Particle going in a circle with speed U problem

In summary: Finally, to solve for the coordinates at time t=0, use the equation x(0)=-Rcos(\theta), y(0)=-Rsin(\theta).
  • #1
hamilbr
3
0

Homework Statement


Hello all,
I am having some trouble with answering the problem below, mostly because I do not know what the letters stand for and what kind of graph is meant to be drawn. Any help on this would be greatly appreciated. Thanks

For a particle going in a circle with speed U, draw a graph showing:
x(t)
y(t)
u(t)=dx/dt
v(t)=dy/dt
du/dt
dv/dt


Homework Equations





The Attempt at a Solution


 

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  • #2
In your diagram you've indicated x and y axes. x(t) will be the x position with respect to time, y(t) the y position with respect to time. So to begin, draw two more graphs with t as the horizontal axis and place x on the vertical axis of one and y on the vertical axis of the other.

Clearly u(t) and v(t) are meant to be the x-velocity and y-velocity. du/dt is the derivative of y-velocity with respect to time (what do we usually call the derivative of a velocity?). You'll want to draw similar graphs for these items.
 
  • #3
Are you serious? You don't know what the letters stand for? That should have been the first thing you learned! x and y are the coordinates of that particle in some coordinate system. u and v, as is said in the problem are the derivatives (do you know what a derivative is?) of x and y and so are the x and y components of the velocity vector. du/dt and dv/dt are the x and y components of acceleration.

It helps to know that a circle, with center at (0, 0) and radius R has equation [itex]x^2+ y^2= R^2[/itex]. And, of course, [itex]sin^2(x)+ cos^2(x)= 1[/itex]. That means that parametric equations for the circle are [itex]x= Rcos(\theta)[/itex], [itex]y= R sin(\theta)[/itex]. Now, the circumference of the circle is [itex]2\pi R[/itex] and if the particle is moving at constant speed U, it will complete the circle (moving through an angle of [itex]2\pi[/itex] radians) in time [itex]\frac{2\pi R}{U}[/itex] so has angular speed [itex]\frac{U}{R}[/itex]. That means the angle, at time t, is [itex]\theta= \frac{U}{R}t[/itex].
 

FAQ: Particle going in a circle with speed U problem

What is the formula for calculating the centripetal force on a particle going in a circle with speed U?

The formula for calculating the centripetal force on a particle going in a circle with speed U is F = m * v^2 / r, where m is the mass of the particle, v is the speed, and r is the radius of the circle.

How does the speed of the particle affect the magnitude of the centripetal force?

The speed of the particle has a direct relationship with the magnitude of the centripetal force. As the speed increases, the centripetal force also increases. This means that a faster-moving particle will require a greater force to keep it moving in a circular path.

What is the direction of the centripetal force on a particle going in a circle?

The direction of the centripetal force is always towards the center of the circle. This is because the force is responsible for keeping the particle moving in a circular path, and any deviation from this path would require a force towards the center to correct it.

Can the centripetal force change the speed of the particle going in a circle?

No, the centripetal force does not change the speed of the particle. Its only function is to change the direction of the particle's velocity, keeping it moving in a circular path. The speed of the particle remains constant unless acted upon by an external force.

What are the real-world applications of the particle going in a circle with speed U problem?

The particle going in a circle with speed U is a common problem in physics and has many real-world applications. Examples include the motion of planets around the sun, the motion of electrons in an atom, and the motion of a car around a curve. Understanding this problem allows us to predict and control the motion of objects in circular paths.

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