DiffyEQs - Undamped motion of spring

In summary, the goal is to find the angular frequency of a 1 kg mass attached to a spring with a constant k. First, find the equation for the motion in amplitude-phase form. Then use the inverse tangent to solve for c2. Finally, use c1 and v0 to solve for x(t).
  • #1
Pi Face
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Homework Statement


A 1 kg mass is attached to a spring with constant k = 16 N/m. Find the motion x(t) in amplitude-phase form (2.37) if x(0) = 1 and x′(0) = −1.
Ignore damping forces.


Homework Equations


combined with 3


The Attempt at a Solution


So I know m=1, k=16, c=0, x0=1, and v0=-1
w=sqrt(k/m)=sqrt(16)=4
md^2x/dt^2+kx=0
characteristic equation
mr^2+k=0
r=+/-iw=+/-4i
x(t)=c1*cos(4t)+c2*sin(4t) (e^0t = 1 and is excluded)
initially x0=1 so
1=c1
v=x'=-4c1sin(4t)+4c2cos(4t)
use intial value of -1 for v
-1=4c2cos(0)=4c2
c2=-1/4
A=sqrt(c1^2+c2^2)=sqrt(17)/4
tan(phi)=c2/c1=-.245, add pi =2.90
so now we have
x(t)=Acos(wt-phi)=sqrt(17)/2*cos(4t-2.90)

the book says the answer should be sqrt(17)/16*cos(4t-6.038)
so I all have right is the angular frequency
where did I mess up?
 
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  • #2
Hi Pi Face

Pi Face said:
initially x0=1 so
1=c1
c2=-1/4

tan(phi)=c2/c1=-.245, add pi =2.90

Tangent pi= -1/4 which is not -0.245.

Find the inverse tangent before adding pi or 2pi.

Look in the unit circle in which quadrant the angle is when the sine is negative, the cosine is positive.

ehild
 
  • #3
Woops, sorry I missed a step, but the answer is still the same.
tan phi=c2/c1
phi=tan-1(c2/c1)=-.245
 
  • #4
OK, phi = -0.245±k(2pi). If the book says 6.038 as the phase constant it should be positive (-0.245+2pi.). The standard amplitude-phase form is Acos(wt+phi).

ehild
 
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  • #5
ah i see.

but what about the amplitude?

A=sqrt(c1^2+c2^2)=sqrt(17)/4, not sqrt(17)/16 right? could it be a typo? maybe its sqrt(17/16)?
 
  • #6
Pi Face said:
ah i see.

but what about the amplitude?

A=sqrt(c1^2+c2^2)=sqrt(17)/4, not sqrt(17)/16 right? could it be a typo? maybe its sqrt(17/16)?

You are right, it is sqrt(17/16)=sqrt(17)/4. I did not notice.

Never trust in the solutions of books...

ehild
 
  • #7
Just one more question, and thank you for your help so far:

I still don't understand exactly when to add pi/2pi to the phase angle. I know we want the phase angle to be between 0 and 2pi. Why did I have to add 2pi in this example and not just pi? Wouldn't have adding pi still led to a value within the 0-2pi range?

On the quiz I had today, I ended up with something like tan^-1 (-1)=-pi/4. by plugging in -pi/4 for phi in sinphi and cosphi, I know that it is in the 4th quadrant. From here, I wasn't sure whether to add pi or 2pi, both would've resulted in values within the desired range. So between 3pi/4 and 7pi/4, I guessed 7pi/4. I know I got a 95 on the quiz so maybe it was 3pi/4 and I added one pi too many...but how do you know how much to add?
Thanks.
 
  • #8
If you know both the sine and a cosine of an angle you exactly know in which quadrant it is. You give the angle+2pik as the whole solution.

When the x,y components (ax=Acos(θ), ay =Asin(θ)) of a vector are given you can decide in which quadrant the angle is from the sign of the components. Draw the unit circle. (I always draw it in case of similar problems.) First quadrant (0,pi/2): both components positive. Second quadrant (pi/2, pi): ax<0, ay>0. Third quadrant(pi,3pi/2): both components negative. Fourth quadrant (3pi/2, 2pi): ax>0, ay<0. You need to add either 0, pi or 2pi to make the angle positive and place it into the appropriate quadrant.

Example: A=5, ax=5cosθ, ay=5sinθ.

ax=4, ay=3: tan(θ)=0.75, arctan(0.75)=0.6435, first quadrant, θ=0.6435

ax=-4, ay=3. tan(θ)=-0.75, the angle is in the second quadrant. arctan(-0.75)=-0.6435, we need to add pi: θ=-0.6435+pi=2.498.

ax=-4, ay=-3. The angle is in the third quadrant: tan(θ)=0.75,arctan(0.75)=0.6435, we add pi to place the angle into the third quadrant: θ=0.6435+pi=3.785.

ax=4, ay=-3: fourth quadrant. tan(θ)=-0.75, arctan(-0.75)=-0.6435, we need to add 2pi to get a positive angle in the fourth quadrant. θ=-0.6435+2pi=5.6397.

ehild
 
  • #9
Thanks for your help.

Also I did get the phase angle right on the quiz, but on one of the problems on the last few steps solving for c2, I accidentally wrote down c2 as c1. Oh well, at least I know how to do them now.
 
  • #10
Silly mistakes are the worst... but they occur at everybody. Always check your test.

ehild
 

FAQ: DiffyEQs - Undamped motion of spring

1. What is an undamped motion of a spring?

An undamped motion of a spring refers to the movement of a spring without any external forces or friction acting upon it. This means that the spring will continue to oscillate back and forth at a constant amplitude and frequency.

2. How is the undamped motion of a spring described mathematically?

The undamped motion of a spring can be described using a differential equation called the "simple harmonic oscillator" equation. It is represented as mx'' + kx = 0, where m is the mass of the object attached to the spring, x'' is the second derivative of the displacement, and k is the spring constant.

3. What factors affect the undamped motion of a spring?

The undamped motion of a spring can be affected by the mass attached to the spring, the spring constant, and the initial displacement or velocity of the spring. These factors can change the frequency and amplitude of the oscillations.

4. How is the solution to the undamped motion of a spring obtained?

The solution to the undamped motion of a spring can be obtained by solving the differential equation using mathematical methods such as the method of undetermined coefficients or Laplace transforms. The solution will be in the form of a sinusoidal function.

5. What is the significance of the undamped motion of a spring in real-world applications?

The undamped motion of a spring has many practical applications, such as in the design of mechanical systems and structures, as well as in understanding the behavior of pendulums and other oscillating systems. It is also important in studying the properties of sound waves and electromagnetic waves.

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