far-sighted correction section 26.1 near-sighted correction zero
TRANSCRIPT
Far-Sighted Correction
Section 26.1
no ssf
111
Near-Sighted Correction
isf
111
zero
Compound Microscope
Section 26.2
i Ntotal obj eyepiece
obj eyepiece
s sm m m , ƒ ƒ
Refracting Telescope
Section 26.3
Tm
obj
eyepiece
mƒ
ƒ
Shutter Speed and ƒ-NumberThere is a trade-off
between shutter speed and ƒ-number If you reduce shutter speed,
you need to compensate by increasing the ƒ-number
Same Exposure Value (Camera settings) can have different f-number and time
Halving f-number reduces EV by sqrt(2)
Section 26.4
time
fEV n
2
Relativity
Chapter 27
Historical Development1600s
Newton discovered his laws of mechanicsApplied to a wide variety of problems over the next two
decadesWorked well
Late 1800sMaxwell’s equations explained the physics of
electromagnetism and lightEarly 1900s
RelativityQuantum Mechanics
Types of RelativitySpecial relativity
Concerned with objects and observers moving at a constant velocity
Topic of this chapterGeneral relativity
Applies to situations when the object or the observer is accelerated
Has implications for understanding gravitation
Relativity
The term relativity arises when a situation is described from two different points of view
When the railroad car moves with a constant velocity, Ted and Alice see different motions of the ball
Section 27.1
Reference FramesA reference frame can be thought of as a set of
coordinate axesInertial reference frames move with a constant
velocityThe principle of Galilean relativity is the idea that
the laws of motion should be the same in all inertial framesFor example, adding or subtracting a constant velocity
does not change the acceleration of an object and if Newton’s Second Law is obeyed in one inertial frame, it is obeyed in all inertial frames
Section 27.1
Interpretation by Ted and AliceTed observes the ball’s motion purely along the vertical
directionAlice sees the ball undergo projectile motion with a
nonzero displacement in both the x- and y-directionsTed would think the ball’s horizontal velocity is zero, but
Alice would disagreeBoth agree that the ball’s acceleration is downward with a
magnitude gBoth agree the ball’s horizontal acceleration is zeroBoth agree that the only force acting on the ball is the
force of gravity and that Newton’s second law is obeyed
Section 27.1
Galilean Relativity and LightAccording to Maxwell’s equations, the speed of light
is a constantHe also showed the speed of light is independent of
the motion of both the source and the observerAssume Ted is moving with a constant velocity v
relative to Alice when he turns on a flashlight Newton’s mechanics predict that speed of the light
wave relative to Alice should be c + vAccording to Maxwell’s theory, Ted and Alice should
both observe the light wave to move with speed c
Galilean Relativity and Light, cont.Galilean Relativity and
electromagnetism predict different results for observers in different inertial frames
Experiments showed that Maxwell’s theory was correct
The speed of light in a vacuum is always cGalilean relativity for how
the speed of light depends on the motion of the source is wrong
Section 27.1
Special RelativityEinstein developed a theory to analyze the Ted and Alice
situation called special relativityHis work was not motivated by any particular experimentHe suspected the speed of light is the same in all reference
frames Maxwell was correct
He then worked out what that implies for all the other laws of physics
The basics of the theory were stated in two postulates about the laws of physicsFor fast-moving objects Newton’s theory breaks down and
Einstein’s theory gives a correct description of motion in this regime
Section 27.2
Postulates of Special RelativityAll the laws of physics are the same in all inertial
reference frames The speed of light in a vacuum is a constant,
independent of the motion of the light source and all observers
Section 27.2
Postulates – Details First postulate is traced to the ideas of Galileo and
Newton on relativityThe postulate goes further than Galileo because it
applies to all physical laws Not just mechanics
The second postulate is motivated by Maxwell’s theory of lightThis is not consistent with Newton’s mechanics
The postulates will lead to a new theory of mechanics that corrects and extends Newton’s Laws
Section 27.2
More About LightOur everyday experience with conventional waves
cannot be applied to lightLight does not depend on having a conventional
material medium in which to travelA light wave essentially carries its medium with it as
it propagatesIn the electric and magnetic fields
The lack of a conventional medium was surprising and hard to reconcile with conventional intuition
Section 27.2
Inertial Reference FramesInertial reference frames play an important role in
special relativityA definition of what it means to be inertial is neededThe modern definition of an inertial reference is one
in which Newton’s First Law holdsYou can test for an inertial frame by observing the
motion of a particle is zero If the particle moves with a constant velocity, the reference
frame is inertialNewton’s other laws should also apply in all inertial
frames
Section 27.2
Earth as a Reference FrameSince the Earth spins about its axis as it orbits the
Sun, all points on the Earth’s surface have a nonzero acceleration
Technically, a person standing on the surface of the Earth is not in an inertial reference frame
However, the Earth’s acceleration is small enough that it can generally be ignored
In most situations we can consider the Earth to be an inertial reference frame
Section 27.2
Light ClockThe two postulates lead to
a surprising result concerning the nature of time
A light clock keeps time by using a pulse of light that travels back and forth between two mirrors
