Course 5.2Lesson 1 of 3
A force is conservative when its work depends only on where a body starts and ends, not on the path. Gravity and spring forces are conservative; friction and drag are not. For a conservative force we can define potential energy, so that ; near the Earth
Try the code and the simulations beside the lesson.
Lift a book onto a shelf and you do work against gravity. Let it fall, and gravity gives the work back as kinetic energy. Push a box across a rough floor, though, and the work is gone: friction turns it into heat, and pushing the box back costs you all over again.
A force is conservative if the work it does on a body moving from A to B is the same whatever path the body takes. Then the work round any closed loop is zero.
Explore it with ramps of the same height.
You should find that gravity's work stays for every angle, while friction takes more on a gentle, longer ramp.
For a conservative force we can keep an account: the potential energy , so that the force's work equals the drop in :
Near the Earth, gravity gives , with measured from any level we choose; only changes in matter. A spring gives .
Run the account backwards: the force is the downhill slope of ,
Where has a minimum, and the body sits in stable equilibrium, like a marble in a bowl.
Watch out. Potential energy belongs to a body and the Earth (or the spring) together. And the minus sign matters: the force points toward lower .
A hiker climbs up a mountain, once by the steep path and once by the long winding road.
Think first. If a force's work depends on the path, it has no potential energy. Then you must work out its work along the actual path.
The program slides a block down four ramps of the same height and compares gravity's work with friction's.
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
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