Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
10 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
11 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
12 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
13 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
14 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
15 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
16 Simple Harmonic Motion
Period- the time it takes for one complete
cycle
Frequency- The number of cycles completed per second
Frequency-measured in Hertz- cycles per sec.
Frequency Units- 1/s or s-1
f1/T
T1/f
17 Simple Harmonic Motion ms 18 Simple Harmonic Motion ms 19 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms 20 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms 21 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms 22 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms 23 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 24 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 3 cycles / 25 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 3 cycles / 9.6 ms 3 cycles /(.0096s) 26 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 3 cycles / 9.6 ms 3 cycles /(.0096s) 312.5 Hz 27 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 3 cycles / 9.6 ms 3 cycles /(.0096s) 312.5 Hz Period 1 / f 28 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 3 cycles / 9.6 ms 3 cycles /(.0096s) 312.5 Hz Period 1 / f 1 / 312.5 s .0032 s or 3.2 ms on average 29 Simple Harmonic Motion 0 ms 3.1 ms 6.3ms 9.6ms ms Frequency cycles per second 3 cycles / 9.6 ms 3 cycles /(.0096s) 312.5 Hz Period 1 / f 1 / 312.5 s .0032 s or 3.2 ms on average 30 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
31 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
32 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
33 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
34 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
35 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
36 Period of oscillation of a Spring Mass SystemPeriod of oscillation of Pendulum Mass System
Spring
T2p m
k
Dependent on mass and inversely related to the spring constant
Pendulum
T2p l
g
Dependent on length and inversely related to the acceleration due to gravity
37 Natural Frequency Forced Vibration-Resonance
The frequency that a system occurs when a force is applied to it.
A Driving Force is a force that is applied over and over again.
38 Natural Frequency Forced Vibration-Resonance
The frequency that a system acquires when a force is applied to it.
A Driving Force is a force that is applied over and over again.
39 Natural Frequency Forced Vibration-Resonance
The frequency that a system acquires when a force is applied to it.
A Driving Force is a force that is applied over and over again.
Resonance occurs when the driving force is applied at the natural frequency or multiples of the natural frequency
40 Natural Frequency Forced Vibration-Resonance
The frequency that a system acquires when a force is applied to it.
A Driving Force is a force that is applied over and over again.
Resonance occurs when the driving force is applied at the natural frequency or multiples of the natural frequency
Resonance produces large amplitude standing waves
41 Natural Frequency Forced Vibration-Resonance
The frequency that a system acquires when a force is applied to it.
A Driving Force is a force that is applied over and over again.
Resonance occurs when the driving force is applied at the natural frequency or multiples of the natural frequency
Resonance produces large amplitude standing waves
42 Natural Frequency Forced Vibration-Resonance
Resonance caused the Tacoma Narrows Bridge to collapse
Resonance can cause a wine glass to break
Resonance can is used in string instruments, open end wind instruments, and closed end tube wind instruments
43 Standing Waves
Nodes points of destructive interference
Antinodes points of constructive interference
Standing waves are produced at natural frequencies or resonant frequencies.
44 Standing Waves strings
L n l / 2
L the length of a string
Lambda equals the wavelength
n an interger
n 1 fundamental frequency
n 2 second harmonic
n 3 third hamonic
45 Standing Waves Open Springs continued.
Nodes are found at the fixed ends.
Antinodes are not possible at the fixed ends
The velocity on a string is directly related to its tension and inversely related to the mass per unit length.
46 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
47 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
48 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
49 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
50 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
51 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
52 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
53 Standing waves open end tubes
Antinodes are possible at the open ends
Ln l / 2
Llength of the tube
lambda wavelength
n 1 fundamental frequency
n 2 2nd harmonic
n 3 3rd harmonic
54 Standing waves open end tubes
v speed of sound
v (331 .6 T) m / s
55 Standing waves closed end tubes
L l / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
56 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
57 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
58 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
59 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
60 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
1 61 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
3 1 62 Standing waves closed end tubes
L lambda / 4
L length of the tube
lamda wavelength
antinodes are possible at the open end.
nodes are possible at the closed end.
