Simple Harmonic Oscillation on a guitar string

In summary: The magnitude of the velocity and acceleration are determined by the equations, and the jerk is maximal when the sine and cosine functions are at their maximum values.
  • #1
kgal
43
0

Homework Statement


A guitar string vibrates at a frequency of 440 Hz. A point at its center moves in SHM with an amplitude of 3.0 mm and a phase angle of zero.
a. Write an equation for the position of the center of the string as a function of time.
b. What are maximum values of the magnitude of the velocity and the acceleration of the center of the string?
c. The derivative of the acceleration with respect to time is a quantity called jerk. Write an equation for the jerk of the center of the string as a function of time and find the maximum value of the magnitude of the jerk.


Homework Equations


x(t) = Acos(ωt + ρ)
ω = 2∏f = v/r

The Attempt at a Solution


a. I found that x(t) = Acos(ωt + ρ) = Acos(ωt).
b. d/dt x(t)= dx/dt = v(t) = -Aωsint(ωt) = 0
dv/dt = a(t) = Aω^2cos(ωt) = 0
I know that you need to set the equations equal to zero in order to find maximum magnitudes but I'm stuck from there on.

c. da/dt = jerk = -Aω^3sin(ωt) = 0.
same problem for me as in section b where I had trouble understanding how I find the max. jerk.
 
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  • #2
kgal said:

Homework Statement


A guitar string vibrates at a frequency of 440 Hz. A point at its center moves in SHM with an amplitude of 3.0 mm and a phase angle of zero.
a. Write an equation for the position of the center of the string as a function of time.
b. What are maximum values of the magnitude of the velocity and the acceleration of the center of the string?
c. The derivative of the acceleration with respect to time is a quantity called jerk. Write an equation for the jerk of the center of the string as a function of time and find the maximum value of the magnitude of the jerk.


Homework Equations


x(t) = Acos(ωt + ρ)
ω = 2∏f = v/r

The Attempt at a Solution


a. I found that x(t) = Acos(ωt + ρ) = Acos(ωt).
b. d/dt x(t)= dx/dt = v(t) = -Aωsint(ωt) = 0
dv/dt = a(t) = Aω^2cos(ωt) = 0
I know that you need to set the equations equal to zero in order to find maximum magnitudes but I'm stuck from there on.

c. da/dt = jerk = -Aω^3sin(ωt) = 0.
same problem for me as in section b where I had trouble understanding how I find the max. jerk.

The sine and cosine functions, all by themselves, both have maximum amplitudes. What are they? What does that say about the maximum or minimum values that the velocity and acceleration functions can have?
 
  • #3
maximum of sine and cosine functions are 1. so do I set up cos/sin(wt) = 1?
 
  • #4
No, because that's incorrect. But x max = A, v max = Aω, etc.
 
  • #5
kgal said:
maximum of sine and cosine functions are 1. so do I set up cos/sin(wt) = 1?

Only the sine and cosine functions are varying in your expressions for position, velocity and acceleration. They are multiplied by constants. If you know the maximum values that the sine and cosine functions can have, then you should be able to say what the minimums and maximums will be for the position, velocity and acceleration without doing any calculus.
 
  • #6
got it, thanks!
 
  • #7
I realize this is an old thread, but I'm working on this same problem now. I understand the equations and have the solutions to each part, but what I don't understand is the signs in the answers. For instance, in part A), the correct answer is given as x(t)=.003cos(-2764.6t). It's easy enough to write in the amplitude and find omega, but why is omega negative here? Further, when determining the equation for the jerk, the correct answer is given as j(t)=(6.3x10^7)sin(2764.6t). How is it that omega now became positive through the process of taking derivatives?? I'm trying to work on these wave functions for my final exam, help would be much appreciated
 
  • #8
leonardthecow said:
I realize this is an old thread, but I'm working on this same problem now. I understand the equations and have the solutions to each part, but what I don't understand is the signs in the answers. For instance, in part A), the correct answer is given as x(t)=.003cos(-2764.6t). It's easy enough to write in the amplitude and find omega, but why is omega negative here? Further, when determining the equation for the jerk, the correct answer is given as j(t)=(6.3x10^7)sin(2764.6t). How is it that omega now became positive through the process of taking derivatives?? I'm trying to work on these wave functions for my final exam, help would be much appreciated

The original problem statement did not include expected answers. Where do your "correct" answers come from?