The time for the clock to “tick” once is the time needed for one round trip: 2ℓ / c
Section 27.3
Moving Light Clock
The clock moves with a constant velocity v relative to the ground
From Ted’s reference frame, the light pulse travels up and down between the two mirrors
Section 27.3
Moving Light Clock, cont.The time for the clock to make one tick as measured
by Ted is
Alice sees the light pulse travel a longer distanceThe speed of light is the same for Alice as for TedBecause of the longer distance, according to Alice
the light will take longer to travel between the mirrors
ot c2
Section 27.3
Moving Clock, Alice’s TimeFor Alice, the time for one tick of the clock is
The time for Ted is different from the time for AliceThe operation of the clock depends on the motion of
the observer
ottv
c2
21
Section 27.3
Moving Clocks Run SlowAlice’s measures a longer time than TedPostulate 1 states that all the laws of physics must
be the same in all inertial reference framesTherefore the result must hold for any clock
Special relativity predicts that moving clocks run slow
This effect is called time dilationFor typical terrestrial speeds, the difference between Δt and Δto is negligible
Section 27.3
Time DilationWhen the speed is
small compared to c, the factor is very close to 1
Approximations given in Insight 27.1 may be used in many terrestrial cases
v c2 21
Section 27.3
Speeds Greater the cIf the value of the speed is greater than the speed of
light, Δt / Δto will be imaginary
Speeds greater than the speed of light have never been observed in nature
Experiments have shown that the time dilation predicted by special relativity is correct
The result applies to all clocks, even biological ones
Section 27.3
Proper TimeThe time interval Δto is measured by the observer at
rest relative to the clockThis quantity is called the proper timeThe time interval measured by a moving observer is
always longer than the proper timeThe proper time is always the shortest possible time
that can be measured for a process, by any observer
Section 27.3
Twin Paradox
An astronaut, Ted, visits a nearby star, Sirius, and returns to EarthSirius is 8.6 light-years from EarthTed is traveling at 0.90 c
Alice, Ted’s twin, stays on Earth and monitors Ted’s trip
Section 27.3
Twin Paradox, TimesAlice measures the trip as taking 19 years
Ted’s body measures the proper time of 8.3 years
Alice concludes that Ted will be younger than she isTed calculates the Earth (and Alice) move away from him
at 0.90 cTed concludes Alice will age 8.3 years while he ages 19
yearsTed concludes that Alice will be younger than he is
lyt years
c17.2
190.90
ot t v c years c c years22 2 21 19 1 0.90 / 8.3
Section 27.3
Twin Paradox, ResolutionTime dilation appears to lead to contradictory resultsAlice’s analysis is correct
She remains in an inertial frame and so can apply the results of special relativity
Ted is incorrectHe accelerates when he turns around at SiriusSpecial relativity cannot be applied during this time
spent in an accelerating frame
Section 27.3
Time Dilation and GPSEach GPS satellite
contains a very accurate clock
The satellite clocks are moving in orbit, so they experience time dilationThey run slow by about
7µs per dayTo accurately determine a
position, the effect of time dilation must be accounted for
Section 27.3
Simultaneity
Two events are simultaneous if they occur at the same timeTed is standing the middle of his railroad carHe moves at a speed v relative to AliceTwo lightning bolts strike the ends of the car and leave burn
marks on the ground which indicate the location of the two ends of the car where the bolts strike
Section 27.4
Simultaneity, cont.Did the two lightning bolts strike simultaneously?According to Alice
She is midway between the burn marksThe light pulses reach her at the same timeShe sees the bolts as simultaneous
According to TedThe light pulse from at B struck before the bolt at A
Since he is moving toward B
The two bolts are not simultaneous in Ted’s view
Section 27.4
Simultaneity, finalSimultaneity is relative and can be different in
different reference framesThis is different from Newton’s theory, in which time
is an absolute, objective quantityIt is the same for all observers
All observers agree on the order of the events
Section 27.4
Length Contraction
Alice marks two points on the ground and measures length Lo between them
Ted travels in the x-direction at constant velocity v and reads his clock as he passes point A and point BThis is the proper time interval of the motion
Section 27.5
Length Contraction, cont.Distance measured by Alice = Lo = v Δt
Distance measured by Ted = L = v Δto
Since Δt ≠ Δto, L ≠ Lo
The difference is due to time dilation and
The length measured by Ted is smaller than Alice’s length
oL L v c2 21 /
Proper LengthTed is at restAlice moves on the
meterstick with speed v relative to Ted
Ted measures a length shorter than Alice
Moving metersticks are shortened
The proper length, Lo, is the length measured by the observer at rest relative to the meterstick
Length Contraction EquationLength contraction is
described by
When the speed is very small, the contraction factor is very close to 1This is the case for
typical terrestrial speeds
o
L vL c
2
21
Section 27.5
Proper Length and Time, ReviewProper time is measured by an observer who is at
rest relative to the clock used for the measurementProper length is measured by an observer who is at
rest relative to the object whose length is being measured
Section 27.5
Experimental SupportA large number of experiments have shown that
time dilation and length contraction actually do occurAt ordinary terrestrial speeds the effects are
negligibly smallFor objects moving at speeds approaching the
speed of light, the effects become significant
Section 27.5