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By Ray Merry
Back to home: www.raymerry.com
Back to Physics: www.raymerry.com/classes/Physics |
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A traveling disturbance consisting of
coordinated vibrations that carry energy with no net movement of matter.
See pages 217,218,219 |
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Have you ever "done the wave" as part
of a large crowd at a football or baseball game? A group of people jump up
and sit back down, some nearby people see them and they jump up, some
people further away follow suit and pretty soon you have a wave traveling
around the stadium. The wave is the disturbance (people jumping up and
sitting back down), and it travels around the stadium. However, none of the
individual people the stadium are carried around with the wave as it
travels - they all remain at their seats. |
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The wave medium is the substance the wave is
traveling through. |
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E.G. Sound requires a media or material to
travel through. The media can be
water, air, wood, etc. |
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Light on the other hand travels through a
vacuum, and may not require a media. |
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A wave pulse is one up and down or back and
forth motion of a wave (short and fleeting). |
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A continuous wave has many pulses (steady and
repeating) . |
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Transverse wave
oscillations are
perpendicular (transverse) to the direction the wave travels. (p. 219 fig.
6.4 a.) |
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Longitudinal wave
oscillations are
along the direction the wave travels. (p. 219 fig. 6.4 b.) note corrections
in book p. 219 & 220 |
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Longitudinal, Sound in air |
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Transverse, fan wave, sea wave. |
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r = greek letter rho, stands for linear density
r= linear mass density of a rope, string,
etc. = m/l (mass/length) |
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v= (F/r)½
(Speed of a wave on a rope, etc. = sq. rt. of Force/linear density.) |
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V= 20.1x(T)1/2 (20.1 x sq.rt of Temp in Kelvins) |
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Speed of sound waves in air at temperature T (SI
units, T in Kelvins) |
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Amplitude: Maximum displacement of points on a
wave, measured from the equilibrium position. |
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Wavelength: (l) The distance between two successive "like"
points on a wave. |
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An example is the distance between two adjacent
peaks or two adjacent valleys. |
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See fig.6.5 p221 |
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The number of cycles of a wave passing a point
per unit time. |
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It equals the number of oscillations per second
of the wave. |
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If 15 waves pass a point in 1 second the
frequency f = 15 Hz. |
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Equation relating the velocity, v, frequency, f,
and wavelength, l, of a continuous wave. |
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V=fl |
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velocity of waves = frequency x
wavelength |
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See p 225 fig. 6.11 & fig 6.12 and p 226
fig. 6.14 |
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The wave energy spreads out in 3 dimensions,
like the surface of a sphere. |
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As a result the same energy is spread out over a
larger and larger surface and amplitude decreases. |
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A wave so far from it’s source that the wave
front appears to be a straight line. |
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Echoes. |
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Parabolic Antennas |
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The apparent change in frequency of a wave due
to motion of the source of the wave, the receiver, or both. |
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If the source is moving towards the observer,
the observer perceives sound waves reaching him or her at a more frequent
rate (high pitch) |
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If the source is moving away from the observer,
the observer perceives sound waves reaching him or her at a less frequent
rate (low pitch). |
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pitch of an ambulance or police siren, goes up
as it approaches and then goes down as it recedes from you |
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Same effect from a passing train whistle. |
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Used in astronomy to deduce the component of
velocity in the line-of-sight of an approaching or receding
planet/star/galaxy etc. |
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Doppler effect was used to determine speed of
galaxies. |
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They were all found to be moving away from the
center |
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The farther away they were the faster they
seemed to be going away! |
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The study of the structure and evolution of the
universe as a whole. |
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A mathematical expression showing that the
farther a galaxy is from us, the faster it is moving away. One implication
of this relation is that the universe is expanding. |
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Process of using the reflection of a wave to
locate objects. |
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We send out a wave, wait for its return. |
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Since we know the speed and the time, from d=v x
t we determine its distance away |
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Sound waves build up in front as plane, etc.
