Physics 213 General Physics Lectures 20 & 21. 1 Last Meeting: Optical Instruments Today: Optics Practice Problems, Relativity (over two lectures)

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Presentation transcript:

Physics 213 General Physics Lectures 20 & 21

1 Last Meeting: Optical Instruments Today: Optics Practice Problems, Relativity (over two lectures)

A concave mirror has radius R. When an object is located a distance 2R from the lens, which describes the image formed? 2 1. real, inverted, diminished 2. real, inverted, enlarged 3. virtual, upright, diminished 4. real, inverted, of equal size

A convex thin lens has a focal length of magnitude F. At which of the following distances from this lens would a real object give an inverted virtual image? 3 1. ½ F 2. 2F 3. Any value greater than 2F. 4. This cannot be done with a convex lens.

A given individual is unable to see objects clearly when they are beyond 100 cm. What focal length lens should be used to correct this problem? 4 1.  100 cm 2.  33.3 cm 3.  20 cm cm

A light source simultaneously emits light of two wavelengths, 480 nm and 560 nm, respectively. The source is used in a double ‑ slit interference experiment where the slit spacing is a mm, and the distance between double slits and the screen is 1.2 m. What is the separation between the second ‑ order bright fringes of the two wavelengths as they appear on the screen? (1 nm = 10  9 m) cm cm cm cm

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Simultaneity In Special Relativity, Einstein abandoned the assumption of simultaneity Thought experiment to show this  A boxcar moves with uniform velocity  Two lightning bolts strike the ends  The lightning bolts leave marks (A’ and B’) on the car and (A and B) on the ground  Two observers are present: O’ in the boxcar and O on the ground

Simultaneity – Thought Experiment Set-up Observer O is midway between the points of lightning strikes on the ground, A and B Observer O’ is midway between the points of lightning strikes on the boxcar, A’ and B’

Simultaneity – Thought Experiment Results The light signals reach observer O at the same time  She concludes the light has traveled at the same speed over equal distances  Observer O concludes the lightning bolts occurred simultaneously

Simultaneity – Thought Experiment Results, cont By the time the light has reached observer O, observer O’ has moved The light from B’ has already moved by the observer, but the light from A’ has not yet reached him  The two observers must find that light travels at the same speed  Observer O’ concludes the lightning struck the front of the boxcar before it struck the back (they were not simultaneous events)

Simultaneity – Thought Experiment, Summary Two events that are simultaneous in one reference frame are in general not simultaneous in a second reference frame moving relative to the first That is, simultaneity is not an absolute concept, but rather one that depends on the state of motion of the observer  In the thought experiment, both observers are correct, because there is no preferred inertial reference frame

Time Dilation The vehicle is moving to the right with speed v A mirror is fixed to the ceiling of the vehicle An observer, O’, at rest in this system holds a laser a distance d below the mirror The laser emits a pulse of light directed at the mirror (event 1) and the pulse arrives back after being reflected (event 2) Clock measures two events at the SAME LOCATION.

Time Dilation, Moving Observer Observer O’ carries a clock She uses it to measure the time between the events (Δt p ) The p stands for proper  She observes the events to occur at the same place  Δt p = distance/speed = (2d)/c

Time Dilation, Stationary Observer Observer O is a stationary observer on the earth He observes the mirror and O’ to move with speed v By the time the light from the laser reaches the mirror, the mirror has moved to the right The light must travel farther with respect to O than with respect to O’

Time Dilation, Observations Both observers must measure the speed of the light to be c The light travels farther for O The time interval, Δt, for O is longer than the time interval for O’, Δt p

Time Dilation, Time Comparisons Observer O measures a longer time interval than observer O’

Time Dilation, Summary The time interval Δt between two events measured by an observer moving with respect to a clock is longer than the time interval Δt p between the same two events measured by an observer at rest with respect to the clock A clock moving past an observer at speed v runs more slowly than an identical clock at rest with respect to the observer by a factor of  -1

Identifying Proper Time The time interval Δt p is called the proper time  The proper time is the time interval between events as measured by an observer who sees the events occur at the same position You must be able to correctly identify the observer who measures the proper time interval

Time Dilation – Generalization All physical processes slow down relative to a clock when those processes occur in a frame moving with respect to the clock  These processes can be chemical and biological as well as physical Time dilation is a very real phenomena that has been verified by various experiments

Length Contraction The measured distance between two points depends on the frame of reference of the observer The proper length, L p, of an object is the length of the object measured by someone at rest relative to the object The length of an object measured in a reference frame that is moving with respect to the object is always less than the proper length  This effect is known as length contraction

Length Contraction The proper length, L p, of an object is the length of the object measured by someone at rest relative to the object The length of an object measured in a reference frame that is moving with respect to the object is always less than the proper length  This effect is known as length contraction Length contraction takes place only along the direction of motion

Length Contraction, Derived A B A B According to outside observer at rest with A and B According to observer inside spaceship Observer at rest with A and B. Observer in spaceship. Time dilation gives Length Contraction

Relativistic Momentum To account for conservation of momentum in all inertial frames, the definition must be modified   v is the speed of the particle, m is its mass as measured by an observer at rest with respect to the mass  When v << c, the denominator approaches 1 and so p approaches mv

Relativistic Energy The definition of kinetic energy requires modification in relativistic mechanics KE =  mc 2 – mc 2  The term mc 2 is called the rest energy of the object and is independent of its speed  The term  mc 2 is the total energy, E, of the object and depends on its speed and its rest energy