The law of reflection can be stated as follows: The angle ofincidence equals the angle of reflection.A spherical concave mirror reflects light toward a point on thecentral radius called
Trang 1The law of reflection can be stated as follows: The angle ofincidence equals the angle of reflection.
A spherical concave mirror reflects light toward a point on thecentral radius called the focal point The radius of curvature is thedistance from the mirror to its center if the mirror were a fullsphere This is called the principal axis
Concave spherical mirrors are important tools in science because
of their ability to focus incident light The point where incidentrays are focused is called the focal point and is one half the radius
of curvature
f =r2
Trang 2Two rules worth remembering about light rays that strike a cave mirror are:
1 Any light ray that is moving parallel to the principal axis and isincident to the mirror will be reflected though the focal point
2 Any light ray that passes through the focal point and is incident
to the mirror will be reflected parallel to the principal axis
Light rays from objects (O) placed in front of a concave mirror produce images (I).
The images produced may be real (projectable onto a screen)
or virtual (appearing to be located on the other side of the mirror);they may be enlarged (magnified) or shrunk (reduced); or they may
be right side up (erect) or upside down (inverted)
The following diagrams illustrate the position of the imagewhen the object is placed in various locations in front of themirror
Object distance is considered infinite
Light rays are parallel as they approach and strike the mirror
Image is located at f It is reduced, inverted, and real.
Trang 3Object is located at r.
Image is located at r It is the same size as the object, inverted, and
real
Object is located between r and f.
Image is located beyond r It is magnified, inverted, and real.
Object is located inside f.
Image is located behind the mirror It is reduced, erect, and virtual
Trang 4The letters I and O are used to represent the height of the image (I) and the height of the object (O) The distance from the mirror to the image is labeled q and the distance from the mirror
to the object is labeled p.
Mirrors are used in a variety of ways throughout the world.Shopkeepers use convex mirrors to keep an eye on the aisles oftheir stores, and sharp corners on roadways have mirrors set out
so drivers can see the road ahead The magnifying capability ofmirrors allows astronomers and laboratory researchers to performtheir work
This capability of a mirror is based upon the set of ratios (ofthe object and image heights) compared to the distance of theobject and the image from the mirror
h h
q p
Object is located in front of the mirror
Image is located behind the mirror and appears to be inside it It isreduced, erect, and virtual
The equation that describes the location of an image in amirror is called the mirror equation
1 1 1
f = +p q
The focal length (f) is positive for concave mirrors and negative for convex mirrors If the image (q) or the object (p) are located in front of the mirror, they are positive If the image (q) and/or the
object is/are located behind the mirror, it is negative
Trang 5Let’s do a typical reflection problem
Find the location of the image for an object that is placed 37
cm in front of a mirror having a focal length of 3.6 cm Describethe image
1025
The image is located 4 cm from the mirror The object is outside
the radius of curvature (2f = 7.2 cm), and the image is located between r and f It is reduced, inverted, and real.
Now we’ll use the original information from the problemabove, but we’ll replace the concave mirror with a convex mirror
cm cmcm
0027
Trang 6The image is located 3.29 cm behind the mirror (the negative sign
for q) It is reduced, erect, and virtual.
REFRACTION
Waves that move into a new medium bend as they enter the dium All waves can be refracted, but our discussion here will belimited to light The light beam shown below passes from air into
me-a cube of plme-astic
At the air/plastic boundary, the light ray bends (refracts) towardthe normal when the light ray passes into the plastic The raymoves in a straight line while in the plastic until it reenters the air
At the plastic/air boundary the light ray bends (refracts) awayfrom the normal
When light enters an optically more dense material, it refractstoward the normal When it enters an optically less dense material,
it refracts away from the normal
Trang 7The mathematical relationship between the velocity of light inone material (usually air) compared to another material was
determined to be
n1sinθ1=n2sinθ2 (Snell’s Law),
where n is the index of refraction of the material through which
light is passing
Example
A typical Snell’s Law problem is one where a scuba diver shines alight upward into the air from under the water The light beammakes an angle of 30° from the vertical What is the angle of thelight beam as it enters the air?
Solution
The index of refraction (n) for water is 1.33 and for air is 1.
