Wednesday, October 29, 2014

Optics HW -1





3.  Review the concept of refraction:  what it is, what causes it, what happens during it, under what circumstances does light bend, etc.  Review also reflection and basics of mirrors.

4.  Show how to calculate the wavelength of WTMD's signal (89.7 MHz).

5.  Review the concept of total internal reflection (and its relation to fiber optics).

Monday, October 27, 2014

Light - 2. Reflection and Refraction.



Reflection - light "bouncing" off a reflective surface. This obeys a simple law, the law of reflection!

The incident (incoming) angle equals the reflected angle. Angles are generally measured with respect to a "normal" line (line perpendicular to the surface).

Note that this works for curved mirrors as well, though we must think of a the surface as a series of flat surfaces - in this way, we can see that the light can reflect in a different direction, depending on where it hits the surface of the curved mirror. More to come here.



Refraction:



Refraction is much different. In refraction, light enters a NEW medium. In the new medium, the speed changes. We define the extent to which this new medium changes the speed by a simple ratio, the index of refraction:
n = c/v
In this equation, n is the index of refraction (a number always 1 or greater), c is the speed of light (in a vacuum) and v is the speed of light in the new medium.
The index of refraction for some familiar substances:
vacuum, defined as 1
air, approximately 1
water, 1.33
glass, 1.5
polycarbonate ("high index" lenses), 1.67
diamond, 2.2
The index of refraction is a way of expressing how optically dense a medium is. The actual index of refraction (other than in a vacuum) depends on the incoming wavelength. Different wavelengths have slightly different speeds in (non-vacuum) mediums. For example, red slows down by a certain amount, but violet slows down by a slightly lower amount - meaning that red light goes through a material (glass, for example) a bit faster than violet light. Red light exits first.
In addition, different wavelengths of light are "bent" by slightly different amounts. This is trickier to see. We will explore it soon.


Refraction, in gross gory detail



Consider a wave hitting a new medium - one in which is travels more slowly. This would be like light going from air into water. The light has a certain frequency (which is unchangeable, since its set by whatever atomic process causes it to be emitted). The wavelength has a certain amount set by the equation, c = f l, where l is the wavelength (Greek symbol, lambda).
When the wave enters the new medium it is slowed - the speed becomes lower, but the frequency is fixed. Therefore, the wavelength becomes smaller (in a more dense medium).
Note also that the wave becomes "bent." Look at the image above: in order for the wave front to stay together, part of the wave front is slowed before the remaining part of it hits the surface. This necessarily results in a bend.
The general rule - if a wave is going from a lower density medium to one of higher density, the wave is refracted TOWARD the normal (perpendicular to surface) line. See picture above.


http://stwww.weizmann.ac.il/lasers/laserweb/java/twoangles2.htm

http://lectureonline.cl.msu.edu/~mmp/kap25/Snell/app.htm

http://www.physics.uoguelph.ca/applets/Intro_physics/refraction/LightRefract.html

Light - 1

Recall that waves can be categorized into two major divisions:

Mechanical waves, which require a medium. These include sound, water and waves on a (guitar, etc.) string

Electromagnetic waves, which travel best where there is NO medium (vacuum), though they can typically travel through a medium as well. All electromagnetic waves can be represented on a chart, usually going from low frequency (radio waves) to high frequency (gamma rays). This translates to: long wavelength to short wavelength.

All of these EM waves travel at the same speed in a vacuum: the speed of light (c). Thus, the standard wave velocity equation becomes:


c = f l



where c is the speed of light (3 x 10^8 m/s), f is frequency (in Hz) and l (which should actually be the Greek letter, lambda) is wavelength (in m).

General breakdown of e/m waves from low frequency (and long wavelength) to high frequency (and short wavelength):

Radio
Microwave
IR (infrared)
Visible (ROYGBV)
UV (ultraviolet)
X-rays
Gamma rays

In detail, particularly the last image:



http://www.unihedron.com/projects/spectrum/downloads/full_spectrum.jpg

Don't forget - electromagnetic waves should be distinguished from mechanical waves (sound, water, earthquakes, strings on a guitar/piano/etc.). 

ALL E/M waves (in a vacuum) travel at the SPEED OF LIGHT (c).




