Conservation of Mechanical Energy Problem

In summary, a 2.00-kg ball attached to a fishline with a breaking strength of 44.5 N is released from rest with the line taut and horizontal. The question is, at what angle will the fishline break? The potential energy of the ball-earth system is maximum at the initial position, which is at rest, and changes only when the ball is set into motion. The velocity of the ball can be used to find the centripetal acceleration and ultimately determine the angle using Newton's Second Law. The length of the string after the ball is released is not a factor as the centripetal acceleration is independent of the string's length due to energy conservation.
  • #1
Moszzad
8
0
A 2.00-kg ball is attached to the bottom end of a length of fishline with a breaking strength of (44.5 N) The top end of line is held stationary. The ball is released from rest with the line taut and horizontal (theta=90.0). At what angle theta(measured from the vertical) will the fishline break.



I think I have a good idea about this problem, yet I wanted to get someone elses opinion. Taking into account that the potential energy of the ball-earth system is a maximum at the initial position which happens to be at rest. The potential energy changes only when the ball is set into motion which the energy is being transferred to kinetic. If I find the velocity of the ball then I could use this for centripetal acceleration to find the theta in Newton's Second Law. What's throwing me off is determining the length of the string at some point after the ball is released.
 
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  • #2
Consider the string to be, as usual, inextensible, with some length L.
Since the square of the speed is proportional to L (through energy conservation), the centripetal acceleration will be independent of L.
 
  • #3


Your understanding of the problem is correct. Conservation of mechanical energy can be applied to this problem since the initial potential energy of the system is equal to the final kinetic energy at any point during the motion. As the ball is released from rest, the initial potential energy is zero. The final kinetic energy can be calculated using the formula KE = 1/2 * mv^2, where m is the mass of the ball and v is the velocity at any given point.

To find the velocity at a specific point, we can use the equation for centripetal acceleration, a = v^2/r, where a is the acceleration, v is the velocity, and r is the radius of the circular motion. In this case, the radius is the length of the fishline, which remains constant throughout the motion.

Since the maximum breaking strength of the fishline is 44.5 N, we can equate this to the centripetal force acting on the ball, which is equal to the tension in the string. This gives us the equation T = mv^2/r. Solving for v, we get v = √(Tr/m), where T is the breaking strength, r is the length of the string, and m is the mass of the ball.

Now, we can use the value of v to calculate the angle theta using Newton's Second Law, which states that the net force acting on an object is equal to its mass times its acceleration. In this case, the net force is the tension in the string, which is acting tangentially to the circular motion. This gives us the equation T = ma, where a is the centripetal acceleration. Solving for theta, we get theta = sin^-1 (a/g), where g is the acceleration due to gravity.

In summary, to find the angle at which the fishline will break, we need to calculate the velocity of the ball using the maximum breaking strength of the string, and then use this velocity to calculate the centripetal acceleration and the angle theta using Newton's Second Law. I hope this helps!
 

What is the principle of conservation of mechanical energy?

The principle of conservation of mechanical energy states that the total amount of mechanical energy in a closed system remains constant over time, regardless of any internal changes or external forces acting on the system. This means that the sum of potential energy and kinetic energy in a system is always constant.

How is the conservation of mechanical energy applied in real-life situations?

The conservation of mechanical energy can be seen in many everyday situations, such as a pendulum swinging back and forth, a rollercoaster moving along its track, or a ball rolling down a hill. In each of these cases, the total mechanical energy of the system remains constant, even as the potential and kinetic energies may change.

What factors can affect the conservation of mechanical energy?

The conservation of mechanical energy is affected by the presence of external forces, such as friction, air resistance, or collisions, which can convert some of the mechanical energy into other forms, such as heat or sound. In addition, any changes in the potential or kinetic energy within the system can also affect the conservation of mechanical energy.

How is the conservation of mechanical energy related to the law of conservation of energy?

The law of conservation of energy states that energy cannot be created or destroyed, only transferred or converted from one form to another. The conservation of mechanical energy is a specific application of this law, focusing on the conservation of mechanical energy within a closed system.

What is an example of a problem involving the conservation of mechanical energy?

An example of a problem involving the conservation of mechanical energy is a ball rolling down a ramp. The ball starts with a certain amount of potential energy at the top of the ramp, which is converted into kinetic energy as it rolls down. The total mechanical energy of the ball remains constant throughout its motion, even as the potential and kinetic energies may change.

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