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.
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.
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
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 ⎠
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. Make sure students have copies of the example problems.\n\n
1. Make sure students have copies of the example problems.\n\n
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1. Make sure students have copies of the example problems.\n\n