| Your Results | Global Average | |
|---|---|---|
| Questions | 5 | 5 |
| Correct | 0 | 2.96 |
| Score | 0% | 59% |
| 18 ft. | |
| 2 ft. | |
| 0 ft. | |
| 6 ft. |
To balance this lever the torques at the green box and the blue arrow must be equal. Torque is weight x distance from the fulcrum so the equation for equilibrium is:
Rada = Rbdb
where a represents the green box and b the blue arrow, R is resistance (weight/force) and d is the distance from the fulcrum.Solving for da, our missing value, and plugging in our variables yields:
da = \( \frac{R_bd_b}{R_a} \) = \( \frac{40 lbs. \times 9 ft.}{60 lbs.} \) = \( \frac{360 ft⋅lb}{60 lbs.} \) = 6 ft.
The mechanical advantage of a third class lever is always:
equal to one |
|
greater than one |
|
less than one |
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not equal to 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.
| 90 ft. | |
| 4.5 ft. | |
| 1.13 ft. | |
| 13.5 ft. |
fAdA = fBdB
For this problem, the equation becomes:
5 lbs. x 9 ft. = 10 lbs. x dB
dB = \( \frac{5 \times 9 ft⋅lb}{10 lbs.} \) = \( \frac{45 ft⋅lb}{10 lbs.} \) = 4.5 ft.
| 1 ft⋅lb | |
| 2146 ft⋅lb | |
| None of these is correct | |
| 1073 ft⋅lb |
What defines the mechanical advantage of a first class lever?
input force |
|
output force |
|
output distance |
|
position of the fulcrum |
A first-class lever is used to increase force or distance while changing the direction of the force. The lever pivots on a fulcrum and, when a force is applied to the lever at one side of the fulcrum, the other end moves in the opposite direction. The position of the fulcrum also defines the mechanical advantage of the lever. If the fulcrum is closer to the force being applied, the load can be moved a greater distance at the expense of requiring a greater input force. If the fulcrum is closer to the load, less force is required but the force must be applied over a longer distance. An example of a first-class lever is a seesaw / teeter-totter.