There's no need to plug in values to find ω, since ω can be found directly from the given frequency of vibration, 440 Hz. ##\omega = 2\pi f##.

Keep in mind that for functions of the form A*sin(t), that A is the magnitude of an oscillation, so the function will take on values between the extremes -A to +A. When you take the derivative and the resulting function ends up with a negative sign in front of it (because, for example, the derivative of Bcos(ωt) is -ωBsin(ωt)), then the amplitude is ωB; Amplitudes are positive values. The "-" sign tells you the relationship between the phase of the derivative sin() function and the original Bcos() function. Note that ## -ω B sin(ω t) = ω B sin(ω t + \pi)##, so the "-" sign can be easily interpreted as a 180° phase shift.
 
  • #9
I should have specified, this example comes from the Mastering Physics website, and is an old problem set I am reworking for practice. The correct answer that they identify is x(t)=.003cos(-2764.6t), or x(t)=.003cos[-440(2pi)t].

What I was originally confused about was the fact that they identify the correct omega to have a minus sign in front of it. I used the general equation x(t)=Acos(ωt+φ), with a phase shift in this case of 0. Plugging in f, ω=2π(440 Hz); there is no negative sign here, nor was it clear to me where it came from (when I originally entered x(t)=.003cos(880π), the website marked it as incorrect, with the message "check your signs".) This seems to imply that the answer takes the form of x(t)=Acos(-ωt), and I'm unsure of why that is. Am I misunderstanding your response?

Thank you for your explanation of signs in relation to phases, that hadn't explicitly occurred to me before and it helps to clarify things conceptually. However, I'm still not sure in this case why the sign in front of ω is affected, not the sign in front of A. Thank you
 
  • #10
leonardthecow said:
Thank you for your explanation of signs in relation to phases, that hadn't explicitly occurred to me before and it helps to clarify things conceptually. However, I'm still not sure in this case why the sign in front of ω is affected, not the sign in front of A. Thank you
Well then, it's a mystery to me, too. I can't think of any good physical reason to introduce what are essentially either negative frequencies or negative times. Both seem distinctly unphysical things for introductory classical mechanics, and as far as I can tell are unwarranted for this problem.

Of course, mathematically cos(-θ) = cos(θ) so it makes no difference...
 
  • #11
Thanks for all your help! Knowing I'm not totally losing it then helps as much as a physical answer would. I guess by virtue of the definition that cos(-θ)=-cos(θ), maybe they're assuming that the guitar string is initially being released from the negative direction of maximum displacement? Not sure why... Regardless, thank you for your time
 

1. What is Simple Harmonic Oscillation on a guitar string?

Simple Harmonic Oscillation on a guitar string refers to the back and forth motion of a guitar string when it is plucked, resulting in a regular vibration and the production of sound.

2. What factors influence the Simple Harmonic Oscillation on a guitar string?

The factors that influence Simple Harmonic Oscillation on a guitar string include the tension of the string, the length of the string, and the mass of the string.

3. How does the frequency of the Simple Harmonic Oscillation affect the pitch of the sound produced?

The frequency of the Simple Harmonic Oscillation is directly proportional to the pitch of the sound produced. This means that a higher frequency results in a higher pitch, while a lower frequency results in a lower pitch.

4. Can the Simple Harmonic Oscillation on a guitar string be changed?

Yes, the Simple Harmonic Oscillation on a guitar string can be changed by altering the factors that influence it. For example, adjusting the tension or length of the string can change the frequency and therefore the pitch of the sound produced.

5. What is the relationship between the Simple Harmonic Oscillation and the harmonics of a guitar string?

The Simple Harmonic Oscillation is the basis for the production of harmonics on a guitar string. When a string is plucked, it produces the fundamental frequency, but it also simultaneously produces harmonics at integer multiples of the fundamental frequency.

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