Applying the work-energy theorem

In summary, the conversation discusses using the work-energy theorem to solve for the final velocity of a branch falling from a 95 m tall tree, neglecting air resistance. The equations used include the work-energy theorem, the equation for kinetic energy, and the equation for gravitational force. The final velocity can be solved for by assuming a mass and carrying through with the equations, with the hope that the mass will cancel out."
  • #1
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Homework Statement


Use the work-energy theorem to solve.
A branch falls from the top of a 95 m tall tree, starting from rest. How fast is it moving when it reaches the ground? Neglect air resistance.

Homework Equations


work-energy theorem:w_total=K_2-K_1
In this problem, K_1 is 0 since it is starting from rest.
K_2=(1/2)*m*v^2 (?)
w=fd (relevant?)

The Attempt at a Solution


If I use the equations I have above, I end up with w=1/2*m*v_f^2.
However, I am not given a mass. I do not know how to finish the calculation without a mass.
If I use w=fd, I have (9.8 m/s^2)(mass)*(95 m).
I am really stuck.
 
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  • #2
In addition to the equations you listed, you also need the equation for the force of gravity on a mass.

You are only asked for the final velocity. Assume a mass, and carry through with the equations. Hopefully the mass will cancel out when you solve for the velocity.
 
  • #3


I would like to clarify that the work-energy theorem states that the total work done on an object is equal to the change in its kinetic energy. In this problem, the work done on the branch is due to the force of gravity, and the change in its kinetic energy is equal to its final kinetic energy.

To solve this problem, we can use the equation for gravitational potential energy, U=mgh, where m is the mass of the branch, g is the acceleration due to gravity (9.8 m/s^2), and h is the height of the tree (95 m). Since the branch starts from rest, its initial kinetic energy is 0. Therefore, the total work done on the branch is equal to its change in potential energy, or W=U_f-U_i=mgh.

Since we do not know the mass of the branch, we cannot solve for the final velocity using the work-energy theorem. However, we can use the equation for velocity in terms of potential energy, v=sqrt(2gh), to find the final velocity. Assuming the branch falls straight down, the potential energy at the top of the tree (U_i) is equal to the kinetic energy at the bottom (K_f), so we can write the equation as mgh=1/2mv_f^2. Solving for v_f, we get v_f=sqrt(2gh).

Substituting the given values, we get v_f=sqrt(2(9.8 m/s^2)(95 m))=43.06 m/s.

Therefore, the branch will be moving at a speed of 43.06 m/s when it reaches the ground. It is important to note that this calculation neglects the effects of air resistance, which would likely decrease the final velocity of the branch.
 

FAQ: Applying the work-energy theorem

What is the work-energy theorem?

The work-energy theorem states that the work done on an object by a net force is equal to the change in kinetic energy of the object. In other words, when a net force acts on an object, it causes a change in the object's speed or direction of motion, resulting in a change in its kinetic energy.

How is the work-energy theorem applied?

The work-energy theorem can be applied in various situations involving the motion of objects, such as a ball rolling down a hill or a car accelerating on a flat road. To apply the theorem, you need to identify the net force acting on the object and calculate the work done by that force. Then, you can use the equation W = ΔKE to determine the change in kinetic energy of the object.

What is the relationship between work and energy in the work-energy theorem?

The work-energy theorem establishes a direct relationship between work and energy. It states that the work done on an object (W) is equal to the change in kinetic energy (ΔKE) of the object. This means that when work is done on an object, it results in a change in the object's energy.

Can the work-energy theorem be applied to all types of forces?

Yes, the work-energy theorem can be applied to all types of forces as long as they result in a change in the object's kinetic energy. This includes both conservative forces, such as gravity, and non-conservative forces, such as friction. The work done by these forces can be calculated and used to determine the change in kinetic energy of the object.

How is the work-energy theorem related to the law of conservation of energy?

The work-energy theorem is closely related to the law of conservation of energy. According to the law of conservation of energy, energy cannot be created or destroyed, only transferred or converted from one form to another. The work done on an object results in a change in its kinetic energy, demonstrating the conversion of energy from one form to another, while the total amount of energy remains constant.

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