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W_{net} = ΔKE = KE_f - KE_i

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College Physics I – Introduction

Definition

The net work done on an object is equal to the change in its kinetic energy, which is the difference between its final kinetic energy (KE_f) and its initial kinetic energy (KE_i). This relationship is known as the work-energy theorem and is a fundamental principle in classical mechanics.

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5 Must Know Facts For Your Next Test

  1. The net work done on an object is the sum of all the work done on the object by various forces, both conservative and non-conservative.
  2. The change in kinetic energy, $\Delta KE$, is the difference between the final kinetic energy ($KE_f$) and the initial kinetic energy ($KE_i$) of the object.
  3. The work-energy theorem is a powerful tool for analyzing the motion of objects, as it allows you to relate the net work done on an object to the changes in its kinetic energy.
  4. The work-energy theorem is applicable to both translational and rotational motion, as long as the appropriate forms of kinetic energy are used.
  5. The work-energy theorem is a fundamental principle in classical mechanics and is used extensively in the analysis of various physical systems and phenomena.

Review Questions

  • Explain the relationship between net work and change in kinetic energy as expressed by the equation $W_{net} = \Delta KE$.
    • The work-energy theorem states that the net work done on an object is equal to the change in its kinetic energy. This means that if a net force acts on an object, causing it to change its velocity, the net work done by that force will be equal to the difference between the object's final kinetic energy ($KE_f$) and its initial kinetic energy ($KE_i$). This relationship is a powerful tool for analyzing the motion of objects, as it allows you to relate the forces acting on an object to the changes in its kinetic energy.
  • Describe how the work-energy theorem can be applied to both translational and rotational motion.
    • The work-energy theorem is applicable to both translational and rotational motion, as long as the appropriate forms of kinetic energy are used. For translational motion, the kinetic energy is given by $\frac{1}{2}mv^2$, where $m$ is the mass of the object and $v$ is its linear velocity. For rotational motion, the kinetic energy is given by $\frac{1}{2}I\omega^2$, where $I$ is the moment of inertia of the object and $\omega$ is its angular velocity. In both cases, the net work done on the object is equal to the change in its kinetic energy, as described by the work-energy theorem.
  • Analyze how the work-energy theorem can be used to understand the motion of an object under the influence of conservative and non-conservative forces.
    • The work-energy theorem is a powerful tool for analyzing the motion of objects under the influence of both conservative and non-conservative forces. Conservative forces, such as gravity or spring forces, do not change the total mechanical energy of the system, and the net work done by these forces is equal to the change in potential energy. Non-conservative forces, such as friction or air resistance, dissipate energy and result in a change in the total mechanical energy of the system. By applying the work-energy theorem, you can determine how the net work done by all the forces acting on an object is related to the changes in its kinetic energy, allowing you to understand and predict the object's motion in a wide range of physical situations.

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