Stating Snell’s Law
n n
1 1 2 2 2
1 1 2 2
2
1 33 5
1 655
sin sinsin sin
sin ( )( ) sin
θθ
Lenses are important because they can focus light Convexlenses converge light rays passing through them toward the focal
point f This kind of lens is called convergent Concave lenses
separate light rays passing through them as if the separated lightrays had originated at the focal point This kind of lens is calleddivergent The two light rays of which to take note are:
• A light ray that is parallel to the principal axis and is incident uponthe lens will be refracted through the focal point (on the other side
of the lens)
Trang 8• A light ray that passes through the focal point and is incident uponthe lens will be refracted parallel to the principal axis (on the otherside).
Light rays from object (O) placed in front of a curved lens produce images (I) The diagrams below illustrate the position of
the image when the object is placed in various positions
Object distance is considered infinite
Light rays are parallel
Image is located at f It is reduced, inverted, and real.
Object distance is outside 2f but not infinite.
Image is located between 2f and f It is reduced, inverted, and real.
Trang 9Image same side and outside object; magnified, erect, and virtual.
The lens equation 1 1 1
f = +p q is the same as the equation used for
mirrors Remember though, the image distance (q) is positive
when on the opposite side of the lens
Trang 10Concave lenses produce virtual images.
As with the mirror equation, the lens equations can be used tolocate an image
1 1
125 05 1
1075
f p q
q q q
Trang 11Polarization is a phenomenon that applies only to transversewaves Light is a transverse wave and is commonly the object ofpolarization Let’s examine polarization by considering a rope tied
to a fixed end Vibrating the rope up and down produces wavesthat travel down the rope
Should we stand beside the rope and hold a meter stick verticallybeside the rope, there is no problem
The rope vibrates on the vertical axis, and the meter stick is ented on the vertical axis If we change the orientation of the stick
ori-to the horizontal axis, the vertical vibrations in the rope strike thehorizontal meter stick
Transverse waves are almost completely stopped when they reachthe meter stick
We can take these results a step further and apply them tolight Light is considered a transverse wave that only differs fromour rope example in that light vibrates 360° around the line path
of the light ray
Trang 12The polarized eyeglasses many people wear restrict the intensity
of the light that reaches their eyes by using a device (polarizer)that only allows light vibrating on one plane to pass through tothe eye
The result is similar to holding a meter stick over a rope that isvibrating up and down, but with the plane polarizer, every planebut one is polarized at the same time
DIFFRACTION AND INTERFERENCE
Water waves approaching a fixed object in their path tend to movearound the object and continue on their way The ability of waves
to bend around obstacles in their path is called diffraction
Like-wise, waves that strike a barrier in which there are openings havethe ability to pass through the opening The opening acts as a newsource of waves that radiate out from the source
Trang 13Suppose the barrier has two holes Then each hole acts as a newsource of waves.
The area of waves beyond the barrier is filled with a confusion ofwaves crossing one another A series of peaks and troughs exists
as waves both constructively and destructively interfere with oneanother
Thomas Young (1801) tested light in this manner using a
double slit Since the confused waves were light waves, Youngdecided he could project the results onto a screen Young learnedthat the light waves would interfere with one another in a waythat produced areas of constructive interference (light spots) anddestructive interference (dark spots)
Trang 14The light traveling from Slit 1 (S1) travels a number of whole
wavelengths (nλ) to reach the screen at P1 Additionally, the light from Slit 2 (S2) would travel the same number of whole wave-
lengths plus one more, nλ + 1 Typically more than one bright spot
on the fringe is visible The central (zeroth) fringe is the fringe
where the light path is exactly equal for both S1 and S2 The firstfringe on either side of the zeroth fringe is called the first orderfringe, the second is the second order fringe, etc The number ofthe fringe is the number of extra wavelengths traveled by the lightray on the longest path
nλ= sind θ
Example
Let’s find the wavelength of the green-yellow mercury spectralline The grating used has a spacing of 1 × 10–6m, and the anglebetween the zeroth and first fringe is 33.l° Write the equation and
remember n = 1 in this case.
and sin
If the angle to the fourth order fringe of a blue light is known to
be 3.9°, and the distance between slits is 0025 cm, find the length of the light
Trang 15( )
and
cm100cm/m
4
40025
6 8 102
4
4 25 10 7 425
λ = × − or nm
Trang 16CHAPTER SUMMARY
• Waves are periodic vibrations that carry energy
• Interference can be constructive or destructive
• The velocity of a wave is a product of its frequency and
wavelength v = λ f.
• Sound is a longitudinal wave
• Light is a transverse wave
• Mirrors reflect light
• The law of reflection is stated as ∠i = ∠r.
