The first-order maximum (m 5 1) is observed at an angle that satisfies the relation-ship sin ubright 5 l/d, the second-order maximum (m 5 2) is observed at a larger angle ubright, and so on. For the small values of d typical in a diffraction grating, the angles ubright are large, as we see in Example 38.5. The intensity distribution for a diffraction grating obtained with the use of a monochromatic source is shown in Figure 38.13. Notice the sharpness of the principal maxima and the broadness of the dark areas compared with the broad bright fringes characteristic of the two-slit interference pattern (see Fig. 37.6). You should also review Figure 37.7, which shows that the width of the intensity maxima decreases as the number of slits increases. Because the principal maxima are so sharp, they are much brighter than two-slit interference maxima.

Q uick Quiz 38.5 Ultraviolet light of wavelength 350 nm is incident on a diffrac-tion grating with slit spacing d and forms an interference pattern on a screen a distance L away. The angular positions ubright of the interference maxima are large. The locations of the bright fringes are marked on the screen. Now red light of wavelength 700 nm is used with a diffraction grating to form another diffraction pattern on the screen. Will the bright fringes of this pattern be located at the marks on the screen if (a) the screen is moved to a distance 2L from the grating, (b) the screen is moved to a distance L/2 from the grating, (c) the grating is replaced with one of slit spacing 2d, (d) the grating is replaced with one of slit spacing d/2, or (e) nothing is changed?

d

P





Diffractiongrating

P

u u

d ! d sin u

Figure 38.12 Side view of a dif-fraction grating. The slit separa-tion is d, and the path difference between adjacent slits is d sin u.

0

m

2ld" d" d

2ld

llsin u

"2 "1 0 1 2

Figure 38.13 Intensity versus sin u for a diffraction grating. The zeroth-, first-, and second-order maxima are shown.

Conceptual Example 38.4 A Compact Disc Is a Diffraction Grating

Light reflected from the surface of a compact disc is multicolored as shown in Figure 38.14. The colors and their intensities depend on the orientation of the CD relative to the eye and rela-tive to the light source. Explain how that works.

The surface of a CD has a spiral grooved track (with adjacent grooves having a separation on

S O L U T I O N

Carlo

s E.

Sant

a M

aria

/Shu

tter

stoc

k.co

m

Figure 38.14 (Conceptual Example 38.4) A compact disc observed under white light. The colors observed in the reflected light and their intensities depend on the orientation of the CD relative to the eye and relative to the light source.

Diffraction Grating

Once again, light from different slits interferes constructively whenthe path differnce δ = mλ (m is an integer).

δ = d sin θ

Maxima (bright fringes) occur when

d sin θmax = mλ where m ∈ Z

Diffraction

We already know that light and other waves that travel through asmall gap (< λ) diverge, and that the smaller the gap, the moredivergence.

35.4 Analysis Model: Wave Under Reflection 1061

35.3 The Ray Approximation in Ray OpticsThe field of ray optics (sometimes called geometric optics) involves the study of the propagation of light. Ray optics assumes light travels in a fixed direction in a straight line as it passes through a uniform medium and changes its direction when it meets the surface of a different medium or if the optical properties of the medium are nonuniform in either space or time. In our study of ray optics here and in Chapter 36, we use what is called the ray approximation. To understand this approximation, first notice that the rays of a given wave are straight lines perpendicular to the wave fronts as illustrated in Figure 35.3 for a plane wave. In the ray approximation, a wave moving through a medium travels in a straight line in the direction of its rays. If the wave meets a barrier in which there is a circular opening whose diameter is much larger than the wavelength as in Figure 35.4a, the wave emerging from the opening continues to move in a straight line (apart from some small edge effects); hence, the ray approximation is valid. If the diameter of the opening is on the order of the wavelength as in Figure 35.4b, the waves spread out from the opening in all directions. This effect, called diffraction, will be studied in Chapter 37. Finally, if the opening is much smaller than the wavelength, the opening can be approxi-mated as a point source of waves as shown in Fig. 35.4c. Similar effects are seen when waves encounter an opaque object of dimension d. In that case, when l ,, d, the object casts a sharp shadow. The ray approximation and the assumption that l ,, d are used in this chapter and in Chapter 36, both of which deal with ray optics. This approximation is very good for the study of mirrors, lenses, prisms, and associated optical instruments such as telescopes, cameras, and eyeglasses.