Only odd harmonics are possible.
3 5 1 63 Beats
The rising and falling of sound intensity is known as beats
The beat frequency tells you how many cycles per second the source frequency is different than the standard frequency.
The beat frequency does not tell you if the source frequency is higher or lower than the standard.
64 Beats 65 Doppler Effect
ffo ( v - vo )
( v - vs)
vo velocity of the observer
vs velocity of the source.
vo observer towards source f increases WHY?
vo - source towards observer-f increases WHY?
66 Doppler Effect
ffo ( v - vo )
( v - vs)
vo observer towards source f increases WHY?
Multiply be a larger Numerator Higher f
vo - source towards observer-f increases WHY?
Divide by a smaller Denominator Higher f
67 Wave Motion
Matter is not carried in mechanical waves.
Energy is carried by mechanical waves.
A wave has a velocity equal to the product of..
its frequency and wavelength. V f lamda
68 Wave Motion
Matter is not carried in mechanical waves.
Energy is carried by mechanical waves.
A wave has a velocity equal to the product of..
its frequency and wavelength. V f lamda
69 Wave Motion
Matter is not carried in mechanical waves.
Energy is carried by mechanical waves.
A wave has a velocity equal to the product of..
its frequency and wavelength. V f lamda
70 Wave Motion
Matter is not carried in mechanical waves.
Energy is carried by mechanical waves.
A wave has a velocity equal to the product of..
its frequency and wavelength. V f l
71 Wave Properties
Amplitudemaximum height relative to
The equilibrium
Wavelengthdistance between crests
Frequency the number of crests which pass a given pt per second cycle per sec 1 Hz
72 Wave Properties
Amplitudemaximum height relative to
The equilibrium
Wavelengthdistance between crests
Frequency the number of crests which pass a given pt per second cycle per sec 1 Hz
73 Wave Properties
Amplitudemaximum height relative to
The equilibrium
Wavelengthdistance between crests
Frequency the number of crests which pass a given pt per second cycle per sec 1 Hz
74 Wave Properties
Amplitudemaximum height relative to
The equilibrium
Wavelengthdistance between crests
Frequency the number of crests which pass a given pt per second cycle per sec 1 Hz
75 Wave Properties
Amplitudemaximum height relative to
The equilibrium
Wavelengthdistance between crests
Frequency the number of crests which pass a given point per second cycle per sec 1 Hz
76 Wave Properties
Amplitudemaximum height relative to
The equilibrium
Wavelengthdistance between crests
Frequency the number of crests which pass a given pt per second cycle per sec 1 Hz
77 Velocity of a Wave on a string
v FT
(m/l)
FT is the equal to the
Tension in the string.
m / L is the
The mass per unit length of the string.
78 Velocity of a Wave on a string
v FT
(m/l)
FT is the equal to the
Tension in the string.
m / L is the
The mass per unit length of the string.
79 Velocity of a Wave on a string
v FT
(m/l)
FT Tension in the string.
m / L is the
The mass per unit length of the string.
80 Velocity of a Wave on a string
v FT
(m/l)
FT Tension in the string.
m / L is the
The mass per unit length of the string.
81 Velocity of a Wave on a string
v FT
(m/l)
FT Tension in the string.
m / L is the
The mass per unit length of the string.
82 Velocity of a Wave on a string
v FT
(m/l)
FT Tension in the string.
m / L is the
The mass per unit length of the string or..
83 Velocity of a Wave on a string
v FT
(m/l)
FT Tension in the string.
m / L is the
The mass per unit length of the string or..
Linear Density in kg/m
84 Types of waves
transverse..
