What is the derivation of the centripetal acceleration in terms of position?

In summary, the conversation discusses a problem that has been previously discussed but one part was not included. The problem involves calculating the acceleration of a particle in terms of its position. The given position equation is r(t) = Rcos(wt) * i + Rsin(wt) * j and the homework equations are v = wR, a = v^2/R, and a = wv. The attempted solution involves using the derivative of the position equation and the correct solution is -w^2r(t) in vector form. The conversation also mentions that the correct answer does not depend on certain variables and functions.
  • #1
unknown_2
29
0
This problem has been discussed before, but one of the parts were not discussed.

Homework Statement


Your calculation is actually a derivation of the centripetal acceleration. To see this, express the acceleration of the particle in terms of its position r(t).

r(t) = [tex]Rcos(\omega t)\textbf{i} + Rsin(\omega t)\textbf{j}[/tex]

Homework Equations



[tex]v = \omega R [/tex]
[tex]a = \frac{v^2}{R} [/tex]
[tex]a = \omega v [/tex]

The Attempt at a Solution



[tex]v = \frac{d}{dt}r(t) \times \omega[/tex]

btw, this is a Mastering engineering question, so i submitted and it says that:
The correct answer does not depend on the variables and functions: d, d, r.

is there another way to display this or am i missing something?

thx,
 
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  • #2
Acceleration = V^2/R = w^2*R. In a uniform circular motion w and R are constant.
 
  • #3
rl.bhat said:
Acceleration = V^2/R = w^2*R. In a uniform circular motion w and R are constant.

omg...too stressed out about finals...i think i got it =_=

please correct me if I'm wrong (again)...

a(t) = [tex] -\omega^{2}r(t)[/tex]
 
  • #4
unknown_2 said:
omg...too stressed out about finals...i think i got it =_=

please correct me if I'm wrong (again)...

a(t) = [tex] -\omega^{2}r(t)[/tex]

If you express in the vector form, it is correct.
 

FAQ: What is the derivation of the centripetal acceleration in terms of position?

What is uniform circular motion?

Uniform circular motion is a type of motion where an object moves in a circular path at a constant speed. This means that the object's velocity is always tangent to the circular path and its magnitude remains constant throughout the motion.

What causes uniform circular motion?

In order for an object to experience uniform circular motion, there must be a centripetal force acting on it. This force is directed towards the center of the circular path and is necessary to keep the object moving in a circular path at a constant speed.

What is the difference between uniform circular motion and non-uniform circular motion?

In uniform circular motion, the speed of the object remains constant while its direction changes continuously. In non-uniform circular motion, the speed of the object may change, either increasing or decreasing, while its direction changes continuously.

How is the centripetal force related to uniform circular motion?

The centripetal force is the force that causes an object to move in a circular path. In uniform circular motion, the centripetal force is always perpendicular to the object's velocity and directed towards the center of the circular path.

What are some real-life examples of uniform circular motion?

Some common examples of uniform circular motion include a car driving around a curved road, a satellite orbiting around the Earth, and a merry-go-round spinning at a constant speed. Any object moving in a circular path at a constant speed can be considered as an example of uniform circular motion.

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