35.4 Analysis Model: Wave Under ReflectionWe introduced the concept of reflection of waves in a discussion of waves on strings in Section 16.4. As with waves on strings, when a light ray traveling in one medium encounters a boundary with another medium, part of the incident light

From the particle under constant speed model, find the speed of the pulse of light:

c 52dDt

52 17 500 m 2

5.05 3 1025 s5 2.97 3 108 m/s

Finalize This result is very close to the actual value of the speed of light.

Rays

Wave fronts

The rays, which always point in the direction of the wave propagation, are straight lines perpendicular to the wave fronts.

Figure 35.3 A plane wave prop-agating to the right.

d

l ,, d l .. d

a b c

l ! d

When l ,, d, the rays continue in a straight-line path and the ray approximation remains valid.

When l ! d, the rays spread out after passing through the opening.

When l .. d, the opening behaves as a point source emitting spherical waves.

Figure 35.4 A plane wave of wavelength l is incident on a bar-rier in which there is an opening of diameter d.

▸ 35.1 c o n t i n u e d

The intensity of light in each direction is not the same however.

Diffraction Patterns


a Fraunhofer diffraction pattern. A bright fringe is observed along the axis at u 5 0, with alternating dark and bright fringes on each side of the central bright fringe. Until now, we have assumed slits are point sources of light. In this section, we abandon that assumption and see how the finite width of slits is the basis for under-standing Fraunhofer diffraction. We can explain some important features of this phenomenon by examining waves coming from various portions of the slit as shown in Figure 38.5. According to Huygens’s principle, each portion of the slit acts as a source of light waves. Hence, light from one portion of the slit can interfere with light from another portion, and the resultant light intensity on a viewing screen depends on the direction u. Based on this analysis, we recognize that a diffraction pattern is actually an interference pattern in which the different sources of light are different portions of the single slit! Therefore, the diffraction patterns we discuss in this chapter are applications of the waves in interference analysis model. To analyze the diffraction pattern, let’s divide the slit into two halves as shown in Figure 38.5. Keeping in mind that all the waves are in phase as they leave the slit, consider rays 1 and 3. As these two rays travel toward a viewing screen far to the right of the figure, ray 1 travels farther than ray 3 by an amount equal to the path difference (a/2) sin u, where a is the width of the slit. Similarly, the path difference between rays 2 and 4 is also (a/2) sin u, as is that between rays 3 and 5. If this path difference is exactly half a wavelength (corresponding to a phase difference of 180°), the pairs of waves cancel each other and destructive interference results. This cancel-lation occurs for any two rays that originate at points separated by half the slit width because the phase difference between two such points is 180°. Therefore, waves from the upper half of the slit interfere destructively with waves from the lower half when

a2

sin u 5l

2

or, if we consider waves at angle u both above the dashed line in Figure 38.5 and below,

sin u 5 6l

a

Dividing the slit into four equal parts and using similar reasoning, we find that the viewing screen is also dark when

sin u 5 62 l

a

Likewise, dividing the slit into six equal parts shows that darkness occurs on the screen when

sin u 5 63 l

a

Pitfall Prevention 38.1Diffraction Versus Diffraction Pattern Diffraction refers to the general behavior of waves spread-ing out as they pass through a slit. We used diffraction in explaining the existence of an interference pattern in Chapter 37. A diffraction pattern is actually a misnomer, but is deeply entrenched in the lan-guage of physics. The diffraction pattern seen on a screen when a single slit is illuminated is actually another interference pattern. The interference is between parts of the incident light illuminating dif-ferent regions of the slit.

Figure 38.4 (a) Geometry for analyzing the Fraunhofer diffrac-tion pattern of a single slit. (Draw-ing not to scale.) (b) Simulation of a single-slit Fraunhofer diffrac-tion pattern.

Slit

min

min

min

min

max

max

max

Incomingwave Viewing screen

u

The pattern consists of a central bright fringe flanked by much weaker maxima alternating with dark fringes.

a b

L

Each portion of the slit acts as a point source of light waves.

a

a/2

a/2

2

3

2

5

4

1

u

The path difference between rays 1 and 3, rays 2 and 4, or rays 3 and 5 is (a/ 2) sin u.

sin ua

Figure 38.5 Paths of light rays that encounter a narrow slit of width a and diffract toward a screen in the direction described by angle u (not to scale).

Diffraction Spikes

1NASA, ESA, and H. Richer (University of British Columbia); SvonHalenbach

Diffraction Spikes in Camera Apertures

Iris diaphragms adjust the amount of light allowed into a camerabody.

They cause characteristic diffraction patterns on photos taken ofbright lights.

