| Term 
 | Definition 
 
        | Particle oscillation is perpendicular to wave propagation ex. Light waves |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Particle oscillation is parallel to the wave propagation ex. Sound waves |  | 
        |  | 
        
        | Term 
 | Definition 
 | 
        |  | 
        
        | Term 
 | Definition 
 | 
        |  | 
        
        | Term 
 
        | Principle of Superposition |  | Definition 
 
        | When two waves interact it causes the resultant wave to have an amplitude equal to the sum of the 2 waves |  | 
        |  | 
        
        | Term 
 
        | Constructive Interference |  | Definition 
 
        | When 2 waves are perfectly in phase (0o or 360o) the resulting amplitude is 2x the amplitude of the waves |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | When 2 waves are perfectly in phase (180o) the resulting amplitude is zero since the amplitude of the waves will cancel each other out |  | 
        |  | 
        
        | Term 
 
        | How does sound waves change as they pass through different mediums? |  | Definition 
 
        | Sound travels fastest through a solid and slowest through a gas |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | fo=fs(v±vov∓vs)
 
   f=fo(v±vdv∓vs)
   :where fo is the emitted frequency |  | 
        |  | 
        
        | Term 
 
        | Sign Convention of Doppler Effect Equation |  | Definition 
 
        | If object is moving away from the other object: Use bottom sign If object is moving towards other object: Use top sign |  | 
        |  | 
        
        | Term 
 | Definition 
 | 
        |  | 
        
        | Term 
 | Definition 
 
        | Β=10 log(I/Io) :where Io is the threshold of hearing with a value of 1e-12 W/m2(dB) |  | 
        |  | 
        
        | Term 
 
        | Change in Sound Level Equation |  | Definition 
 | 
        |  | 
        
        | Term 
 
        | Length of Standing Waves: Strings |  | Definition 
 
        | L=n(λ/2): where n is the harmonic number (#of antinodes/half-wavelengths) |  | 
        |  | 
        
        | Term 
 
        | Wavelength of Standing Waves: Strings |  | Definition 
 | 
        |  | 
        
        | Term 
 
        | Wavelength of Standing Waves: Strings |  | Definition 
 
        | λ=2L/n :where n is the harmonic number (# of antinodes/half-wavelengths) |  | 
        |  | 
        
        | Term 
 
        | Frequency of Standing Waves: Strings |  | Definition 
 
        | f=nv/2L :where n is the harmonic number (# of antinodes/half-wavelengths) |  | 
        |  | 
        
        | Term 
 
        | Length of Standing Waves: Open Pipes |  | Definition 
 
        | L=n(λ/2) :where n is the harmonic number (# of nodes/half-wavelengths) |  | 
        |  | 
        
        | Term 
 
        | Wavelength of Standing Waves: Open Pipes |  | Definition 
 
        | λ=2L/n :where n is the harmonic number (# of nodes/half-wavelengths) |  | 
        |  | 
        
        | Term 
 
        | Frequency of Standing Waves: Open Pipes |  | Definition 
 
        | f=nv/2L :where n is the harmonic number (# of nodes/half-wavelengths) |  | 
        |  | 
        
        | Term 
 
        | Length of Standing Waves: Closed Pipes |  | Definition 
 
        | L=n(λ/4) :where n is the harmonic number and can only be odd number |  | 
        |  | 
        
        | Term 
 
        | Wavelength of Standing Waves: Closed Pipes |  | Definition 
 
        | λ=4L/n :where n is the harmonic number that can only be odd numbers |  | 
        |  | 
        
        | Term 
 
        | Frequency of Standing Waves: Closed Pipes |  | Definition 
 
        | f=nv/4L :where n is the harmonic number that can only be odd numbers |  | 
        |  |