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**2**

B

Pressure vs. Position Graph

P

x

A

C

A: P = 0; P = P0

B: P > 0; P = Pmax

C: P < 0; P = Pmin

animation

Slide 6

The pressure at a given point does not stay constant. If we only observed one position we would find the pressure there varies sinusoidally with time, ranging from:

P0 to P0 + Pmax back to P0 then to P0 - Pmax and back to P0

The time it takes to go through this cycle is the period of the wave. The number of times this cycle happens per second is the frequency of the wave in Hertz.

Therefore, the pressure in the medium is a function of both position and time!

The cycle can also be described as:

equilibrium compression equilibrium rarefaction equilibrium

Slide 7

P

T

t

Rather than looking at a region of space at an instant in time, here we’re looking at just one point in space over an interval of time. At time zero, when the pressure readings began, the molecules were at their normal pressure. The pressure at this point in space fluctuates sinusoidally as the waves pass by: normal high normal low normal. The time needed for one cycle is the period. The higher the frequency, the shorter the period. The amplitude of the graph represents the maximum deviation from normal pressure (as it did on the pressure vs. position graph), and this corresponds to loudness.

Slide 8

Pressure vs. Position: The graph is for a snapshot in time and displays pressure variation for over an interval of space. The distance between peaks on the graph is the wavelength of the wave.

Pressure vs. Time: The graph displays pressure variation over an interval of time for only one point in space. The distance between peaks on the graph is the period of the wave. The reciprocal of the period is the frequency.

Both Graphs: Sound waves are longitudinal even though these graphs look like transverse waves. Nothing in a sound wave is actually waving in the shape of these graphs! The amplitude of either graph corresponds to the loudness of the sound. The absolute pressure matters not. For loudness, all that matters is how much the pressure deviates from its norm, which doesn’t have to be much. In real life the amplitude would diminish as the sound waves spread out.

Slide 9

As with all waves, the speed of sound depends on the medium through which it is traveling. In the wave unit we learned that the speed of a wave traveling on a rope is given by:

- Sound
- Longitudinal Waves
- Sound Waves: Molecular View
- Pressure vs. Position
- Pressure vs. Time
- Pressure vs. Time Graph
- Comparison of Pressure Graphs
- Speed of Sound
- Mach Numbers
- Temperature & the Speed of Sound
- Frequency & Pitch
- The Human Ear
- Range of Human Hearing
- Echoes & Reverberation
- Sonar
- Doppler Effect
- Sonic Booms
- Doppler Problem
- Interference: Distance in Wavelengths
- Interference: Sound Demo
- Interference: Noise Reduction
- Acoustics
- Standing Waves: 2 Fixed Ends
- Vibrating String Example
- Tuning Forks & Resonance
- Resonance: Shattering a Glass
- Standing Waves: Musical Instruments
- Complex Sounds
- Octaves & Ratios
- Beats
- Beats Example
- Intesity
- Intensity Example
- Threshold Intensity
- Sound Level in Decibels
- The Decibel Scale
- Decibel Example

- Waves & Sound
- Simulation at NASA for the Space Radiation Effort
- Newton’s third law of motion
- Newton’s laws of motion
- Resource Acquisition and Transport in Vascular Plants
- Sound
- Newton’s law of universal gravitation

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