1Wikipedia user Cmglee

Diffraction Patterns: Arago SpotDirectly in the center of the shadow produced by a round object litwith coherent light, a spot of light can be observed!

This is called the Arago spot, Fresnel bright spot, or Poisson spot.

1Photo taken at Exploratorium in SF, own work.

Understanding the Diffraction Pattern from a SingleSlit



a2

sin u 5l

2


sin u 5 6l

a


sin u 5 62 l

a


sin u 5 63 l

a



Slit

min

min

min

min

max

max

max


u


a b

L


a

a/2

a/2

2

3

2

5

4

1

u


sin ua


Diffraction and Huygens’ PrincipleWhen we have a slit or aperture illuminated by coherent light, eachpart of the aperture acts as a point source of spherical wavelets.








Old wavefront

New wavefront

A B

Old wavefront

New wavefront

A! B!

c "t

c "t

a b



▸ 35.5 c o n t i n u e d

A C

B D

1

2

gg!

u1



u!1


These wavelets interfere to produce a diffraction pattern.


Consider a series of point sources in different parts of the slit. Theslit has width a.



a2

sin u 5l

2


sin u 5 6l

a


sin u 5 62 l

a


sin u 5 63 l

a



Slit

min

min

min

min

max

max

max


u


a b

L


a

a/2

a/2

2

3

2

5

4

1

u


sin ua



We can find minima (dark fringes) in the pattern by breaking upour point sources into pairs that cancel each other out.

Matching point sources in the top half of the slit with ones in thebottom half, the source separation distances will be d = a/2.

This will be a fringe dark when:

δ =a

2sin θ =

λ

2


However, we could also break the slit up into 4 equal parts andmatch sources from the 1st and 2nd, and match from the 3rd and4th.

This will be dark when:

δ =a

4sin θ =

λ

2

If we break the slit up into 6 equal parts and match sources fromthe 1st and 2nd, the 3rd and 4th, and the 5th and 6th.

This will be dark when:

δ =a

6sin θ =

λ

2


In general we expect dark fringes when:

sin θmin = mλ

awhere m = ±1,±2,±3, ...

Question



a2

sin u 5l

2


sin u 5 6l

a


sin u 5 62 l

a


sin u 5 63 l

a



Slit

min

min

min

min

max

max

max


u


a b

L


a

a/2

a/2

2

3

2

5

4

1

u


sin ua


Quick Quiz 38.12 Suppose the slit width in the figure is madehalf as wide. Does the central bright fringe

(A) become wider,

(B) remain the same, or

(C) become narrower?

2Serway & Jewett, page 1163.

The Intensity Pattern from a Single Slit

For a single slit:

I = Imax

(sin((πa/λ) sin θ)

(πa/λ) sin θ)

)2

This is a sinc-function squared.

Just to check, we said the minima should be

sin θmin = mλ

a

This corresponds tosin((πa/λ) sin θmin) = 0 ⇒ (πa/λ) sin θmin = mπ

The Intensity Pattern from a Single Slit996 CHAPTE R 36 DI FFRACTION

We assume that the wavelets arriving at P all have the same amplitude !E.To find the amplitude Eu of the resultant wave at P, we add the amplitude !E viaphasors. To do this, we construct a diagram of N phasors, one corresponding tothe wavelet from each zone in the slit.

For point P0 at u " 0 on the central axis of Fig. 36-4, Eq. 36-4 tells us that thephase difference !f between the wavelets is zero; that is, the wavelets all arrive inphase. Figure 36-7a is the corresponding phasor diagram; adjacent phasorsrepresent wavelets from adjacent zones and are arranged head to tail. Becausethere is zero phase difference between the wavelets, there is zero angle betweeneach pair of adjacent phasors.The amplitude Eu of the net wave at P0 is the vectorsum of these phasors.This arrangement of the phasors turns out to be the one thatgives the greatest value for the amplitude Eu. We call this value Em; that is, Em isthe value of Eu for u " 0.

Fig. 36-7 Phasor diagrams for N " 18 phasors, corresponding tothe division of a single slit into 18zones. Resultant amplitudes Eu areshown for (a) the central maximumat u " 0, (b) a point on the screen ly-ing at a small angle u to the centralaxis, (c) the first minimum, and (d)the first side maximum.

E = 0

I

θ

(c)

Eθ

(d)

Eθ

(b)

E (= Em)θ

E∆

⎧ ⎨ ⎩

(a)

Phasor fortop ray

Phasor forbottom ray

θHere, with an even largerphase difference, they addto give a small amplitudeand thus a small intensity.

