A force of 400 Newtons stretches a spring 2 meters. A mass of 50 kilograms is attached to the end of the spring and is initially released from the equilibrium position with an upward velocity of 10 m/s. After finding the equation of motion, calculate x(t =pi/12). Round in the tenths place.
"After finding the equation of motion" what are you currently learning?! you can jump in with \(x(t) = A \cos (\omega t + \phi)\) as the general solution to shm and fit it to these facts or you can build a differential equation from forces or energy conservation...
We are learning how to solve in-homogeneous and homogeneous 2nd order linear differential equations. However the class I'm taking an engineering course but it is essentially half differential equations and half multi-variable calculus.
soz, that doesn't really tell me what you want to do. do you have the DE that you want to solve? if not, do you need to find it? to illustrate: as it starts at equilibrium position (ie x=0 at t = 0), you could just say that \(x(t) = A \sin \omega t\) as that ticks all the shm boxes. so \(\dot x(t) = \omega A \cos \omega t\) ; and as it is "released from the equilibrium position with an upward velocity of 10 m/s", we know \(\dot x (0) \) also we know/ should know that \(\omega = \sqrt{\dfrac{k}{m}}\); and we get k from the info that "400 Newtons stretches a spring 2 meters" or we can start with \(m \ddot x + kx = 0\) and solve from there i hope that helps....:p
the DE that needs to be solved is \[x(t)=C _{1}\cos(\omega \times t)+ C _{2}\sin (\omega \times t)\]
ok \(x(t)=C _{1}\cos(\omega t)+ C _{2}\sin (\omega t)\) \(\dot x(t)=-\omega C _{1}\sin(\omega t)+ \omega C _{2}\cos (\omega t)\) and you know that: \(x(0) = 0, \qquad \dot x(0) = -10\) that still leaves us with the task of finding \(\omega\), though that has been covered above.
Where did I go wrong? If you can't read it let me know.
@IrishBoy123
how did you figure out k, the spring constant?
It gives you that m= 50 kg and the stretch is s=2m so (mg)/s= k (50)(9.8)/2=245
A force of 400 Newtons stretches a spring 2 meters.
take k from that :p
Do I need to convert the newtons to kg?
\(F = kx\) \(k = \dfrac{F}{x}\) and plug in the numbers
F in newtons, x in metres
so k=200 how do I get omega without a mass? Sorry to pester you so much.
we already saw that \(\omega = \sqrt{\dfrac{k}{m}}\) they gave you the mass in the question you're not pestering btw. this is interesting. i just hope that you are getting something from it :p
That makes sense because k is a constant you can m=50 instead of having to know how to convert from Newtons to kg.
I still got it wrong.
what do you make \(\omega\) out to be?
\[\omega=\sqrt{\frac{ 200 }{ 50 }}=\sqrt{4}=2\]
that looks good
my homework says I'm wrong
so... we have \(x(t)= A \sin 2t\) so \(\dot x(t)= 2A \cos 2t\) and from \(\dot x(0) = 10\), we can say \(2A \cos 0= 2A\)so \(A = 5\) so we have \(x(t)= 5 \sin 2t\) \(x(\frac{\pi}{12}) = 5 \sin \dfrac{\pi}{6}\)
which gives you x=2.5 that's what I put and it says it is incorrect.
you can also try x = -2.5 but this is the correct approach. i can think of several different approaches to the problem that will give the same result.
Yeah it was x=-2.5 I'm assuming it is because the velocity is negative and A is technically equal to \[\pm5\]
it's convention. i stated it as -10 here and then thought i was over complicating it |dw:1445039584590:dw|
Thank you for your help sorry it took so long but at least now I know how to do the problem.
it was good. thanks.
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