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5.5 Modeling Harmonic Motion
5.5 Modeling Harmonic Motion
We will do 5 problems on the handout you’ve received.
 Groups will do 1 & 2 ... then we’ll do 3-5 as a class.
5.5 Modeling Harmonic Motion
 We will do 5 problems on the handout you’ve received.
  Groups will do 1 & 2 ... then we’ll do 3-5 as a class.




Proverbs 3:5-6 Trust in the LORD with all your heart and
lean not on your own understanding; in all your ways
acknowledge him, and he will make your paths straight.
Frequency is defined as the reciprocal of
the period of a periodic function.
Frequency is defined as the reciprocal of
the period of a periodic function.

Problem 1 on your handout:
Frequency is defined as the reciprocal of
the period of a periodic function.

Problem 1 on your handout:

        amp. : 5 inches
               2π
        per. :     = 1 second
               2π
        freq.: 1 Hz.
Problem 2 on your handout:
Problem 2 on your handout:
   a.   amp. : .8
                 2π    2
        per. :       =
                 49π 49
                  49
         freq. :
                  2
Problem 2 on your handout:
   a.   amp. : .8
                 2π    2
        per. :       =
                 49π 49
                  49
         freq. :
                  2
   b.   increase a ... louder
        decrease a ... quieter
Problem 2 on your handout:
   a.   amp. : .8
                 2π    2
        per. :       =
                 49π 49
                  49
         freq. :
                  2
   b.   increase a ... louder
        decrease a ... quieter
   c.   increase freq. ... sharp
        decrease freq. ... flat
Problem 3 on your handout:
Problem 3 on your handout:
   function: cosine
Problem 3 on your handout:
   function: cosine
   amp.: 6
Problem 3 on your handout:
   function: cosine
   amp.: 6
   per.:
Problem 3 on your handout:
   function: cosine
   amp.: 6
                      normal period
   per.:     period =
                            b
Problem 3 on your handout:
   function: cosine
   amp.: 6
                      normal period
   per.:     period =
                           b
                   normal period
                b=
                      period
Problem 3 on your handout:
   function: cosine
   amp.: 6
                      normal period
   per.:     period =
                           b
                   normal period
                b=
                      period
                        2π
                     b=
                         1
                         4
Problem 3 on your handout:
   function: cosine
   amp.: 6
                      normal period
   per.:     period =
                           b
                   normal period
                b=
                      period
                         2π
                     b=
                          1
                          4
                     b = 8π
Problem 3 on your handout:
   function: cosine
   amp.: 6
                      normal period
   per.:     period =
                             b
                     normal period
                  b=
                        period
                             2π
                         b=
                              1
                              4
                         b = 8π
    y = 6 cos ( 8π t )
Problem 4 on your handout:
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:    -cosine
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:    -cosine

   amplitude:
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:    -cosine

   amplitude:   .35
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:    -cosine

   amplitude:   .35

   period:
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:    -cosine

   amplitude:   .35

                   2π
   period:      b=
                   5.2
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:     -cosine

   amplitude:    .35

                    2π
   period:       b=
                    5.2

   vertical shift:
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:     -cosine

   amplitude:    .35

                    2π
   period:       b=
                    5.2

   vertical shift:     4
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:     -cosine

   amplitude:    .35

                    2π
   period:       b=
                    5.2

   vertical shift:     4

                ⎛ 2π ⎞
   y = −.35 cos ⎜    t ⎟ + 4
                ⎝ 5.2 ⎠
Problem 4 on your handout:
   Let time = 0 be when the star is at it’s dimmest.

   function:     -cosine

   amplitude:    .35

                    2π           please include when
   period:       b=                 t = 0 as other
                    5.2
                                    equations are
   vertical shift:     4               possible.

                ⎛ 2π ⎞
   y = −.35 cos ⎜    t ⎟ + 4
                ⎝ 5.2 ⎠
Problem 5 on your handout:
Problem 5 on your handout:
   function:
Problem 5 on your handout:
   function:   cosine
Problem 5 on your handout:
   function:    cosine

   amplitude:
Problem 5 on your handout:
   function:    cosine

   amplitude:   135
Problem 5 on your handout:
   function:    cosine

   amplitude:   135

   period:
Problem 5 on your handout:
   function:    cosine

   amplitude:   135
                              1
   period:      frequency =
                            period
Problem 5 on your handout:
   function:    cosine

   amplitude:   135
                              1
   period:      frequency =
                            period
                               b
                  frequency =
                              2π
Problem 5 on your handout:
   function:    cosine

   amplitude:   135
                              1
   period:      frequency =
                            period
                              b
                 frequency =
                             2π
                2π gfrequency = b
Problem 5 on your handout:
   function:    cosine

   amplitude:   135
                              1
   period:      frequency =
                            period
                              b
                 frequency =
                             2π
                2π gfrequency = b
                      b = 140π
Problem 5 on your handout:
   function:    cosine

   amplitude:   135
                              1
   period:      frequency =
                            period
                              b
                 frequency =
                             2π
                2π gfrequency = b
                      b = 140π


   V = 135 cos (140π t )
HW #7

When you are not practicing, remember, someone
somewhere is practicing, and when you meet him
he will win.                  Ed Macauley