approaches the speed of sound. When
it passes the speed of sound they are left behind. |
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Similar to bow waves on a boat. |
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The bending of a wave as it passes around the
edge of a barrier. |
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Diffraction causes a wave passing through a gap
or a slit to spread out into the shadow regions. |
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See fig. 6.26 p. 232 |
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Sound waves traveling around corners |
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Water waves going through openings. |
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The consequence of two waves arriving at the
same place and combining. |
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See fig. 6.28 p. 233 |
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occurs wherever the two waves meet in phase
(peak matches peak); |
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the waves add together. |
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Destructive interference occurs wherever the two
waves meet out of phase (peak matches valley); the waves cancel each other. |
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Give an explanation of how the phase
relationship of superposed waves determines whether they interfere
constructively or destructively. |
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In phase is constructive, out of phase 180
degrees (half a cycle) is destructive. |
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A wave disturbance which our ears are sensitive
to. A longitudinal wave in air, if
it is audible it has a frequency between 20 and 20,000 hz. |
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Does sound occur if there is no one to hear it? |
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The back and forth vibrations of the surrounding
air molecules creates a pressure wave which travels outward from its
source. This pressure wave consists of compressions and rarefactions. The
compressions are regions of high pressure, where the air molecules are
compressed into a small region of space. The rarefactions are regions of
low pressure, where the air molecules are spread apart. This alternating
pattern of compressions and rarefactions is known as a sound wave. |
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The back and forth vibrations of the surrounding
air molecules creates a pressure wave which travels outward from its
source. This pressure wave consists of compressions and rarefactions. |
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The compressions are regions of high pressure,
where the air molecules are compressed into a small region of space. |
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The rarefactions are regions of low pressure,
where the air molecules are spread apart. |
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This alternating pattern of compressions and
rarefactions is known as a sound wave. |
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How high or low a sound is, related to the
frequency of the sound. |
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Higher pitches have higher frequency waves. |
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Very high frequency sound waves, higher than we
can hear. |
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Used in medicine in imaging and to destroy
kidney stones in the bladder |
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Sonar |
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Ultrasound Analysis |
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Bats Echolocation |
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Insect Repellant/Dog Whistle |
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8 notes in the scale, key is the starting
note Key of C has CDEFGAB |
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Notes repeat in octaves. |
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One octave is double the frequency of the one
below. |
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Waves close in frequency sometimes
constructively interfere, causing a sudden loudness. |
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E.G. sound of 500 hz and 502 hz, 2 hz is the
difference or beat frequency, 502 –500 = 2 |
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Two times per second they would interfere
constructively. |
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Recognize some differences in the ways various
musical instruments produce sound. |
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wind instruments: blow reed vibrates |
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percussion: stike and they vibrate |
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strings: pluck or bow and they vibrate |
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Harmonics are sounds emitted in simple ratios of
the main or fundamental frequency |
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First Harmonic or fundamental = f |
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Second H = 2f |
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Third H= 3f, etc. |
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http://id.mind.net/~zona/mstm/physics/waves/standingWaves/standingWaves1/StandingWaves1.html |
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If a sound of A has 220 Hz, what are the first
and third harmonics? |
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1st H = f = 1 x 220 = 220 Hz |
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2nd H = 2 x f, |
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third = 3 x f = 3 x 220 = 660Hz |
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A bel is a rating of the power of 10 of the
amplitude of a wave. E.g. 10, vs
100, = 1 bel more (101 vs. 102 ) which is 10 decibels |
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Related to intensity of the sound. Closest measurement is the decibel (.1
bel) |
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Minimum difference in intensity we can hear is 1
db, to sound louder |
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120 db
is the threshold of pain |
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2 identical sounds are 3 db higher than the
single sound. |
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It takes 10 identical sounds to sound twice as
loud, which is a change of 10 db. |
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This is cumulative, 100 db sounds 4x as loud as
80 db. |
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Back to home: www.raymerry.com |
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Back to Physics: www.raymerry.com/classes/physics |
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