Sound Sound travels as a longitudinal wave (like a slinky). A sound wave needs a medium in which to travel (like air or water). The speed of sound in air depends on the temperature of the air. Vsound = (331 m/s) [1 + (T/273)] T = temperature of air in º C. Speed of sound - example What is the speed of a sound wave in air at 22.0º C (room temperature)? Vsound = (331 m/s) [1 + (T/273)] Vsound = (331 m/s) [1 + (22/273)] Vsound = 344 m/s Use this value for the speed of sound if a temperature isn’t given. Sound and music Musically, each note has a characteristic frequency. For example, a low C has a frequency of 261.6 Hz, a D has a frequency of 293.7 Hz, an E has a frequency of 329.6 Hz Note that this does NOT correspond to a directly linear relationship between note and frequency. Standing waves A standing wave is the result of identical waves traveling in opposite directions. It has nodes (a stationary amplitude of zero) and anti-nodes (a maximum amplitude that is stationary). Nodes and anti-nodes on a standing wave Strings and music Plucking, striking, or bowing a string sets up a standing wave. Nodes (stationary zero amplitude) must exist at the ends of the string (cuz the ends are attached and can’t move) Antinodes (stationary maximum amplitude) exist at regularly spaced intervals throughout the string. Air columns and music An instrument often consists of a column of air that resonates at frequencies. The length of the column of air determines the frequency at which it resonates (and so the note that is heard). The length can be changed by opening and closing keys (like on a trumpet or flute) or by extending the slide of a trombone. We study 2 types of air columns: Closed-end air columns: A closed-end air column is closed at one end. A node must be at the closed end. An anti-node must be at the open end. A wave (with wavelength λ) will resonate in a closed end air column of length L if: λ = 4L. Open-end air columns: An open-end air column is open at both ends. Anti-nodes must be at each open end. A wave (with wavelength λ) will resonate in an open end air column of length L if: λ = 2L. Both open and closed end air columns will resonate at more than 1 frequency (called harmonics). Open & Closed End Air Columns Sound demo and activity Demo of sound in a vacuum. Speed of sound of music lab. Beats When 2 notes of different frequencies sound at the same time, a phenomenon called “beats” occurs in which the loudness varies at a regular intervals. The frequency of the beats = |f2–f1| If 450 Hz and 457 Hz are sounded at the same time, an observer will hear 7 beats per second. Beats picture If we added the amplitude of waves a + b, we would get wave c. If t2 = 1 sec, then wave a has 2.5 waves/second = 2.5 Hz. Wave b = 3 Hz. fbeats = .5 Hz (once every 2 seconds it has complete destructive interference - a node) Octaves A note an octave above is twice the frequency. So if a note had a frequency of 250 Hz, what would be the frequency of the note an octave above? 2(250 Hz) = 500 Hz What would be the frequency of the note an octave above that? 2(500 Hz) = 1000Hz Echoes An echo travels there and back again. It travels twice the distance in twice the time. If it takes t seconds for the echo to return from a surface, then it took ½t to get to the surface. If a surface is d meters away, then the echo will travel 2d meters. Echoes - example If a physics student screams towards the whiteboard, and hears the echo of her scream 0.26 seconds later, how far away is the whiteboard? Assume room temperature. The time it took the scream to reach the whiteboard is ½ (.26 s) = 0.13 s. v = d/t 344 m/s = d/.13 s d = 45 m (big classroom!) Doppler Effect Doppler effect – a change in the observed frequency of waves (light or sound) stemming from motion of the source and/or observer relative to each other. Lucky you, you live in the MidWest and hear the Doppler effect regularly. Hint: it is a train whistle Doppler is due to relative motion between source and observer In figure a, the source is stationary and λ (the distance btwn the waves) is constant. In figure b, the source is moving towards observer A, and λ decreases for observer A. At the same time, λ increases for observer C (because the source is moving away). Doppler simulation This simulation shows waves being generated by a moving source. The wavelength is shorter in front of the moving source, and longer in back of the moving source. Click here for the simulation. Doppler Equations For observer and source approaching each other: fo = f (v + vo) / (v – vs) Where fo = observed frequency (Hz) f = frequency of sound or light (Hz) v = velocity of sound or light (m/s) vo = velocity of observer (m/s) vs = velocity of source (m/s) Doppler Equations For observer and source moving away from each other: fo = f (v - vo) / (v + vs) Doppler Example What is the observed frequency of a 225 Hz train whistle as heard by a passenger in a car moving at 10 m/s towards a train that is oncoming at 25 m/s? Assume room temperature. f = 225 Hz v = 344 m/s vo = 10 m/s vs = 25 m/s Doppler Example fo = f (v + vo) / (v - vs) fo = 225 Hz (344 m/s + 10 m/s) / (344 m/s – 25 m/s) fo = 250 Hz Doppler Explanation Note that the frequency is higher when the observer and source are approaching each other. This corresponds to a higher pitch. Similarly, the frequency (and pitch) is lower when the observer and source are moving away from each other. In part, this lower pitch is why a receding train whistle is called a “melancholy” or “plaintive” sound. See? Physics really is everywhere. Remember waves that are closer together are higher in frequency and pitch, farther apart are lower in frequency and pitch Doppler effect influences sound, light, and any type of wave References http://www.revisionworld.com/files/wave.jpg http://www.physics.uc.edu/~sitko/CollegePhysicsIII/14Sound/Sound_files/image035.jpg http://electron9.phys.utk.edu/phys135d/modules/m10/im ages/stand.gif http://www.pas.rochester.edu/~afrank/A105/LectureVI/FG 03_005_PCT.gif http://www.ifa.hawaii.edu/~stockton/a110/imag es/Doppler_effect.jpg http://www.phschool.com/atschool/science_activity_librar y/images/properties_sound_doppler.jpg http://www.ifa.hawaii.edu/~barnes/ast110_06/tsaas/Dop pler_effect.jpg