Force Vectors and Circular Motion

In summary, the conversation discusses the concept of forces in circular motion on a ferris wheel. It touches on the idea of balancing forces and the role of gravity, centripetal force, and normal force. The answer given involves subtracting Fc from Fg to determine Fn, which is in conflict with the speaker's understanding of the vectors involved.
  • #1
Ronnin
168
1
This is a case where I know the results but am fighting the math. At the top of a ferris wheel your acceleration in Y is 0. Ol' Newton says all all forces then must cancel, got that. I know my weight at this point will feel less at this point. Here is where I am troubled, vector for gravity points down so does the vector for the circle's accleration but my Normal points up and must have the same magnitude as Fg and Fc. The answer given subtracts Fc from Fg to get Fn (which feels right, but contradicts my vectors). Any conceptual help is appreciated.
 
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  • #2
Your acceleration at the top of a ferris wheel is NOT zero. Assuming you are undergoing perfect circular motion, you will have a centripetal force at the top. Gravity will supply the centripetal force, but all of the weight will be too much centripetal force, so therefore the normal force will balance some of the weight.

In perfect circular motion, the only unbalancd force will be centripetal and equal (mv^2)/r . At the top of the ferris wheel the unbalanced force is equal to mg-N.
 
  • #3


First of all, it is completely normal to struggle with the math behind force vectors and circular motion. These concepts can be complex and require a solid understanding of physics principles. However, with practice and a deep understanding of the underlying concepts, you will be able to confidently solve these types of problems.

Now, let's address the specific issue you are having. At the top of the ferris wheel, your acceleration in the y-direction is indeed 0. This means that the net force in the y-direction must also be 0, as stated by Newton's second law (ΣF=ma). This does not necessarily mean that all forces must cancel out, but rather that the sum of all forces in the y-direction must equal 0.

In this case, the forces acting on you are your weight (Fg), the normal force (Fn), and the centrifugal force (Fc). The normal force is the force exerted by the seat of the ferris wheel on your body, perpendicular to the surface of the seat. This force is what allows you to feel the seat supporting you and prevents you from falling out of the ride.

Now, let's consider the vectors for these forces. Fg and Fc both point downwards, while Fn points upwards. This may seem like a contradiction, but remember that vectors represent both magnitude and direction. The magnitude of Fg and Fc are equal, but their directions are opposite. The magnitude of Fn must also be equal to Fg and Fc, but its direction is opposite to both of them.

When you subtract Fc from Fg, you are essentially taking into account the opposite directions of these forces. This results in a net force of 0, as required by Newton's second law. So, while it may seem counterintuitive that the normal force is equal to the difference between Fg and Fc, it is a result of taking into account the direction of these forces.

I hope this explanation helps clarify your understanding of force vectors and circular motion. Remember to always consider the direction and magnitude of forces when solving these types of problems. With practice and a solid understanding of the underlying principles, you will be able to confidently solve any physics problem.
 

FAQ: Force Vectors and Circular Motion

What is a force vector?

A force vector is a representation of a force in terms of its magnitude and direction. It is typically represented graphically as an arrow, with the length of the arrow representing the magnitude and the direction of the arrow representing the direction of the force.

How are force vectors used in circular motion?

In circular motion, force vectors are used to represent the forces acting on an object that is moving in a circular path. These forces can include centripetal force, which acts towards the center of the circle, and tangential force, which acts tangentially to the circle.

What is centripetal force?

Centripetal force is the force that keeps an object moving in a circular path. It acts towards the center of the circle and is necessary for an object to maintain its circular motion. Without centripetal force, an object would continue in a straight line instead of following a circular path.

How is centripetal force calculated?

Centripetal force can be calculated using the formula Fc = mv^2/r, where Fc is the centripetal force, m is the mass of the object, v is the velocity of the object, and r is the radius of the circular path. This formula is derived from Newton's second law of motion, which states that force is equal to mass times acceleration.

What are some real-life examples of circular motion?

Some examples of circular motion in everyday life include the rotation of the Earth around the Sun, the motion of a Ferris wheel, and the movement of a satellite in orbit around a planet. Other examples include the circular motion of a car going around a roundabout or a person swinging on a swing.

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