Title: Exam 3: Friday December 3rd, 8:20pm to 10:20pm
1- Exam 3 Friday December 3rd, 820pm to 1020pm
- You must go to the following locations based on
the 1st letter of your last name - Review session Thursday Dec. 2 (Woodard), 615
to 810pm in NPB 1001 (HERE!)
- Final Exam (cumulative) Tuesday December 14th,
1230pm to 230pm. - Room assignments A to K in NPB1001 (in here)
L to Z in Norman Hall 137. - Two more review sessions Dec. 7 (Hill) and Dec.
9 (Woodard), 615 to 810pm in NPB1001 (HERE!)
2Class 40 - Waves I Chapter 16 - Wednesday
December 1st
- QUICK review
- Wave interference
- Standing waves and resonance
- Sample exam problems
- HiTT (if time permits, otherwise Friday)
Reading pages 413 to 437 (chapter 16) in
HRW Read and understand the sample
problems Assigned problems from chapter 16 (due
Dec. 2nd!) 6, 20, 22, 24, 30, 34, 42, 44, 66,
70, 78, 82
3Review - traveling waves on a string
Velocity
- The tension in the string is t.
- The mass of the element dm is mdl, where m is the
mass per unit length of the string.
Energy transfer rates
4The principle of superposition for waves
- It often happens that waves travel simultaneously
through the same region, e.g.
5The principle of superposition for waves
- If two waves travel simultaneously along the same
stretched string, the resultant displacement y'
of the string is simply given by the summation
where y1 and y2 would have been the displacements
had the waves traveled alone.
6Interference of waves
- Suppose two sinusoidal waves with the same
frequency and amplitude travel in the same
direction along a string, such that
7Interference of waves
8Interference of waves
9Interference of waves
If two sinusoidal waves of the same amplitude and
frequency travel in the same direction along a
stretched string, they interfere to produce a
resultant sinusoidal wave traveling in the same
direction.
Link
10Standing waves
If two sinusoidal waves of the same amplitude and
wavelength travel in opposite directions along a
stretched string, their interference with each
other produces a standing wave.
- This is clearly not a traveling wave, because it
does not have the form f(kx - wt). - In fact, it is a stationary wave, with a
sinusoidal varying amplitude 2ymcos(wt).
Link
11Reflections at a boundary
- Waves reflect from boundaries.
- This is the reason for echoes - you hear sound
reflecting back to you. - However, the nature of the reflection depends on
the boundary condition. - For the two examples on the left, the nature of
the reflection depends on whether the end of the
string is fixed or loose.
Movies
12Standing waves and resonance
- At ordinary frequencies, waves travel backwards
and forwards along the string.
- Each new reflected wave has a new phase.
- The interference is basically a mess, and no
significant oscillations build up.
13Standing waves and resonance
- However, at certain special frequencies, the
interference produces strong standing wave
patterns.
- Such a standing wave is said to be produced at
resonance. - These certain frequencies are called resonant
frequencies.
14Standing waves and resonance
- Standing waves occur whenever the phase of the
wave returning to the oscillating end of the
string is precisely in phase with the forced
oscillations.
l determined by geometry
15Standing waves and resonance
- Here is an example of a two-dimensional vibrating
diaphragm. - The dark powder shows the positions of the nodes
in the vibration.