The last phasor is out ofphase with the first phasorby 2 rad (full circle).

Here, with a larger phasedifference, the phasors addto give zero amplitude andthus a minimum in the pattern.

Here the phasors have a smallphase difference and add to givea smaller amplitude and thusless intensity in the pattern.

The phasors from the 18 zonesin the slit are in phase and addto give a maximum amplitudeand thus the central maximumin the diffraction pattern.

π

A


Two Slits that have some width

Suppose two slits each have width a and their centers are adistance d apart.

What intensity pattern do they create?

Two Slits that have some width 38.2 Diffraction Patterns from Narrow Slits 1165

blue curve in Figure 38.7 represents the factor in square brackets in Equation 38.3. The cosine-squared factor by itself would give a series of peaks all with the same height as the highest peak of the red-brown curve in Figure 38.7. Because of the effect of the square-bracket factor, however, these peaks vary in height as shown. Equation 37.2 indicates the conditions for interference maxima as d sin u 5 ml, where d is the distance between the two slits. Equation 38.1 specifies that the first diffraction minimum occurs when a sin u 5 l, where a is the slit width. Dividing Equation 37.2 by Equation 38.1 (with m 5 1) allows us to determine which interfer-ence maximum coincides with the first diffraction minimum:

d sin ua sin u

5ml

l

da 5 m (38.4)

In Figure 38.7, d/a 5 18 mm/3.0 mm 5 6. Therefore, the sixth interference maxi-mum (if we count the central maximum as m 5 0) is aligned with the first diffrac-tion minimum and is dark.

Q uick Quiz 38.2 Consider the central peak in the diffraction envelope in Figure 38.7 and look closely at the horizontal scale. Suppose the wavelength of the light is changed to 450 nm. What happens to this central peak? (a) The width of the peak decreases, and the number of interference fringes it encloses decreases. (b) The width of the peak decreases, and the number of interference fringes it encloses increases. (c) The width of the peak decreases, and the number of interference fringes it encloses remains the same. (d) The width of the peak increases, and the number of interference fringes it encloses decreases. (e) The width of the peak increases, and the number of interference fringes it encloses increases. (f) The width of the peak increases, and the number of interference fringes it encloses remains the same. (g) The width of the peak remains the same, and the number of interference fringes it encloses decreases. (h) The width of the peak remains the same, and the number of interference fringes it encloses increases. (i) The width of the peak remains the same, and the number of interference fringes it encloses remains the same.

!3p !2p 2p 3p!p p

The diffraction pattern acts as an “envelope” (the blue dashed curve) that controls the intensity of the regularly spaced interference maxima.

I

Diffractionminima

Interferencefringes

a sin ulp

Figure 38.7 The combined effects of two-slit and single-slit interference. This pattern is pro-duced when 650-nm light waves pass through two 3.0-mm slits that are 18 mm apart.

Resolution and the Rayleigh criterion

We use optical systems like our eyes, a camera, or a telescope toview distant objects and interpret them.

Imagine two distant stars. If they are very close together, or so faraway that they make a very small angle to each other in the sky,they may look like only one star.

When can we distinguish them as two separate points?



38.3 Resolution of Single-Slit and Circular AperturesThe ability of optical systems to distinguish between closely spaced objects is lim-ited because of the wave nature of light. To understand this limitation, consider Figure 38.8, which shows two light sources far from a narrow slit of width a. The sources can be two noncoherent point sources S1 and S2; for example, they could be two distant stars. If no interference occurred between light passing through dif-ferent parts of the slit, two distinct bright spots (or images) would be observed on the viewing screen. Because of such interference, however, each source is imaged as a bright central region flanked by weaker bright and dark fringes, a diffraction pattern. What is observed on the screen is the sum of two diffraction patterns: one from S1 and the other from S2. If the two sources are far enough apart to keep their central maxima from over-lapping as in Figure 38.8a, their images can be distinguished and are said to be resolved. If the sources are close together as in Figure 38.8b, however, the two cen-tral maxima overlap and the images are not resolved. To determine whether two images are resolved, the following condition is often used:

When the central maximum of one image falls on the first minimum of another image, the images are said to be just resolved. This limiting condition of resolution is known as Rayleigh’s criterion.

