Unit: Work, Energy, and Power

Lesson Preview

Forces are classified into two categories based on how they do work:

Conservative forces do work that depends only on initial and final positions, not on the path taken.

Gravity and spring forces are the primary examples.

Consider lifting a book of mass mm to height hh. Gravity does work Wg=mghW_g = -mgh whether you lift it straight up or along any other path. Only the vertical displacement matters.

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Non-conservative forces do path-dependent work.

Friction and air resistance are the main examples.

Consider pushing a box across a floor with kinetic friction force fk=μkmgf_k = \mu_k mg. The work done by friction is:

Wfriction=fkdW_{\text{friction}} = -f_k \cdot d

where dd is the total distance traveled. A straight path of length d1d_1 gives work W1=μkmgd1W_1 = -\mu_k mg d_1. A longer path of length d2>d1d_2 > d_1 between the same endpoints gives more negative work: W2=μkmgd2W_2 = -\mu_k mg d_2. The endpoints are identical, but the work differs because the path lengths differ.

... continued in the full lesson.

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