• A concave mirror reflects light toward the focal point
• A convex mirror reflects light as if the rays had passedthrough a focal point on the other side of the mirror
• The mirror equation
1 1 1
f = +p q is the same for both concaveand convex mirrors: f is positive for concave mirrors, and f is
negative for convex mirrors
• Light passing between two transparent materials is refracted
at the surface boundary of the materials
• Snell’s Law is n1 sinθ1 = n2 sinθ2 where n is the index of
refrac-tion for the materials, and θ is the angle of refraction
• A convex lens (converging) refracts light toward a focal point
• A concave lens (diverging) refracts light as if it had passedthrough a focal point and the other side of the lens
• The lens equation
1 1 1
f = +p q is identical in form to the mirrorequation However, q is positive when the image is located on the opposite side of the lens from p the object.
• Light that has had all its vibrations eliminated except for those
on a single plane is plane polarized
• Diffraction is the ability of waves to bend around barriersplaced in their way
• Interference is the constructive or the destructive
Trang 18superposi-Chapter 4
HEA
HEAT T T AND AND AND THERMOD THERMOD THERMODYN YN YNAMICS AMICS
Trang 20CHAPTER 4
HEA HEAT T T AND AND AND THERMOD THERMOD THERMODYN YN YNAMICS AMICS
TEMPERATURE
The atoms and molecules of which matter is made are constantly inmotion The more energy they contain, the faster they move Thekinetic energy the particles have is called internal energy A hot bodyhas more internal energy than a cold body The measure of the inter-nal energy of a body is called temperature The temperature of anobject is not dependent on the amount of the substance present andcan be measured with a thermometer
• Temperature scales are the method by which the heat energy ofbodies can be compared They are often based on an arbitrarypoint
• The Fahrenheit scale was devised to read 0°F as the coldest perature reached on earth and 100°F as the hottest material tem-perature on the earth The freezing point of water is 32°F and itsboiling point is 212°F
tem-• The Celsius scale was devised to measure between the freezing andboiling points of water The freezing point of water on the Celsius
scale is 0°C, and the boiling point of water is 100°C.
• The Kelvin or absolute scale places 0K at the point where there is
no heat, thus no lower temperature is possible Zero on the Kelvinscale is absolute, thus absolute zero means no heat energy is
present Note the degree sign is not used on the Kelvin or lute scale.
abso-• There are 180 degrees between the freezing and boiling points ofwater on the Fahrenheit scale
• There are 100degrees between the freezing and boiling points ofwater on the Celsius scale
• The Kelvin scale places the freezing point of water at 273K and the boiling point of water at 373K, which is also a 100-unit difference.
The Celsius and the Kelvin scales have a 1:1 relationship Thus to
change °C to K, all that’s necessary is to add 273 to the Celsius
temperature
Trang 21THERMAL PROPERTIES OF MATTER
Thermal energy is the energy substances possess when their ture is greater than absolute zero As energy is added, most sub-stances expand You have probably seen the open joints in concrete
tempera-or on bridges—they are there to allow room ftempera-or the expansion of theconcrete as the seasons change Continued addition of heat energycan cause solids to change into liquids or liquids to change to gases.These are called phase changes
• Solids change to liquids by melting
• Liquids change to solids by freezing
• Liquids change to gases by evaporation
• Gases change to liquids by condensation
Trang 22Above is a generalized heat and temperature graph for materials.Note the increase in temperature in the substance until a phasechange begins to occur During a phase change all the heat energyadded to the material is converting the substance from one phase toanother The temperature remains constant The temperature doesnot begin to rise again until the phase change is complete Reversingthe process means removing heat Should we apply the graph towater, we can say that during the freezing/melting phase, both liquidwater and ice are present Likewise, during the condensation/evapo-ration phase, both liquid water and steam are present The graph isflat during these processes, showing that no temperature changeoccurs during a phase change.
The heat required to change a substance from a solid to a liquid
is called heat of fusion The heat required to change a substance from
a liquid to a gas is called heat of vaporization Typically the heat of
vaporization is greater than the heat of fusion for a given substance
Expansion and ContractionWhen the temperature of a substance is raised, the atoms and mol-ecules of the substance have more energy This causes the distancebetween the atoms and molecules to increase As a result, the materialexpands Lowering the temperature of a substance causes the dis-tance between atoms and molecules to decrease or shrink
Heat Heat TTTrrrrransfansfansfererHeat can be transferred between substances in several ways Everycase of heat transfer involves the movement of heat from an area ofhigh heat content to an area of low heat content