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Welcome to Physics 7C!Welcome to Physics 7C!
Lecture 2 -- Winter Quarter -- 2005
Professor Robin Erbacher
343 Phy/Geo
AnnouncementsAnnouncements• Course policy and regrade forms on the web: http://physics7.ucdavis.edu
• Quiz today! ~20 minutes long.
• Reminder: Friday is “Academic Monday”. Monday DL’s: please attend DL this Friday. Friday DL’s are canceled. See calendar on website.
• Final on Saturday, March 19 1:30pm. Let me know this week if you cannot make this.
• Turn off cell phones and pagers during lecture.
Simple Harmonic OscillatorsSimple Harmonic Oscillators
2
€
T = 2πm
k€
T = 2πl
gPendulum:
Mass/Spring:
€
y(t) = Asin(2π
Tt +φ) + BA generalized solution
is of the form:
Simple 1D WavesSimple 1D WavesWhat is a wave?A wave is a type of internal motion of a medium, in which the displaced portion returns to equilibrium. This disturbance propagates in space as well.
Particles of the medium oscillate about their equilibrium positions in both a spatial and a temporal way.
What kind of waves are there?
Transverse Waves
Longitudinal Waves
Combo Waves
(circular)
WaterWaves
We will focus on these
Wave ParametersWave ParametersCertain independent parameters characterize all waves:1) Amplitude: Controlled by the magnitude of the forces that
started the wave2) Speed: Determined by the properties of the medium.3) Direction: Determined by the direction of the forces starting
the wave 1) Longitudinal: Oscillations in direction of wave velocity v 2) Transverse: Oscillations are perpendicular to v
4) Frequency f of oscillations: controlled by forces starting the wave
Need y(x,t) !
Wave: disturbancepropagates in x…
Snapshot v. MovieSnapshot v. MovieSome waves are simply a pulse, and some are repetitive. These are harmonic (or sinusoidal), generated by SHOs. Harmonic waves have a dependent variable, wavelength , the distance at which the oscillation repeats.
wavelength: vwave/f
2
y(x)
2
y(t)
Snapshot: Hold time constant, see where we are in space.
Movie: Go forward in time, see how spatial points move in SHM.
The Wave RepresentationThe Wave RepresentationDescribing the behavior of harmonic (sinusoidal) waves is extremely important in our physical world.
Because there is both a time-dependence and a translation of the wave in space, we need to represent the wave using both t and x.
€
What are all these parameters?x: location in the medium (spatial)t: time (temporal)T,f, period, freq., wavelengthA: amplitude phase
€
Δy(x,t) = Asin[Φ(x,t)]
Too complicated? Think of the sin argument as one big phase (or angle)
€
y(x,t) - y0 = A sin(2π
Tt ±
2π
λx +φ) + BThe most general
solution is of the form:
Note: I swapped x and t term. Block notes differ from DL expression. Both ok. Use DL version
Total Phase of the WaveTotal Phase of the Wave
€
y(x,t) - y0 = A sin(2π
Tt ±
2π
λx +φ) + B
€
€
Δy(x,t) = Asin[Φ(x,t)]
Total phase
If we hold x constant, the wave will repeat in T seconds.If we hold t constant, the wave will repeat in meters.
T and play similar roles in the wave function, determininghow often the wave will repeat in time and space.
Wave: a displacement in space and time. The angle, , found from (T, , x, t, ), determines the total displacement y(x,t).
Period, Frequency, Wavelength, Wave Speed
Period, Frequency, Wavelength, Wave Speed
€
T = 1f (sec)period:
€
f = vwaveλ (1/sec)frequency:
wavelength:
€
= vwavef = vwaveT (meters)
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
€
Φ = 2π
Tt ±
2π
λx +φ = wave phase
Ride the wave: constant
€
± x = λ
2πΦ m
λ
Tt -
λ
2πφ
€
∴ v = dx
dt= m
λ
T
If we choose + in the wave function, the velocity is negative.
What’s the wave velocity?
Particle VelocityParticle Velocity
€
vwave = dxdt = mλ T
So, the velocity of the wave, or propagating disturbance, can be found by riding along the wave at constant :
What is the velocity of a particle (or length of string) on the wave?
As always:
€
v = dy(x,t)
dt Why y?
Transverse Waves:Particle moves as SHO!
€
vparticle = A2π
Tcos(
2π
Tt ±
2π
λx +φ)
€
y(x,t) - y0 = Δy(x,t) = A sin(2π
Tt ±
2π
λx +φ) + B
Note: I swapped x and t term. Block notes differ from DL expression. Both ok. Use DL version
Longitudinal Waves
Sound WavesSound Waves
€
P(x,t) - Patm = ΔP(x,t) = A sin(2π
Tt ±
2π
λx) ⇒ AsinΦ(x,t)
The sound vibrations in 1-Dimension, such as long, narrow tubes, trombone, flute, trumpet, follows harmonic oscillations. But how does one describe the vibrations of the air?
It’s all about pressure (density) fluctuations!
Equilibrium = Atmospheric (or surrounding) pressure
Power and IntensityPower and IntensitySound is a pressure fluctuation in a medium. Sound energy is transported through the medium via these fluctuations.
Power: sound energy time
emitted by a source
Intensity: Psource
area(area of wavefront)
How About Light?How About Light?What kind of wave is a light wave? It’s a transverse excitation, perpendicular to the direction of wave propagation.
What’s the medium that’s displaced as the wave propagates?
Nothing!
Light propagates via oscillating electric and magnetic fields (more on this later in the course!)
The Enigmatic Ether!
Light: Visible, and Invisible Light: Visible, and InvisibleThe light we see is a small portion of the radiation that exists!
Visible Light:4.3-7.5 x 1014 Hz
Ultra Violet (UV)X-rays/ rays
Infra Red IRwave, AM/FM, TV
frequency
wavelength
Wave Interference Wave InterferenceWhat happens when there is more than one wave?When two or more waves meet, they interfere with each other.Combining waves by adding them is known as superposition.
Consider two waves on a string. What’s the maximum displacement of the string from equilibrium?
Δy(wave1+wave2) = A1+A2
In Phase: 1 - 2 = n2 (n=integer)
(constructive interference)
Out of Phase: 1 - 2 = [(2n-1)/2]2 (n=integer)
(destructive interference)
Superposition of Waves Superposition of Waves
Adding 1D Waves Together:
€
Δytotal(x,t) = Δy1(x,t) +Δy2(x,t) = A1 sinΦ1 + A1 sinΦ2
€
Δytotal(x,t) = A1 sin(2πt
T1
± 2πx
λ1
+ϕ1) + A2 sin(2πt
T2
± 2πx
λ 2
+ϕ 2)
Using the Full Expressions:
What determines the total excursion of the medium at arbitrary time and position?
Phase angles and amplitudes!