Wednesday, October 22, 2014

Practice questions in music

Consider the musical note G, 392 Hz.  Find the following:

1.  The frequencies of the next two G's, one and two octaves above.

2.  The frequency of the G one octave lower than 392 Hz.

3.  The frequency of G#, one semi-tone (piano key or guitar fret) above this G.

4.  The frequency of A#, 3 semi-tones above G.

5.  The wavelength of the 392 Hz sound wave, assuming that the speed of sound is 340 m/s.

6.  Review the notes on the Doppler effect - be able to explain it, and know how it applies to sound and light waves.

7.  What are the differences between longitudinal and transverse waves?  Gives examples of each.  What type of wave is sound?


Also for your consideration.  Understand the following concepts:

a.  harmonics on a string

b.  how waves form in a tube - what actually happens with the air inside?

c.  Here's a thought question for you - why does breathing in helium make your voice higher?

answers:

1.  392 x 2; 392 x 4

2.  392/2

3.  392 x 1.0594

4.  392 x 1.0594 x 1.0594 x 1.0594  (or 392 x 1.0594^3)

5.  340/392

6-7.  See notes.

Doppler Effect!


http://www.lon-capa.org/~mmp/applist/doppler/d.htm

http://falstad.com/mathphysics.html
Run the Ripple tank applet -
http://falstad.com/ripple/

The key in the Doppler effect is that motion makes the "detected" or "perceived" frequencies higher or lower.

If the source is moving toward you, you detect/measure a higher frequency - this is called a BLUE SHIFT.

If the source is moving away from you, you detect/measure a lower frequency - this is called a RED SHIFT. Distant galaxies in the universe are moving away from us, as determined by their red shifts. This indicates that the universe is indeed expanding (first shown by E. Hubble). The 2011 Nobel Prize in Physics went to local physicist Adam Riess (and 2 others) for the discovery of the accelerating expansion of the universe. Awesome stuff!

http://www.nobelprize.org/nobel_prizes/physics/laureates/2011/

It's worth noting that the effect also works in reverse. If you (the detector) move toward a sound-emitter, you'll detect a higher frequency. If you move away from a detector move away from a sound-emitter, you'll detect a lower frequency.

Mind you, these Doppler effects only happen WHILE there is relative motion between source and detector (you).

And they also work for light. In fact, the terms red shift and blue shift refer mainly to light (or other electromagnetic) phenomena.

Monday, October 20, 2014

Waves in Pipes









This is far from obvious but - the mathematics of sound waves (harmonics) in organ pipes and waves (harmonics) on a string are mathematically identical.  But here are some distinctions:

Waves on a string are TRANSVERSE - this means that the wave vibrates in a direction perpendicular to the direction of wave travel.  These are traditional looking waves.

Sound waves are LONGITUDINAL (also known as COMPRESSIONAL) - this means that the wave vibrates in a direction parallel to the direction of wave travel.  See the second set of illustrations above.

When you speak, you are oscillating the air around your mouth.  It vibrates BACK AND FORTH (not up and down).  Each air molecule vibrates the air molecules next to it and the impulse/wave travels at the speed of sound - which in room temperature dry air is around 345 m/s.

Now tubes that are open on both ends are forced to produce waves that have anti-nodes on both ends - meaning that there is nothing for the sound to bounce off of.  This is similar to strings which have nodes on both ends - something to bounce off of both ends.  In both cases, the wavelength is the same for the resonant frequency:

wavelength (for n=1) = 2L

And the sequence of harmonics is exactly the same as for strings.

Waves in tubes LOOK different than waves on strings, but they act very similarly and the mathematics are the same.

(If the tube is closed on one end, you are forced to have an anti-node on one end only.  This is trickier.  See the top 2 images of figure 1 above.)

Another image that depicts the sound in organ pipes.  Below are 6 pairs of images.  The first 3 pairs depict the waves formed in organ pipes open at both ends.  Pairs 4-6 depict the waves formed in organ pipes capped on one end.  There is a major difference with tubes capped at one end - since you are forced to have a node at one end and an antinode at the other, you only get ODD harmonics.  The wavelength is also doubled (compared to the same harmonics in tubes open at both ends).  Since the wavelengths are twice as long, the frequencies are half as much.  This means that a resonant frequency (n=1) for a tube open only on one end is half as much (one octave lower) than the same length tube open on both ends.

In other words, if you cap a tube on one end, the tone produced is one octave lower.