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0508 ch 5 day 8

  • 2. 5.5 Modeling Harmonic Motion We will do 5 problems on the handout you’ve received. Groups will do 1 & 2 ... then we’ll do 3-5 as a class.
  • 3. 5.5 Modeling Harmonic Motion We will do 5 problems on the handout you’ve received. Groups will do 1 & 2 ... then we’ll do 3-5 as a class. Proverbs 3:5-6 Trust in the LORD with all your heart and lean not on your own understanding; in all your ways acknowledge him, and he will make your paths straight.
  • 4. Frequency is defined as the reciprocal of the period of a periodic function.
  • 5. Frequency is defined as the reciprocal of the period of a periodic function. Problem 1 on your handout:
  • 6. Frequency is defined as the reciprocal of the period of a periodic function. Problem 1 on your handout: amp. : 5 inches 2π per. : = 1 second 2π freq.: 1 Hz.
  • 7. Problem 2 on your handout:
  • 8. Problem 2 on your handout: a. amp. : .8 2π 2 per. : = 49π 49 49 freq. : 2
  • 9. Problem 2 on your handout: a. amp. : .8 2π 2 per. : = 49π 49 49 freq. : 2 b. increase a ... louder decrease a ... quieter
  • 10. Problem 2 on your handout: a. amp. : .8 2π 2 per. : = 49π 49 49 freq. : 2 b. increase a ... louder decrease a ... quieter c. increase freq. ... sharp decrease freq. ... flat
  • 11. Problem 3 on your handout:
  • 12. Problem 3 on your handout: function: cosine
  • 13. Problem 3 on your handout: function: cosine amp.: 6
  • 14. Problem 3 on your handout: function: cosine amp.: 6 per.:
  • 15. Problem 3 on your handout: function: cosine amp.: 6 normal period per.: period = b
  • 16. Problem 3 on your handout: function: cosine amp.: 6 normal period per.: period = b normal period b= period
  • 17. Problem 3 on your handout: function: cosine amp.: 6 normal period per.: period = b normal period b= period 2π b= 1 4
  • 18. Problem 3 on your handout: function: cosine amp.: 6 normal period per.: period = b normal period b= period 2π b= 1 4 b = 8π
  • 19. Problem 3 on your handout: function: cosine amp.: 6 normal period per.: period = b normal period b= period 2π b= 1 4 b = 8π y = 6 cos ( 8π t )
  • 20. Problem 4 on your handout:
  • 21. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest.
  • 22. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function:
  • 23. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine
  • 24. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude:
  • 25. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35
  • 26. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35 period:
  • 27. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35 2π period: b= 5.2
  • 28. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35 2π period: b= 5.2 vertical shift:
  • 29. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35 2π period: b= 5.2 vertical shift: 4
  • 30. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35 2π period: b= 5.2 vertical shift: 4 ⎛ 2π ⎞ y = −.35 cos ⎜ t ⎟ + 4 ⎝ 5.2 ⎠
  • 31. Problem 4 on your handout: Let time = 0 be when the star is at it’s dimmest. function: -cosine amplitude: .35 2π please include when period: b= t = 0 as other 5.2 equations are vertical shift: 4 possible. ⎛ 2π ⎞ y = −.35 cos ⎜ t ⎟ + 4 ⎝ 5.2 ⎠
  • 32. Problem 5 on your handout:
  • 33. Problem 5 on your handout: function:
  • 34. Problem 5 on your handout: function: cosine
  • 35. Problem 5 on your handout: function: cosine amplitude:
  • 36. Problem 5 on your handout: function: cosine amplitude: 135
  • 37. Problem 5 on your handout: function: cosine amplitude: 135 period:
  • 38. Problem 5 on your handout: function: cosine amplitude: 135 1 period: frequency = period
  • 39. Problem 5 on your handout: function: cosine amplitude: 135 1 period: frequency = period b frequency = 2π
  • 40. Problem 5 on your handout: function: cosine amplitude: 135 1 period: frequency = period b frequency = 2π 2π gfrequency = b
  • 41. Problem 5 on your handout: function: cosine amplitude: 135 1 period: frequency = period b frequency = 2π 2π gfrequency = b b = 140π
  • 42. Problem 5 on your handout: function: cosine amplitude: 135 1 period: frequency = period b frequency = 2π 2π gfrequency = b b = 140π V = 135 cos (140π t )
  • 43. HW #7 When you are not practicing, remember, someone somewhere is practicing, and when you meet him he will win. Ed Macauley

Editor's Notes

  1. 1. Make sure students have copies of the example problems.\n\n
  2. 1. Make sure students have copies of the example problems.\n\n
  3. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  4. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  5. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  6. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  7. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  8. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  9. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  10. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  11. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  12. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  13. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  14. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  15. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  16. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  17. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  18. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  19. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  20. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  21. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  22. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  23. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  24. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  25. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  26. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  27. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  28. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  29. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  30. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  31. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  32. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  33. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  34. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  35. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  36. 1. After Example 1 has been presented, discuss a weight hanging from a spring: when compressed up and released ... t=0 at the top; pulled down and released ... t=0 at the bottom. Also discuss the resulting trig functions which need to be used to model these cases.\n
  37. 1. Make sure students have copies of the example problems.\n\n