Conservation of Mechanical Energy Problem

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SUMMARY

The discussion focuses on determining the angle theta at which a 2.00-kg ball, attached to a fishline with a breaking strength of 44.5 N, will break when released from rest. The conservation of mechanical energy principle is applied, equating the initial potential energy to the final kinetic energy. The velocity of the ball is derived using the centripetal force equation T = mv²/r, leading to the calculation of theta using Newton's Second Law with the formula theta = sin⁻¹(a/g). This method provides a clear pathway to solving the problem definitively.

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Moszzad
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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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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.
 


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!
 

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