FYI

https://www.youtube.com/watch?v=23fTMkcDOhE&feature=youtu.be

If you missed the class on Chladni plates and resonating wire loops, etc.  Thanks to Alex M for filming this.

Also:

https://www.youtube.com/watch?v=kBmRNkM9saA


Wednesday, October 15, 2014

Music

In western music, we use an "equal tempered (or well tempered) scale."  It has a few noteworthy characteristics;

The octave is defined as a doubling (or halving) of a frequency.

You may have seen a keyboard before.  The notes are, beginning with C (the note immediately before the pair of black keys):

C
C#
D
D#
E
F
F#
G
G#
A
A#
B
C

(Yes, I could also say D-flat instead of C#, but I don't have a flat symbol on the keyboard.  And I don't want to split hairs over sharps and flats - it's not that important at the moment.)

There are 13 notes here, but only 12 "jumps" to go from C to the next C above it (one octave higher).  Here's the problem.  If there are 12 jumps to get to a factor of 2 (in frequency), making an octave, how do you get from one note to the next note on the piano?  (This is called a "half-step" or "semi-tone".)

The well-tempered scale says that each note has a frequency equal to a particular number multiplied by the frequency that comes before it.  In other words, to go from C to C#, multiply the frequency of the C by a particular number.

So, what is this number?  Well, it's the number that, when multiplied by itself 12 times, will give 2.  In other words, it's the 12th root of 2 - or 2 to the 1/12 power.  That is around 1.0594.

So to go from one note to the next note on the piano or fretboard, multiply the first note by 1.0594.  To go TWO semi-tones up, multiply by 1.0594 again - or multiply the first note by 1.0594^2.  Got it?





Monday, October 13, 2014

Wave problems 1

1.  Differentiate between mechanical and electromagnetic waves.  Give examples.

2.  Draw a wave and identify the primary parts (wavelength, crest, trough, amplitude).

3.  Find the speed of a 500 Hz wave with a wavelength of 0.4 m.

4.  What is the frequency of a wave that travels at 24 m/s, if 3 full waves fit in a 12-m space?  (Hint:  find the wavelength first.)

5.  Approximately how much greater is the speed of light than the speed of sound?

6.  Harmonics

a.  Draw the first 3 harmonics for a wave on a string.
b.  If the length of the string is 1-m, find the wavelengths of these harmonics.
c.  If the frequency of the first harmonic (n = 1) is 10 Hz, find the frequencies of the next 2 harmonics.
d.  Find the speeds of the 3 harmonics.  Notice a trend?

7.  Show how to compute the wavelength of WTMD's signal (89.7 MHz).  Note that MHz means 'million Hz."

8.  A C-note vibrates at 262 Hz (approximately).  Find the frequencies of the next 2 C's (1 and 2 octaves above this one).

>

(answers)

1, 2.  See notes.

3.  200 m/s

4.  wavelength is 4 m.  Frequency is 6 Hz.

5.  3,000,000 / 340 --- that's around a million to one ratio

6.
a.  see notes
b.  wavelengths are:  2 m, 1 m, and 2/3 m
c.  frequencies are 10, 20 and 30 Hz, respectively, for n = 1, 2 and 3
d.  speeds are all constant:  20 m/s

7.  speed of light divided by 89.7 MHz.  That is 300,000,000 / 89,700,000, which works out to around 3.3 m.


8.  524 Hz and 1048 Hz

Wednesday, October 8, 2014

Energy

I stole my energy story from the famous American physicist Richard Feynman. Here is a version adapted from his original energy story. He used the character, "Dennis the Menace." The story below is paraphrased from the original Feynman lecture on physics (in the early 1960s).

Dennis the Menace
Adapted from Richard Feynman
Imagine Dennis has 28 blocks, which are all the same. They are absolutely indestructible and cannot be divided into pieces.
His mother puts him and his 28 blocks into a room at the beginning of the day. At the end of each day, being curious, she counts them and discovers a phenomenal law. No matter what he does with the blocks, there are always 28 remaining.
This continues for some time until one day she only counts 27, but with a little searching she discovers one under a rug. She realises she must be careful to look everywhere.
One day later she can only find 26. She looks everywhere in the room, but cannot find them. Then she realises the window is open and two blocks are found outside in the garden.
Another day, she discovers 30 blocks. This causes considerable dismay until she realises that Bruce has visited that day, and left a few of his own blocks behind.
Dennis' mother removes the extra blocks, gives the remaining ones back to Bruce, and all returns to normal.
We can think about energy in this way (except there are no blocks!). We can use this idea to track energy transfers during changes. We need to be careful to look everywhere to ensure that we can account for all of the energy.

