Resonance and Musical Instruments Unit 8 Class 3 E. Alexander Burt
Review of Standing Waves Time to recall standing waves from the previous chapter. Remember the key characteristic of standing waves:  nodes and antinodes At the node, there is no displacement of the medium At the antinode, the displacement is a maximum. Remember the spring lab?
Standing waves on physical systems Think about a guitar string.  It is attached at each end.  Because of this, the ends are not free to move.  Therefore, there must be a node at each end. Now think about a tuning fork.  The metal is attached at one end and not at the other.  Therefore, there will be a node at the attached end and an antinode at the open end. Finally, think about a metal bar supported in the middle.  Neither end is attached, therefore both ends will be antinodes.
In a nutshell… The points where the physical medium is unable to move – such as the ends of the guitar string – must be nodes. If the medium ends without being “tied down” the end will be an antinode.
Node – Node:  what wave “fits?” If each end is a node, then any number of half waves will fit If the length of the string is L, then the formula is: L = n  /2 Solving for    we get:   = 2L / n
If each end is an antinode… The pattern is the same as if each end is a node.  Any number of half waves will fit.
Node - Antinode How much of a wave is between a node and an antinode?  ¼ of the wave. The next antinode happens at ¾ of the wave. Odd numbered quarter waves will fit.  If the length of the resonant column is L, that means: L = n   / 4  where n = 1, 3, 5…

U8 Cn3 Resonance

  • 1.
    Resonance and MusicalInstruments Unit 8 Class 3 E. Alexander Burt
  • 2.
    Review of StandingWaves Time to recall standing waves from the previous chapter. Remember the key characteristic of standing waves: nodes and antinodes At the node, there is no displacement of the medium At the antinode, the displacement is a maximum. Remember the spring lab?
  • 3.
    Standing waves onphysical systems Think about a guitar string. It is attached at each end. Because of this, the ends are not free to move. Therefore, there must be a node at each end. Now think about a tuning fork. The metal is attached at one end and not at the other. Therefore, there will be a node at the attached end and an antinode at the open end. Finally, think about a metal bar supported in the middle. Neither end is attached, therefore both ends will be antinodes.
  • 4.
    In a nutshell…The points where the physical medium is unable to move – such as the ends of the guitar string – must be nodes. If the medium ends without being “tied down” the end will be an antinode.
  • 5.
    Node – Node: what wave “fits?” If each end is a node, then any number of half waves will fit If the length of the string is L, then the formula is: L = n  /2 Solving for  we get:  = 2L / n
  • 6.
    If each endis an antinode… The pattern is the same as if each end is a node. Any number of half waves will fit.
  • 7.
    Node - AntinodeHow much of a wave is between a node and an antinode? ¼ of the wave. The next antinode happens at ¾ of the wave. Odd numbered quarter waves will fit. If the length of the resonant column is L, that means: L = n  / 4 where n = 1, 3, 5…