A particle, initially at rest, moves along the x-axis such that its acceleration at time t>0 is given by a(t)=cos(t). At the time t=0, its position is x=3. A) Find the velocity and position functions for the particle. B) Find the values of t for which the particle is at rest.
We will start with velocity.
Alright :D
\[ v(t)-v(0) = \int_0^t\cos(t)~dt \]
They have already given us that \(v(0) = 0\), so that simplifies things for us.
Oh so "initially at rest" means velocity right
Yes
Can you integrate?
Uhm That would mean that the acceleration would be sin(t) + C
No, there is no constant of integration here, because it isn't an indefinite integral.
We used a definite integral, so any constant of integration was canceled out through subtraction.
I don't think I've learned definite/indefinite yet
Definite integrals are ones where we have limits of integration. In this case our limits were \(0\) to \(t\). Indefinite ones don't have limits of integration.
Actually I think I've only learned indefinite
Oh
Technically, I should have written:\[ v(t)-v(0) = \int_0^t\cos(x)~dx \]Or something, because your variable of integration can't be a limit of integration as well, but is isn't a bit issue.
Anyway, we should get: \[ v(t)-v(0) = \sin(t)\\ v(t)-0 = \sin(t)\\ v(t) = \sin(t) \]
That is our velocity. The next thing to find is our position.\[ x(t)-x(0) = \int_0^t \sin(u)~du \]
So I'm on the first chapter of integration, so I'm not very familiar with the vocab. but why don't we include C into the answer.
Did you learn the fundamental theorem of calculus?
I don't think so
Okay, suppose you have a function \(f(x)\) with a derivative \(f'(x)\).
One of the things the fundamental theorem of calculus says is that: \[ \int_a^bf'(t)~dt = f(b)-f(a) \]
I also haven't learned the little notation on the ends of the integral sign either :c
So you really haven't learned definite integrals?
Nope, only indefinite
Okay...
Okay, let's just suppose then that: \[ v(t) = \sin(t) + C \]
Yeah
In that case we need to solve for \(C\) by using \(v(0)=0\).
C=0
So that would make v(t) = sin(t)
and the position function is x(t)= -cos(t)
How did you get that?
The integral of the Velocity function would be Position right
But how did you find \(C\)?
well you said that v(0) = 0 so i plugged it into the V(t) = sint +c 0=sin(0) +C C=0
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