Some ideas about energy
  • Energy is stored in fuels (chemicals).
  • Energy can be stored by lifting objects (potential energy).
  • Moving objects carry energy (kinetic energy).
  • Electric current carries energy.
  • Light (and other forms of radiation) carries energy.
  • Heat carries energy.
  • Sound carries energy.

But is energy a real thing?  No, not exactly.  It is a mathematical concept, completely consistent with Newton's laws and the equations of motion.  It allows us to see that some number (calculated according to other manifest changes - speed, mass, temperature, position, etc.) remains constant before and after some "event" occurs.

Waves!


So - Waves.....  

We spoke about energy.  Energy can, as it turns out, travel in waves.  In fact, you can think of a wave as a traveling disturbance, capable of carrying energy.

There are several wave characteristics (applicable to most conventional waves) that are useful to know:

amplitude - the "height" of the wave, from equilibrium (or direction axis of travel) to maximum position above or below

crest - peak (or highest point) of a wave

trough - valley (or lowest point) of a wave

wavelength (lambda - see picture 2 above) - the length of a complete wave, measured from crest to crest or trough to trough (or distance between any two points that are in phase - see picture 2 above).  Measured in meters (or any units of length).

frequency (f) - literally, the number of complete waves per second.  The unit is the cycle per second, usually called:  hertz (Hz)

wave speed (v) -  the rate at which the wave travels.  Same as regular speed/velocity, and measured in units of m/s (or any unit of velocity).  It can be calculated using a simple expression:





There are 2 primary categories of waves:

Mechanical – these require a medium (e.g., sound, guitar strings, water, etc.)

Electromagnetic – these do NOT require a medium and, in fact, travel fastest where is there is nothing in the way (a vacuum). All e/m waves travel at the same speed in a vacuum (c, the speed of light):

c = 3 x 10^8 m/s

First, the electromagnetic (e/m) waves:

General breakdown of e/m waves from low frequency (and long wavelength) to high frequency (and short wavelength):

Radio
Microwave
IR (infrared)
Visible (ROYGBV)
UV (ultraviolet)
X-rays
Gamma rays

In detail, particularly the last image:



http://www.unihedron.com/projects/spectrum/downloads/full_spectrum.jpg

Mechanical waves include:  sound, water, earthquakes, strings (guitar, piano, etc.)....

Again, don't forget that the primary wave variables are related by the expression:

v = f l


speed = frequency x wavelength

(Note that 'l' should be the Greek symbol 'lambda', if it does not already show up as such.)

For e/m waves, the speed is the speed of light, so the expression becomes:

c = f l


Note that for a given medium (constant speed), as the frequency increases, the wavelength decreases.

Next up - Sound!

Wednesday, October 1, 2014

Test 1 review questions and topics

Gravitation and flight questions and problems:

1.  Explain the meaning of "inverse square law".

2.  Discuss each of Kepler's 3 laws.

3.  At what point in its orbit is the Earth closest to the Sun?

4.  At what point in its orbit is the Earth moving fastest?

5.  What causes seasons?

6.  What is a semi-major axis of orbit (a)?

7.  What is an Astronomical Unit (AU)?

8.  Consider Jupiter.  It's orbit is 5 AU in size (roughly).  How long should it take Jupiter to orbit the Sun once?  Show how this calculation would be done.

9.  What is the period of Earth's orbit around the Sun?

10.  What is the size of Earth's orbit (in AU)?

11.  When you stand on the Earth's surface, you experience your "normal" Earth weight.  What would happen to your Earth weight if you were one Earth radius above the surface?  (That's twice as far from the center as simply standing on the surface.)

12.  What does gravitational force between 2 objects depend on?

13.  Explain the Bernoulli principle, particularly as it is applied to flying things.  What does the shape of an airfoil help accomplish?

(Answers below.)



General topics for exam 1.  Be sure to review all assigned homework, blog posts and your notes.

