Vibrations - Modeling system, equation of motion

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Discussion Overview

The discussion revolves around modeling a system involving vibrations and deriving the equation of motion for a setup with multiple masses and a spring. Participants express confusion regarding the influence of angles and the relationships between various parameters in the system, including the roles of angular displacement and restoring forces.

Discussion Character

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

Main Points Raised

  • One participant expresses uncertainty about how to model the system and the significance of the angle theta on the spring's displacement.
  • Another participant clarifies that the angle theta changes with the spring's contraction or expansion and that the masses are fixed on rods, forming a triangle that can rotate.
  • There is a discussion about the assumptions made, including negligible damping and the system being a one degree of freedom (DOF) system.
  • Participants explore the relationship between angular velocity and time, with one participant questioning the meaning of variables used in their equations.
  • Another participant emphasizes the importance of torque and angular acceleration in the context of oscillations, suggesting that the exercise requires translating linear motion concepts to angular terms.
  • There is a debate about the contributions of each mass to the torque about a pivot point, with some participants suggesting that the center of mass's position complicates the analysis.
  • One participant proposes that the exercise's author may have intended for certain torque contributions to be ignored, while others challenge this assumption.

Areas of Agreement / Disagreement

Participants do not reach a consensus on several points, including the treatment of torque contributions from each mass and the implications of the angle of l2. There are competing views on how to approach the problem and what assumptions are valid.

Contextual Notes

Participants note that the center of mass's position is not at the pivot point, which may affect the analysis of torques. There is also uncertainty regarding the correct interpretation of angular frequency and its relationship to natural frequency.

  • #31
haruspex said:
Figure 5? (But you can do better than trying to read the slope at time zero.)
Ok, I tried it a different way, can you tell me if this is right:

for SHM, θ(t) = θ^sin(ωnt) (where θ^ = amplitude).

⇒ θ'' = -ωn2θ

Itotalθ'' = -kθ

⇒Itotaln2θ = -kθ

⇒ωn = √k/Itotal

?
 
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  • #32
thepikminman said:
Ok, I tried it a different way, can you tell me if this is right:

for SHM, θ(t) = θ^sin(ωnt) (where θ^ = amplitude).

⇒ θ'' = -ωn2θ

Itotalθ'' = -kθ

⇒Itotaln2θ = -kθ

⇒ωn = √k/Itotal

?
Let's get the DE right first. Can you use my hints in post 26 to correct your sign error in post 23?
 
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  • #33
haruspex said:
##\theta## is positive anticlockwise, so its derivatives are too. Does a positive displacement increase or decrease the anticlockwise moment from m2 ? Does it increase or decrease the anticlockwise moment from the spring?

Once you have recognised a DE as SHM, the easiest way is to plug in a generic solution Acos(ωt+φ) and solve.

A positive (angular) displacement would increase the anticlockwise moment, and decrease the anticlockwise moment from the spring (but increase the spring force)

Ok so the DE should be: θ''In + 0θ' + (m2gl2 + kl3) θ= 0

But then from the -b formula, how can I get the sqaure root of 4*[m1l12 + m2l22 + m3l32]*(m2gl2 + kl3)? I've no idea
 
  • #34
thepikminman said:
A positive (angular) displacement would increase the anticlockwise moment, and decrease the anticlockwise moment from the spring
So why do you have the same sign for each in the equation?
thepikminman said:
how can I get the sqaure root of 4*[m1l12 + m2l22 + m3l32]*(m2gl2 + kl3)?
Just deduce ω from the graph.
 
  • #35
haruspex said:
So why do you have the same sign for each in the equation?

Just deduce ω from the graph.
Haha I had the minus in my first answer and you said it was wrong ? That's why I'm confused

And for deducing ω from the graph, I see that θ = 0.02 at ωt=0, but how do i get ω from that?
 
  • #36
thepikminman said:
Haha I had the minus in my first answer and you said it was wrong ? That's why I'm confused
There are two terms in the factor for θ. Originally you had both negative, which will not give SHM. The overall value must be positive (ω2). Now you have both positive, yet you stated, correctly, that one increases while the other decreases.
thepikminman said:
And for deducing ω from the graph, I see that θ = 0.02 at ωt=0, but how do i get ω from that?
What's the period?
 
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  • #37
haruspex said:
There are two terms in the factor for θ. Originally you had both negative, which will not give SHM. The overall value must be positive (ω2). Now you have both positive, yet you stated, correctly, that one increases while the other decreases.

What's the period?

Okay, I get it now, thank you for your patience! So it's: θ''In + 0θ' + (m2gl2 - kl3) θ= 0

As for the period...I know it's = 1/f = 2π/ω, but I don't know what f is. The period seems to be 6 from the graph but that's just by looking, so is it 1/6?
 
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  • #38
thepikminman said:
how can I get the sqaure root of 4*[m1l12 + m2l22 + m3l32]*(m2gl2 + kl3)?
I just noticed that all the constants are given in Table 2 at the top of page 4, so you can calculate this.
thepikminman said:
θ''In + 0θ' + (m2gl2 - kl3) θ= 0
You wrote, correctly, that as θ increases the effect of the spring (kl3θ) is to reduce ##\ddot\theta##. So what sign should the kl3θ term have? You might find it easier to answer if you rearrange the equation as ##\ddot θ##In = (+ or -?)m2gl2θ + (+ or -?)kl3 θ.
 
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  • #39
haruspex said:
I just noticed that all the constants are given in Table 2 at the top of page 4, so you can calculate this.

You wrote, correctly, that as θ increases the effect of the spring (kl3θ) is to reduce ##\ddot\theta##. So what sign should the kl3θ term have? You might find it easier to answer if you rearrange the equation as ##\ddot θ##In = (+ or -?)m2gl2θ + (+ or -?.
Ah yes, the table, that makes sense!

