Chapter 7: Waves and Sound Flashcards

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1
Q

crest

A

distance from one maximun of the wave

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2
Q

wavelenght (λ)

A

diatance form one crest to the other

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2
Q

frequency (f)

A

number of wavelenghts passing a fixed point per second, measure in heartz (Hz)

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3
Q

propagation speed (v)

A

v = f λ

f = frequency
λ = wavelenght

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4
Q

angular frequency (w)

A

w = 2 π f = 2π / T

f = frequency
T = period

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4
Q

perios (T)

A

T = 1 / f

unit is second

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5
Q

amplitude (A)

A

maximun magnitude of displacement in a wave

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5
Q

phases in waves

A

if two waves are perfectly in phase, the resultant wave has an amplitude equal to the sum of the amplitude of the ywo waves. If two equal waves are exactly 180 degrees out of phase, then the resultant wave has zero amplitude.

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6
Q

traveling wave

A

wave is moving

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7
Q

standinf waves

A

the only movement is amplitudeat fixed points along the lenght of the string

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8
Q

speed of sound is

A

v = √B / ρ

B= bulk modulud, a measure of the medium resistance to compression (B increases from gas to solid)
ρ = density of the medium

the speed of sound is fastest in a solid with low density and slowest in a very dense gas.

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9
Q

the speed of sound in air at 20C is ____

A

343 m/s

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10
Q

normal range for a human hearing is

A

20 Hz to 20,000Hz

Infrasonic is below 20 Hz

Ultrasonic is above 20,000 Hz

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10
Q

doppler effect

A

f’ =f ( v ± vd ) / (v (reverse of (±)) vs)

vd = speed of the detector
vs = speed of the source

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11
Q

doppler effect explained

A

if the source and detector are moving towards each other the perceived frequency f’ is greater than the actual frequency f

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12
Q

intensity is inversely proportional to the square of the ____

A

distance from the source

I ∝ 1 / r^2

12
Q

sound that a human can hear that causes pain intensity:

A

10 W / m^2

13
Q

intensity

A

I = P / A

P = power
A = area

unit is W / m^2

14
Q

softest sound that a human can hear

A

1 x 10^ -12 W / m^2

15
Q

perforation fo the eardrum

A

1 x 10^4 W / m^2

16
Q

sound lebel

A

β = 10 log I / Io

β = sound level
I =intensity of the sound wave
Io= threshold of hearing (10^-12 W/m^2)

16
Q

strings

A

λ = 2L / n

L = lenght of the string
n = it is called the harmonic

16
Q

when intensity of sound is changed by some factor, we can calculate the new sound using:

A

βf = βi + 10 If / Ii

If / Ii ratio is the final intensity over the initial intensity

17
Q

first harmonic in string

A

λ = 2L

L = λ /2

18
Q

third harmonic in string

A

λ = 2L / 3

L = 3λ / 2

19
Q

second harmonic in string

A

λ = L

20
Q

rule for harmonic in string

A

the number of antinodes present will tell you which harmonic it is

21
Q

open pipes rule

A

the number os nodes present will tell you which harmonic it is

22
Q

second harmonic in open pipes

A

L = λ

23
Q

first harmonic in open pipes

A

L = λ / 2

24
Q

third harmonic in open pipes

A

L = 3λ / 2

24
Q

closed pipes rule

A

count the number of quarter-wavelenght contained in the pipe to determine the harmonic. there are only odd harmonics

λ = 4L / n

f = n v / 4 L

25
Q

third harmonic in closed pipes

A

L = 3λ / 4

25
Q

first harmonic in closed pipes

A

L = λ / 4

26
Q

fifth harmonic in closed pipes

A

L = 5λ / 4