| Your Results | Global Average | |
|---|---|---|
| Questions | 5 | 5 |
| Correct | 0 | 2.98 |
| Score | 0% | 60% |
| 0.83 ft. | |
| 1.25 ft. | |
| 2.5 ft. | |
| 5 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 = \( \frac{R_bd_b}{R_a} \) = \( \frac{25 lbs. \times 5 ft.}{50 lbs.} \) = \( \frac{125 ft⋅lb}{50 lbs.} \) = 2.5 ft.
| 17.14 lbs. | |
| 51.43 lbs. | |
| 4.29 lbs. | |
| 270 lbs. |
fAdA = fBdB + fCdC
For this problem, this equation becomes:
30 lbs. x 9 ft. = 50 lbs. x 3 ft. + fC x 7 ft.
270 ft. lbs. = 150 ft. lbs. + fC x 7 ft.
fC = \( \frac{270 ft. lbs. - 150 ft. lbs.}{7 ft.} \) = \( \frac{120 ft. lbs.}{7 ft.} \) = 17.14 lbs.
The principle of conservation of mechanical energy states that, as long as no other forces are applied, what will remain constant as an object falls?
acceleration |
|
kinetic energy |
|
total mechanical energy |
|
potential energy |
As an object falls, its potential energy is converted into kinetic energy. The principle of conservation of mechanical energy states that, as long as no other forces are applied, total mechanical energy (PE + KE) of the object will remain constant at all points in its descent.
| 2.2 | |
| 10 | |
| 0 | |
| 2 |
The mechanical advantage (MA) of an inclined plane is the effort distance divided by the resistance distance. In this case, the effort distance is the length of the ramp and the resistance distance is the height of the green box:
MA = \( \frac{d_e}{d_r} \) = \( \frac{10 ft.}{5 ft.} \) = 2
Collinear forces:
act along the same line of action |
|
are unrelated to each other |
|
pass through a common point |
|
act in a common plane |
Collinear forces act along the same line of action, concurrent forces pass through a common point and coplanar forces act in a common plane.