Calculating Centripetal Acceleration in a Vertical Loop

In summary: At the instant at which the block has just left the loop the block is in free fall and undergoes projectile motion.
  • #1
Fitz Watson
7
0
Homework Statement
A small particle slides from height H=45 cm as shown and
then loops inside the vertical loop of radius R from where a
section of angle = 60° has been removed. If R = (1/N)
meter, such that after losing contact at A and flying through
the air, the particle will reach at the topmost point B. Find
N. Neglect friction everywhere.
Relevant Equations
$$mg(h) = mg(h') + \frac{1}{2}mv^2$$

$$mg = \frac{mv^2}{r}$$
IMG_20190327_192255.jpg
$$mg(0.45) = mg(R + R \cdot cos(\frac{π}{3})) + \frac{1}{2}mv^2$$

$$v^2 = g(0.9 - 3R)$$

The centripetal acceleration during the "flying through air" will be given by gravity

$$mg \cdot cos(\frac{\pi}{3}) = \frac{mv^2}{r}$$

$$R = \frac{1.8}{5}$$

But my book says $$ R = \frac{1}{5}$$
 
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  • #2
Your equation

$$mg=\frac{mv^2}{r}$$​

is incorrect. The weight and the centripetal force do not point in the same direction. You have to consider components if this equation is meant to express Newton's 2nd law. Also, there is a normal force acting on the mass just before the particle reaches the gap.
 
  • #3
kuruman said:
Your equation $$mg=\frac{mv^2}{r}$$is incorrect. The weight and the centripetal force do not point in the same direction. You have to consider components if this equation is meant to be Newton's 2nd law. Also, there is a normal force acting on the mass just before the particle reaches the gap.
I've used $$mg \cdot cos\frac{\pi}{3} $$ in the solution. As for the normal force, it's not present because I've considered the instant at which the block has just left the loop
 
  • #4
Fitz Watson said:
I've used $$mg \cdot cos\frac{\pi}{3} $$ in the solution. As for the normal force, it's not present because I've considered the instant at which the block has just left the loop
At the instant at which the block has just left the loop the block is in free fall and undergoes projectile motion.

On edit: The answer in the book that you quoted is correct if the units are meters. Treat the problem as projectile motion as soon as the particle loses contact with the track.
 
Last edited:
  • #5
Fitz Watson said:
The centripetal acceleration during the "flying through air" will be given by gravity
Not sure what your thinking is behind that statement.
It will fly through the air in a parabola, not a circle.
Of course, centripetal acceleration doesn't only apply to circular motion. In general, it is just the acceleration component at right angles to the velocity. But once it loses contact with the loop that will cease to point to the centre of the loop.
 

What is the definition of "Motion in a vertical loop"?

Motion in a vertical loop refers to the movement of an object in a circular path while being pulled downward by gravity. This type of motion is commonly seen in roller coasters or other amusement park rides.

What is the centripetal force in a vertical loop?

The centripetal force in a vertical loop is the force that is directed towards the center of the circular path. In the case of motion in a vertical loop, this force is provided by gravity.

What factors affect the speed of an object in a vertical loop?

The speed of an object in a vertical loop is affected by the radius of the loop, the mass of the object, and the force of gravity. A larger radius, smaller mass, and stronger gravity will result in a higher speed.

Can an object fall off a vertical loop?

No, as long as the object maintains enough speed and the radius of the loop is not too small, it will not fall off the loop. This is due to the centripetal force constantly pulling the object towards the center of the loop.

How does the acceleration change in a vertical loop?

The acceleration in a vertical loop changes as the object moves through different points in the loop. At the top of the loop, the acceleration is equal to the force of gravity, while at the bottom of the loop, the acceleration is equal to the force of gravity plus the centripetal force.

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