You are permitted to have a sheet of notes for this test.  I will NOT give equations.

pseudoscience
SI units (m, kg, s) - meanings, definitions
velocity
acceleration
related problems using the formulas
speed of light (c)
gravitational acceleration (g)
average vs. instantaneous velocity
freefall problems; using the equations of motion
Newton's 3 laws - applications and problems
Kepler's 3 laws - applications and problems
Newton's law of universal gravitation (inverse square law)
weight
the basics of flight

Relevant equations.  Expect a few numerical problems - calculator should not be required.

v = d/t

a = (vf - vi)/t

or:  vf = vi + at

d = vi t  +  0.5 a t^2


F = m a

W = m g

a^3 = T^2

>


1.  Explain the meaning of "inverse square law".

The force (of gravity, in this case) gets progressively weaker by the factor 1 over the distance squared.  Double the distance --> force is 1/4 as great as it was.  Triple the distance --> force is 1/9 the original.

2.  Discuss each of Kepler's 3 laws.

See notes.

3.  At what point in its orbit is the Earth closest to the Sun?

Perihelion, which is approximately January 3 each year.

4.  At what point in its orbit is the Earth moving fastest?

Same point as 3 above.

5.  What causes seasons?

Tilt of Earth's axis.

6.  What is a semi-major axis of orbit (a)?

Half the longest distance across the orbital path (ellipse).

7.  What is an Astronomical Unit (AU)?

Defined as the semi-major axis of Earth's orbit - roughly 93,000,000 miles - or  half the longest width across Earth's orbit.

8.  Consider Jupiter.  It's orbit is 5 AU in size (roughly).  How long should it take Jupiter to orbit the Sun once?  Show how this calculation would be done.

5^3 = T^2

So, T = the square root of 125.

9.  What is the period of Earth's orbit around the Sun?

1 year, or approximately 365.25 days.

10.  What is the size of Earth's orbit (in AU)?

Defined as 1 AU.

11.  When you stand on the Earth's surface, you experience your "normal" Earth weight.  What would happen to your Earth weight if you were one Earth radius above the surface?  (That's twice as far from the center as simply standing on the surface.)

1/4 your surface weight.

12.  What does gravitational force between 2 objects depend on?

mass of the objects; distance between; a universal (unchanging) constant (G)


>

Earlier questions to review:


1. What are epicycles and why were they important?  What is retrograde motion and what is *actually* going on when Mars seems to move backward?

2.  What contributions did Galileo make with his telescope? What got him into trouble?

3.  What is Copernicus' main contribution to science?

4. Know and understand the demonstrations with the "ball dropping and launching" cart.

5.  Consider a ball falling for 3 seconds.  Find the speed after 3 seconds of fall, and the distance this ball would fall (without air resistance).

6.  A car starts from rest and accelerates for 5 seconds at 2 m/s/s.  Find the speed after 5 seconds and the distance the car will travel in this time.  (Note the similarity with the previous problem.  Only the acceleration is different.)


>

1. Know and understand Newton's laws of motion.

2.  A 10-kg object is pushed on by a 200-N force.  What will be the acceleration?

3.  What is the weight of a 100-kg man?

4.  Would the answer to 3 be different if he was on the moon?  How so?

5.  Consider yourself standing on a scale in an elevator.  The scale reads your weight.  Compared to being at rest, how would the scale reading change (if at all) if the elevator were:

A.  Moving with constant velocity upward
B.  moving with constant velocity downward
C.  Moving with constant acceleration upward
D.  Moving with constant acceleration downward
E.  If the cable snapped (yikes!) and the elevator were falling


Things that fly!




The amazing science of flight is largely governed by Newton's laws.

Consider a wing cross-section:




Air hits it at a certain speed.  However, the shape of the wing forces air to rush over it and under it at different rates.  The top curve creates a partial vacuum - a region "missing" a bit of air.  So, the pressure (force/area) on top of the wing can become less than the pressure below.  If the numbers are right, and the resulting force below the wing is greater than the weight of the plane, the plane can lift.

This is often expressed as the Bernoulli Principle:

Pressure in a moving stream of fluid (such as air) is less than the pressure of the surrounding fluid.





The image above shows another way to think of flight - imagine the wing first shown, but slightly inclined upward (to exacerbate the effect).  There is a downward deflection of air.  The reaction force from the air below provides lift and the lift is proportional to the force on the wing.

In practice, it works out (in general) to be:

Lift = 0.3 p v^2 A

where p is the density of air, v (squared) is the speed of the plane, and A is the effective area.  Note that the lift is proportional to the speed squared - so, the faster the plane goes, the (much) easier it is to take flight.