Oscillation is perpendicular to the wave motion
(Electromagnetic waves are transverse waves
85 Types of waves
Longitudinal
Oscillation is parallel to the wave motion
(sound waves are longitudinal waves )
86 Types of waves
Longitudinal
Oscillation is parallel to the wave motion
(sound waves are longitudinal waves )
87 Speed of waves
The speed of a wave is directly related to the..
Elastic force factor and.
The interia factor (density of the medium
88 Speed of waves
The speed of a wave is directly related to the..
Elastic force factor and.
The interia factor (density of the medium
89 Wave intensity
Intensity is
The power transported across a unit area perpendicular the energy flow of a wave.
Intensity energy / time divided by area
Intensity power / area
Intensity Watt / meters squared.
The intensity of a wave decreases by 1/r2
90 Wave intensity
Intensity is
The power transported across a unit area perpendicular the energy flow of a wave.
Intensity energy / time divided by area
Intensity power / area
Intensity Watt / meters squared.
The intensity of a wave decreases by 1/r2
91 Wave intensity
Intensity is
The power transported across a unit area perpendicular the energy flow of a wave.
Intensity energy / time divided by area
Intensity power / area
Intensity Watt / meters squared.
The intensity of a wave decreases by 1/r2
92 Wave intensity
Intensity is
The power transported across a unit area perpendicular the energy flow of a wave.
Intensity energy / time divided by area
Intensity power / area
Intensity Watt / meters squared.
The intensity of a wave decreases by 1/r2
93 Wave intensity
Intensity is
The power transported across a unit area perpendicular the energy flow of a wave.
Intensity energy / time divided by area
Intensity power / area
Intensity Watt / meters squared.
The intensity of a wave decreases by 1/r2
94 Wave intensity
Intensity is
The power transported across a unit area perpendicular the energy flow of a wave.
Intensity energy / time divided by area
Intensity power / area
Intensity Watt / meters squared.
The intensity of a wave decreases by 1/r2
95 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
96 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
97 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
98 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
99 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
100 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
101 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
102 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
103 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
104 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
105 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
106 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
107 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
108 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
What is the intensity of a 75 dB sound wave?
75dB 10 log ( I / Io)
7.5 log ( I / Io)
7.5 log I log Io
7.5 log I log (1 x10-12 W/m2)
7.5 log I (-12)
7.5 12 log I
-4.5 log I
3.16 x10-5 W / m2 I
109 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
How many times more intense is a 120 dB sound wave
compared to a 80 dB sound wave?
120dB 80 dB 40 db
40 dB / 10 4
104 10,000 times greater
110 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
How many times more intense is a 120 dB sound wave
compared to a 80 dB sound wave?
120dB 80 dB 40 db
40 dB / 10 4
104 10,000 times greater
111 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
How many times more intense is a 120 dB sound wave
compared to a 80 dB sound wave?
120dB 80 dB 40 db
40 dB / 10 4
104 10,000 times greater
112 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
How many times more intense is a 120 dB sound wave
compared to a 80 dB sound wave?
120dB 80 dB 40 db
40 dB / 10 4
104 10,000 times greater
113 Decibels
Relative measure of the perceived loudness of a sound wave
Decibels are based on a logarithmic scale
dB10 log ( Intensity of the sound wave )
( Threshold of Human Hearing Intensity )
Threshold of Hearing 1x10-12 W/m2
How many times more intense is a 120 dB sound wave
compared to a 80 dB sound wave?
120dB 80 dB 40 db
40 dB / 10 4
104 10,000 times greater
114 Wave Reflection-Fixed end
A single wave crest which reflects off a fixed end will leave as a single wave trough.
The wave crests puts a force up on the fixed end.
The fixed puts an equal but opposite force on the string which produces an equal but opposite wave trough.
115 Wave Reflection-Fixed end
A single wave crest which reflects off a fixed end will leave as a single wave trough.
The wave crests puts a force up on the fixed end.
The fixed puts an equal but opposite force on the string which produces an equal but opposite wave trough.
116 Wave Reflection-Free end
A single wave peak which reflects off a free end will leave as a single wave peak.
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