Understanding Simple Harmonic Motion: Explaining x=Acos(wt+phi)

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SUMMARY

The discussion centers on the equation of Simple Harmonic Motion represented as x=Acos(wt+phi). Participants clarify the significance of the phase constant phi in determining the initial position of the oscillating system at time t=0. When phi=0, the system starts at its maximum displacement (x=A), while a non-zero phi indicates a different starting position. The relationship between the initial displacement x(0) and phi is crucial for understanding the motion's behavior over time.

PREREQUISITES
  • Understanding of Simple Harmonic Motion (SHM)
  • Familiarity with trigonometric functions, particularly cosine
  • Knowledge of angular frequency (ω) and amplitude (A)
  • Basic grasp of periodic functions and their properties
NEXT STEPS
  • Explore the implications of different values of phi in SHM equations
  • Learn about the graphical representation of Simple Harmonic Motion
  • Investigate the relationship between phase shift and initial conditions in oscillatory systems
  • Study the effects of varying amplitude and frequency on the motion of oscillators
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillations, as well as educators seeking to clarify concepts related to Simple Harmonic Motion.

Jozefina Gramatikova
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Homework Statement



x=Acos(wt+phi)

Homework Equations


can somebody explain to me please when phi=0. I saw many different questions with many solutions and I can't understand when we have just x=Acos(wt) and when x=Acos(wt+phi)

The Attempt at a Solution

 
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Jozefin Gramatikova said:

Homework Statement



x=Acos(wt+phi)

Homework Equations


can somebody explain to me please when phi=0. I saw many different questions with many solutions and I can't understand when we have just x=Acos(wt) and when x=Acos(wt+phi)

The Attempt at a Solution


It depends where the system starts at ##t=0##.
 
So, if it starts from x=0 at t=0 => phi=0? and at t=0 x=1 => phi would be different from zero?
 
Jozefin Gramatikova said:
So, if it starts from x=0 at t=0 phi=0? and at t=0 x=1 phi would be different from zero?

Yes. ##-A \le x(0) \le A##, where ##x(0)## is the displacement of the system at ##t=0##, and determines ##\phi##.
 
Jozefin Gramatikova said:
So, if it starts from x=0 at t=0 => phi=0? and at t=0 x=1 => phi would be different from zero?
Plug t=0 and ##\phi=0## into ##x(t) = A\cos(\omega t + \phi)##. Is ##x(0)## equal to 0?
 
vela said:
Plug t=0 and ##\phi=0## into ##x(t) = A\cos(\omega t + \phi)##. Is ##x(0)## equal to 0?
x(t)=Acos(0)
x(t)=A
 
Jozefin Gramatikova said:
x(t)=Acos(0)
x(t)=A
Presumably ##A \ne 0## otherwise there'd be no oscillating going on, so clearly ##x(0)=0## and ##\phi=0## contradict each other.
 
Jozefin Gramatikova said:
So, if it starts from x=0 at t=0 => phi=0?
No.
If it is at x0 at t=0 and at x=Acos(ωt+φ) at time t, what equation can you write for x0?
 
I don't know I am really confused right now.
 
  • #10
Jozefin Gramatikova said:
I don't know I am really confused right now.

##\cos(0) = 1##
 
  • #11
PeroK said:
##\cos(0) = 1##
I know that :D Thats why I said:
"x(t)=Acos(0)
x(t)=A"
 
  • #12
Jozefin Gramatikova said:
I don't know I am really confused right now.
Just substitute those t and x values in the general equation in post #8.
 
  • #13
Jozefin Gramatikova said:
x(t)=Acos(0)
When plugging in a value for t you should replace all occurrences of t.
 
  • #14
Jozefin Gramatikova said:
I know that :D Thats why I said:
"x(t)=Acos(0)
x(t)=A"
You did not seem to know it in post #3.
 
  • #15
haruspex said:
Just substitute those t and x values in the general equation in post #8.
x=Acos(ωt+φ)
x0=Acos(ω x 0+φ)
x0=Acos(ω x 0+φ)
x0=Acos(φ)?
 
  • #16
Could you give me the right solution, please? I get more and more confused with every single post.
 
  • #17
Jozefin Gramatikova said:
Could you give me the right solution, please? I get more and more confused with every single post.

Let's assume that ##A>0##, so when ##x(t) = A \cos( \omega t + \phi)##, the value of ##x(t)## oscillates back and forth between ##-A## and ##+A##. That is, ##-A \leq x(t) \leq A## for all ##t##. Furthermore, we have ##x = -A## for some ##t## and ##x = +A## for some other ##t##.

If ##\phi = 0## we have ##x(0) = A##, so that means that the motion starts at time zero from the upper end of the allowed interval. Then for a while ##x(t)## will decrease until it hits the lower end ##-A## of the allowed interval, at time ##\pi/\omega##. Then it will start to increase until it hits ##x=A## at time ##2 \pi/\omega,## etc., etc.

If you want ##x(0)## to be a point other than ##A## you need to have ##\phi \neq 0.## To help you to enhance your understanding, try the following question: "what would be the value of ##\phi## if you require ##x(0) = 0?## (Of course, because the ##\cos## function is periodic there will be many values of ##\phi## that will work, but among these there is one that is "simplest", and that is the one you should attempt to find.)
 
Last edited:
  • #18
Jozefin Gramatikova said:
x0=Acos(φ)?
Yes.
 

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