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PS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November 18 th , 2015

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Page 1: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

PS 250: Lecture 29 Wave Energy, Momentum,

and Relativity Intro.J. B. Snively

November 18th, 2015

Page 2: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Today’s Class

Wave Energy and MomentumSpecial RelativitySummary

Page 3: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Describes magnitude and direction of energy flow rate in W/m2 = J/(s*m2)

Allows calculation of power exiting through any closed surface:

Wave Energy Flow Poynting Vector

P =

I�S · d �A

�S =1

µo

�E ⇥ �B

Page 4: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Wave Energy Flow Average Quantities and Intensity

I = Sav

=E

max

Bmax

2µo

=E

max

2µo

Emax

c=

E2

max

2µo

c

Average value of S over a sinusoidal wave cycle (Sav = Wave Intensity I)

=1

2�o

cE2

max

Which can also be written as:

NOTE: Poynting Vector is Instantaneous Vector Quantity Intensity if Averaged Scalar Quantity

Page 5: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Wave Energy Flow Average Quantities and Intensity

So, since: P =

I�S · d �A

P = SavA

Intensity = Sav =P

A

Applicable for simple sinusoidal wave sources that radiate equally in all directions – i.e., in Example Problems.

Page 6: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Wave Momentum “Radiation Pressure”

Electromagnetic waves apply a “radiation pressure” (Force per Area)

when they impact a surface:

prad =Sav

c=

I

c

prad =2Sav

c=

2I

c

Pressure on absorbing surface.

Pressure on reflecting surface.

Page 7: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Today’s Class

Wave Energy and MomentumSpecial RelativitySummary

Page 8: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Principle of relativity:

The laws of physics are the same in every inertial (non-accelerating) reference frame.

Speed of Light is a Constant:

The speed of light in vacuum is the same in all inertial frames of reference and is independent of the motion of the source.

Einstein’s Postulates Foundation of Special Relativity

Page 9: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

There is no specific medium that light propagates through – no “ether” – and (in vacuum) it has the same speed in any direction relative to any observer.

Laws of electro-magnetics apply in any inertial reference frame. (You can move a magnet inside a solenoid to produce an EMF, or a solenoid around a magnet!)

It is not possible for an observer to travel at the speed of light.

What this implies...

Page 10: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Two Big Conclusions:

Moving clocks run slow.(Time Dilation)

Moving objects are shortened.(Length Contraction)

Page 11: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Newton vs. Einstein

Page 12: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Newton vs. Einstein

Page 13: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Relativity of Simultaneity“Two events that are simultaneous in one inertial

system are not, in general, simultaneous in another”

Page 14: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November
Page 15: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Relativity of SimultaneityIn Mavis’ reference frame, the strikes

could not have been simultaneous: She is sitting in the middle of the train, and the

speed of light is constant!

Page 16: Wave Energy, Momentum, and Relativity Intro.pages.erau.edu/~snivelyj/ps250/PS250-Lecture29.pdfPS 250: Lecture 29 Wave Energy, Momentum, and Relativity Intro. J. B. Snively November

Summary / Next Class:

Mastering Physics for Today

Homework for Friday