So it would be θ''In = (+m2gl2 - kl3 )θ...right?
 
  • #40
thepikminman said:
Ah yes, the table, that makes sense!

So it would be θ''In = (+m2gl2 - kl3 )θ...right?
Yes.
 
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  • #41
haruspex said:
Yes.
Okay, so that gives me the correct DE, now is finding the roots of the characteristic equation the next step? (with b=0)
 
  • #42
thepikminman said:
Okay, so that gives me the correct DE, now is finding the roots of the characteristic equation the next step? (with b=0)
As I posted, it is easier to work from the generic equation ##\theta=A\cos(\omega t+\phi)##. You can calculate ω from the coefficient in the differential equation ##(\ddot \theta+\omega^2\theta=0)##, and read off the amplitude and φ from the graph.
 
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  • #43
haruspex said:
As I posted, it is easier to work from the generic equation ##\theta=A\cos(\omega t+\phi)##. You can calculate ω from the coefficient in the differential equation ##(\ddot \theta+\omega^2\theta=0)##, and read off the amplitude and φ from the graph.
Is the coefficient of the θ variable always = ω2?

If so, can't I just get ω2 = √27.513 (the coefficient in front of θ) = 5.245?

Is that the natural frequency value?

How do I go about reading the amplitude and φ from the graph anyway? A seems to be about 3.9 (?) but how do I read φ ? The sin wave seems to be shifted 5.5 rad to the right so is θ = 3.9sin(ω(0)-5.5)? (⇒ θ = 2.75 rad?
 
  • #44
thepikminman said:
Is the coefficient of the θ variable always = ω2?
Yes. Plug θ=A cos(ωt+φ) into ##\ddot \theta+\omega^2\theta## and see what happens.
thepikminman said:
27.513
If that is = (+m2gl2 - kl3 )/In, yes.
 
  • #45
thepikminman said:
How do I go about reading the amplitude and φ from the graph
You could measure with a ruler, but by eye I would put the amplitude about 0.037 or 0.038.
For the phase, the first peak is at about ωt=0.8 or 0.9 radians. What value of φ would result in that?
 
  • #46
haruspex said:
Yes. Plug θ=A cos(ωt+φ) into ##\ddot \theta+\omega^2\theta## and see what happens.

If that is = (+m2gl2 - kl3 )/In, yes.
Ah they cancel, that's cool! But does that only work for this particular example? With the θ' coefficient being = 0?

Basically, I'm asking if that's a way to calculate ω in every question, not just this one? Because most past exam questions ask for ωn, so if I find the equation of motion, then will ωn always be the coefficient of the "x" term (θ in this problem)?
 
  • #47
haruspex said:
You could measure with a ruler, but by eye I would put the amplitude about 0.037 or 0.038.
For the phase, the first peak is at about ωt=0.8 or 0.9 radians. What value of φ would result in that?
Would it be sin(θ-0.9), so ψ = 0.9?

On a different topic, I'm able to do most of the questions now, but I have just 2 last queries for you;

1. In Question 6(a) I derived the formula fine, but what are the units for ωn in terms of E,I,L and m? I did it as ωn = √(Gpa*mm4)/(mm3*kg) = √(Gpa*mm)/kg...does that results in the correct units for the natural frequency? If not, what does?

2.In Question 6(c) how does the factor of safety come into play here? The "hint" with λ in it actually made me think I have no idea how to answer this correctly because none of my lecture notes have that info on modes or λ(c). Any ideas on how to approach this?

Thanks so much to you and @BvU for all your help so far, you really helped me take the edge off this difficult subject.
 
  • #48
thepikminman said:
if that's a way to calculate ω in every question,
Yes, but don't forget the square root. If ##\ddot x + kx=0## then the angular frequency is ##\sqrt k##.
(If k is negative it is not SHM, since the system will accelerate away from the neutral position, like a pencil balanced on its point).
thepikminman said:
Would it be sin(θ-0.9), so ψ = 0.9?
Careful with signs. Substitute that in the equation with ωt=0.9 to check.
thepikminman said:
√(Gpa*mm)/kg...does that results in the correct units for the natural frequency?
It certainly produces the right dimension (1/time). Do you know dimensional analysis? But you need to check whether the units are s-1.
thepikminman said:
how does the factor of safety come into play here?
This gets beyond my competence. Knowing the natural frequency etc. and the applied frequency and power, there must be some formula that tells you the maximum stress. Look up forced oscillations.
thepikminman said:
The "hint" with λ in it
All this is saying is that the mode is the simplest possible: at any instant, the displacement at offset x is c(x)cos(ωt), where c(x) gives the shape of the beam under a static deflection.
 
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  • #49
haruspex said:
Careful with signs. Substitute that in the equation with ωt=0.9 to check.

Thank you!

So it the angular displacement, θ = Acos(ωt + Φ) = 0.037cos(0 + 0.9)?
 
  • #50
thepikminman said:
Thank you!

So it the angular displacement, θ = Acos(ωt + Φ) = 0.037cos(0 + 0.9)?
No, you misunderstand.
According to the graph, you need a peak at ωt=0.9. What value of Φ maximises Acos(0.9 + Φ)?
 
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  • #51
haruspex said:
No, you misunderstand.
According to the graph, you need a peak at ωt=0.9. What value of Φ maximises Acos(0.9 + Φ)?
Oh, is it for Φ=-0.9, because cos(0) is the maximum value you can get?
 
  • #52
thepikminman said:
Oh, is it for Φ=-0.9, because cos(0) is the maximum value you can get?
Yes.
 
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