Force
NOTE: Objects can be taken as point particles (for illustration)
Mass
Weight
*Gravity is not acceleration due to gravity (which is what’s changing)
Converting between mass and weight
W = mg (weight = mass x acceleration due to gravity [we use W or mg to represent weight])
Same as F = ma
Tension (T)
*In ex., arrow towards person pulling b/c tension toward him (pulling toward him)
*In ex. 2, b/c the ceiling is the one holding it, it’s pulling
Normal reaction force (R)
Gravitational force (W or mg)
*Normal force starts at point of contact (surface) and gravity starts at center
Friction force (F)
Upthrust (U)
Air resistance (R)
Opposes motion of an object through the air
Free-body diagrams
A diagram that shows only the forces acting on a specific object (if there was a box and a table, the question would tell us what to focus on)
*On a ramp, weight bigger b/c it’s what’s pulling it down
*W/ the ceiling thing, tension, again, longer b/c the ball isn’t falling down (something’s holding it up)
*For object attached to two strings on the ceiling, one of the T’s would equal weight b/c they’re not on the same line of action (?)
NOTE
*if forces in the same line of action have to be 0, we may have to resolve certain forces (ex. If we find the vertical components, add them up, and they add up to net force = 0)
*Constant speed/velocity means no acceleration and, thus, no net force
*R could’ve been from the top, but to make it look nice, we connect them
*See examples (motion of parachutist, car moving to the right)
*See ex. (ff moving horizontally, vertical forces must be balanced [also, if accelerating force—?—was less than friction, car would be deccelerating/slowing down])
*Can have equilibrium in rota
*See elevator ex.
Addition of forces
Forces are vectors and must be added vectorially (length and direction must be considered):
- Opposite forces have opposite signs
- Equal parallel forces are the same
- Sum of forces is called resultant force
*Also, remember Pythagoras’s Theorem and to use the parallelogram/head-to-tail method for direction
Balanced forces
*Remember that if resolving, horizontal components must equate as well
*Draw triangles, use trig, ex. W = sum of vertical component of R + vertical component of F
*See formulae, but calculate to make sure
*Tension was 0 in that first example b/c both falling at the same time
Hooke’s Law
*Doesn’t have to pass through origin (sometimes, systematic error)
*When the variables are flipped (axis-wise), the slope becomes the inverse of the original
Newton’s 1st Law
Translational equilibrium
Conditions necessary for an object to be in equilibrium
*You can’t say for sure that the object is either at rest or moving at constant velocity, but you can say for sure that the object’s net force is 0