| Your Results | Global Average | |
|---|---|---|
| Questions | 5 | 5 |
| Correct | 0 | 2.43 |
| Score | 0% | 49% |
| 1 ft⋅lb | |
| 14 ft⋅lb | |
| 38500 ft⋅lb | |
| 28 ft⋅lb |
| 0 lbs. | |
| 150 lbs. | |
| 42.5 lbs. | |
| 14.17 lbs. |
fAdA = fBdB + fCdC
For this problem, this equation becomes:
50 lbs. x 9 ft. = 65 lbs. x 3 ft. + fC x 6 ft.
450 ft. lbs. = 195 ft. lbs. + fC x 6 ft.
fC = \( \frac{450 ft. lbs. - 195 ft. lbs.}{6 ft.} \) = \( \frac{255 ft. lbs.}{6 ft.} \) = 42.5 lbs.
Torque involves a perpendicular force applied to a lever arm that moves around a center of rotation. Increasing the length of the lever arm will do which of the following?
increase applied force |
|
decrease torque |
|
decrease applied force |
|
increase torque |
Torque measures force applied during rotation: τ = rF. Torque (τ, the Greek letter tau) = the radius of the lever arm (r) multiplied by the force (F) applied. Radius is measured from the center of rotation or fulcrum to the point at which the perpendicular force is being applied. The resulting unit for torque is newton-meter (N-m) or foot-pound (ft-lb).
The mechanical advantage of a third class lever is always:
less than one |
|
equal to one |
|
not equal to one |
|
greater than one |
A third class lever is designed to multiply distance and speed at the expense of effort force. Because the effort force is greater than the resistance, the mechanical advantage of a third class lever is always less than one.
An example of a third class lever is a broom. The fulcrum is at your hand on the end of the broom, the effort force is your other hand in the middle, and the resistance is at the bottom bristles. The effort force of your hand in the middle multiplies the distance and speed of the bristles at the bottom but at the expense of producing a brushing force that's less than the force you're applying with your hand.
Concurrent forces:
act along the same line of action |
|
act in a common plane |
|
pass through a common point |
|
act in a common dimension |
Collinear forces act along the same line of action, concurrent forces pass through a common point and coplanar forces act in a common plane.