Derivation of Work-Energy Theorem

In summary, the Work-Energy Theorem can be used to show that an object with initial velocity vo will travel a distance d on a rough horizontal surface before stopping, where d = vo2/(2muKg). The friction force can be calculated and the work done by this force will result in the object losing all its kinetic energy and coming to a stop.
  • #1
IncognitoSOS
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Homework Statement


Use the Work-Energy Theorem to show that an object with initial velocity vo will travel a distance d across a rough horizontal surface before stopping, where d = vo2/(2muKg).

Homework Equations


W = delta KE = mV^2/2


The Attempt at a Solution


To be honest, I have absolutely no idea where to even start. Any suggestions on how to start would be greatly appreciated.
 
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  • #2
Can you compute what the friction force is?

The work done by this force is force * distance (if the force is always in the same direction as the movement, but that is the case here)

The object will lose all the kinetic energy is has at the start while it slows to a stop.
 
  • #3


Dear student,

The Work-Energy Theorem is a fundamental principle in physics that relates the work done on an object to its change in kinetic energy. It states that the net work done on an object is equal to the change in its kinetic energy, or W = ΔKE. In other words, the work done on an object is responsible for changing its speed or direction of motion.

To apply this theorem to the given scenario, we can break down the problem into two parts: the work done on the object and the change in its kinetic energy. The work done on the object can be calculated by considering the forces acting on it. In this case, the only force acting on the object is the frictional force between the object and the rough horizontal surface. This force is given by the equation F = μkmg, where μk is the coefficient of kinetic friction, m is the mass of the object, and g is the acceleration due to gravity. The work done by this force can be calculated by multiplying it by the distance traveled, which in this case is d. Therefore, the work done on the object is W = μkmgd.

Next, we need to calculate the change in kinetic energy of the object. Initially, the object has a kinetic energy of KE = ½ mv0^2, where v0 is the initial velocity of the object. When the object comes to a stop, its kinetic energy becomes zero. Therefore, the change in kinetic energy is ΔKE = ½ mv0^2 - 0 = ½ mv0^2.

Now, we can apply the Work-Energy Theorem by equating the work done on the object to its change in kinetic energy. This gives us the equation μkmgd = ½ mv0^2. Solving for d, we get d = v0^2/(2μkmg). This is the distance traveled by the object before it comes to a stop on the rough horizontal surface.

In conclusion, the Work-Energy Theorem provides a useful tool for understanding the relationship between work and energy. By applying this theorem to the given scenario, we were able to derive the equation for the distance traveled by an object with initial velocity v0 before stopping on a rough horizontal surface. I hope this explanation helps you understand the concept better. Keep up the good work in your studies!
 

Related to Derivation of Work-Energy Theorem

1. What is the Work-Energy Theorem?

The Work-Energy Theorem is a fundamental principle in physics that states that the work done on an object is equal to the change in its kinetic energy. In other words, the net work done on an object is equal to the change in its speed or velocity.

2. How is the Work-Energy Theorem derived?

The Work-Energy Theorem is derived from the principle of conservation of energy, which states that energy cannot be created or destroyed, only transferred or transformed. By considering the different types of forces acting on an object and the work done by those forces, we can derive the relationship between work and kinetic energy.

3. What are the key equations used in the derivation of the Work-Energy Theorem?

The key equations used in the derivation of the Work-Energy Theorem include the definition of work as force multiplied by displacement, the definition of kinetic energy as one-half the mass multiplied by the square of the velocity, and Newton's second law of motion, which states that the net force acting on an object is equal to its mass multiplied by its acceleration.

4. What are some real-life applications of the Work-Energy Theorem?

The Work-Energy Theorem is used in various fields of physics and engineering, such as in the design of roller coasters, calculating the efficiency of machines, and understanding the motion of projectiles. It is also used in everyday situations, such as when pushing a shopping cart or throwing a ball.

5. Are there any limitations to the Work-Energy Theorem?

While the Work-Energy Theorem is a useful tool for understanding the relationship between work and kinetic energy, it does have some limitations. It assumes that there are no non-conservative forces, such as friction, acting on the object. It also only applies to objects with constant mass and velocity, and cannot be used for objects with changing mass or velocity.

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