From Rayleigh’s criterion, we can determine the minimum angular separation umin subtended by the sources at the slit in Figure 38.8 for which the images are just resolved. Equation 38.1 indicates that the first minimum in a single-slit diffraction pattern occurs at the angle for which

sin u 5l

a

where a is the width of the slit. According to Rayleigh’s criterion, this expres-sion gives the smallest angular separation for which the two images are resolved. Because l ,, a in most situations, sin u is small and we can use the approximation sin u < u. Therefore, the limiting angle of resolution for a slit of width a is

umin 5l

a (38.5)

where umin is expressed in radians. Hence, the angle subtended by the two sources at the slit must be greater than l/a if the images are to be resolved. Many optical systems use circular apertures rather than slits. The diffraction pat-tern of a circular aperture as shown in the photographs of Figure 38.9 consists of

a b

Slit Viewing screen Slit Viewing screen

uu

The angle subtended by the sources at the slit is large enough for the diffraction patterns to be distinguishable.

The angle subtended by the sources is so small that their diffraction patterns overlap, and the images are not well resolved.

S1

S2

S1

S2

Figure 38.8 Two point sources far from a narrow slit each pro-duce a diffraction pattern. (a) The sources are separated by a large angle. (b) The sources are sepa-rated by a small angle. (Notice that the angles are greatly exaggerated. The drawing is not to scale.)

When the central maximum of one falls on the first dark fringe ofthe other, the two images begin to look like they came from oneobject.

θmin ≈ sin θmin =λ

a

Resolution and the Rayleigh criterion 38.3 Resolution of Single-Slit and Circular Apertures 1167

a central circular bright disk surrounded by progressively fainter bright and dark rings. Figure 38.9 shows diffraction patterns for three situations in which light from two point sources passes through a circular aperture. When the sources are far apart, their images are well resolved (Fig. 38.9a). When the angular separation of the sources satisfies Rayleigh’s criterion, the images are just resolved (Fig. 38.9b). Finally, when the sources are close together, the images are said to be unresolved (Fig. 38.9c) and the pattern looks like that of a single source. Analysis shows that the limiting angle of resolution of the circular aperture is

umin 5 1.22 l

D (38.6)

where D is the diameter of the aperture. This expression is similar to Equation 38.5 except for the factor 1.22, which arises from a mathematical analysis of diffraction from the circular aperture.

Q uick Quiz 38.3 Cat’s eyes have pupils that can be modeled as vertical slits. At night, would cats be more successful in resolving (a) headlights on a distant car or (b) vertically separated lights on the mast of a distant boat?

Q uick Quiz 38.4 Suppose you are observing a binary star with a telescope and are having difficulty resolving the two stars. You decide to use a colored filter to maximize the resolution. (A filter of a given color transmits only that color of light.) What color filter should you choose? (a) blue (b) green (c) yellow (d) red

�W Limiting angle of resolution for a circular aperture

a b c

The sources are far apart, and the patterns are well resolved.

The sources are so close together that the patterns are not resolved.

The sources are closer together such that the angular separation satisfies Rayleigh’s criterion, and the patterns are just resolved.

Figure 38.9 Individual diffraction patterns of two point sources (solid curves) and the resultant patterns (dashed curves) for various angular separations of the sources as the light passes through a circular aperture. In each case, the dashed curve is the sum of the two solid curves.

Example 38.2 Resolution of the Eye

Light of wavelength 500 nm, near the center of the visible spectrum, enters a human eye. Although pupil diameter var-ies from person to person, let’s estimate a daytime diameter of 2 mm.

(A) Estimate the limiting angle of resolution for this eye, assuming its resolution is limited only by diffraction.

Conceptualize Identify the pupil of the eye as the aperture through which the light travels. Light passing through this small aperture causes diffraction patterns to occur on the retina.

Categorize We determine the result using equations developed in this section, so we categorize this example as a sub-stitution problem.

S O L U T I O N

continued


For circular points being resolved, the Rayleigh Criterion is:

θmin = 1.22λ

D

where D is the diameter of the aperture.

The 1.22 factor comes from a full analysis of the 2-dimensionaldiffraction pattern for a circular aperture.

Summary• Huygen’s principle

• two-slit interference

• multiple slit interference

• diffraction gratings

• diffraction patterns

• diffraction and interference

• resolution and Raleigh’s criterion

Final Exam 6:15-8:15pm, Monday, June 26.

Homework Serway & Jewett:

• Ch 37, onward from page 1150. OQs: 3, 9; CQs: 3, 5; Probs:1, 3, 5, 13, 19, 21, 25, 51, 60

• Ch 38, onward from page 1182. OQs: 3, 5; CQs: 5; Probs: 1,7, 10, 15, 21, 25, 60

Optics Wave Behavior in Optics - De Anza...

Documents

Transcript of Optics Wave Behavior in Optics - De Anza...