Understanding Simple Harmonic Motion: Position and Velocity Functions Explained

Click For Summary

Discussion Overview

The discussion revolves around the position and velocity functions of simple harmonic motion, specifically the need to verify the phase constant ϕ using both position and velocity at time t=0. Participants explore the implications of multiple solutions in trigonometric functions and their relevance to the physics of harmonic motion.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant states that after determining the position function, it is necessary to check the velocity function at t=0 to confirm the phase constant ϕ.
  • Another participant suggests that the need to check v(0) arises because a given x value can be crossed during upward or downward motion.
  • Concerns are raised about the ambiguity in choosing values when using inverse trigonometric functions, particularly in the context of multiple solutions within a specified interval.
  • Some participants discuss the mathematical properties of inverse functions, noting that arccos has a restricted interval to ensure a single solution.
  • A participant presents a graph to illustrate that multiple x values can correspond to the same y value in periodic functions, emphasizing the need for initial conditions for both position and velocity to uniquely define ϕ.
  • There is a discussion about the nature of the arcsin and arccos functions, with one participant expressing confusion about how arcsin can be a function given the multiple solutions of sin(x)=y.
  • Another participant provides definitions of the arcsin, arccos, and arctan functions in the context of real analysis.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the necessity of checking both position and velocity functions. There is no consensus on the best approach to resolving the ambiguities presented by inverse trigonometric functions and their implications for defining the phase constant ϕ.

Contextual Notes

Participants highlight the limitations of using inverse trigonometric functions without considering the periodic nature of sine and cosine, which can lead to multiple solutions. The discussion also reflects the dependence on definitions and the context of the problem in both mathematics and physics.

tahayassen
Messages
269
Reaction score
1
[tex]x(t)=Acos(ωt+ϕ)\\v(t)=-ωAsin(ωt+ϕ)[/tex]

I think my physics professor said in one of the lectures that: after setting up your position function by finding amplitude, angular speed, and solving for ϕ by setting t=0 and using the x(0) value given in the question, you need to to set t=0 in the velocity function and use the v(0) value to make sure your ϕ value is correct.

I'm confused. Why is this necessary?
 
Physics news on Phys.org
If you have some x value you can cross it on the way up or on the way down, this is why you need to check v(0)
 
0xDEADBEEF said:
If you have some x value you can cross it on the way up or on the way down, this is why you need to check v(0)

Hmmm... That seems weird.
 
tahayassen said:
Hmmm... That seems weird.

Not really. When you do the inverse cos at some point, how do you know which value to take - there are two solutions in the 0 to 2pi interval.
 
mickybob said:
Not really. When you do the inverse cos at some point, how do you know which value to take - there are two solutions in the 0 to 2pi interval.
Arccos has a restricted interval so that you only get one solution otherwise you can't even define Arccos. Inverse maps can only be defined if the original mapping is bijective with respect to the codomain.
 
Okay, this still doesn't make sense to me.

Attached is a graph of f(x) and f'(x). When you do the inverse sign you get a value plus [itex]2πn[/itex] where n is an integer.

For example:
[tex]sin(x)=1\\<br /> x={π\over 2}+2πn[/tex]
Each x value would be 1 period apart. Therefore, as you can see in the diagram, points A, B, and C are all 1 period apart, and f'(A)=f'(B)=f'(C).
 

Attachments

  • Untitled.jpg
    Untitled.jpg
    20.4 KB · Views: 413
WannabeNewton said:
Arccos has a restricted interval so that you only get one solution otherwise you can't even define Arccos. Inverse maps can only be defined if the original mapping is bijective with respect to the codomain.

Yes, if you want to be a mathematical pedant, this is true.

Although note I did say inverse cos and not arccos.

More correctly then:

[tex]x(t)=Acos(ωt+ϕ)[/tex] has two solutions in the interval 0 < [itex]\phi[/itex] < 2[itex]\pi[/itex]

In any case, the important thing is the physics of the problem, not mathematical conventions.
 
Last edited:
tahayassen said:
Okay, this still doesn't make sense to me.

Attached is a graph of f(x) and f'(x). When you do the inverse sign you get a value plus [itex]2πn[/itex] where n is an integer.

For example:
[tex]sin(x)=1\\<br /> x={π\over 2}+2πn[/tex]
Each x value would be 1 period apart. Therefore, as you can see in the diagram, points A, B, and C are all 1 period apart, and f'(A)=f'(B)=f'(C).

If you look at the top graph, you'll see that, inbetween A and B, there are two points where the plotted curve crosses any value on the y axis.

Mathematically, there are generally two solutions of
[tex]sin(x)=y[/tex]
in the range 0 [itex]\leq[/itex] y < 2[itex]\pi[/itex].

Your example of
[tex]sin(x)=1[/tex] is a special case because it's a turning point.

In terms of the physics:

The pendulum returns to its initial position twice within the period.

The difference is that it is now moving in the opposite direction, so the velocity has changed sign.

So we need an initial condition for the velocity as well as the position in order to uniquely define [itex]\phi[/itex]
 
Last edited:
mickybob said:
Mathematically, there are generally two solutions of
[tex]sin(x)=y[/tex]
in the range 0 [itex]\leq[/itex] y < 2[itex]\pi[/itex].

Then how is arcsin a function? I think I get it now. Dang. My trig is rusty.
 
  • #10
In real analysis the arcsin function is defined as
[tex]\arcsin:[-1,1] \rightarrow [-\pi/2,\pi/2],[/tex]
arccos as
[tex]\arccos:[-1,1] \rightarrow [0,\pi],[/tex]
and arctan as
[tex]\arctan:\mathbb{R} \rightarrow (-\pi/2,\pi/2).[/tex]
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 11 ·
Replies
11
Views
16K
  • · Replies 3 ·
Replies
3
Views
8K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 6 ·
Replies
6
Views
6K
  • · Replies 17 ·
Replies
17
Views
3K