PHYS 218 Chapter 3
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Motion in 2 Dimensions
- Velocity is tangent to an object's path.
- Acceleration always points toward the concave side of an object's path
Any change in an object's path is the result of acceleration (you can feel acceleration). This means that even with a constant speed, velocity might change.
Acceleration perpendicular to velocity maintains speed but changes direction
Circular Motion
A particle moving around a circle (stays same distance from center)
At two instances, the angles between the change around the radius and the change in velocity are equivalent
Always true in circular motion:
- (always to center)
If velocity is not constant around the entire circle, the resultant acceleration vector always points inward, but not necessarily toward center.
If the velocity remains constant around the entire circle, the parallel acceleration is 0, and the perpendicular velocity is a constant pointing to the center
Example
Imagine a perfectly circular race track with an even bank around the edge. A car is traveling at a constant speed around the track. The only (resultant) acceleration acting on the car is pointing toward the center.
Uniform Circular Motion
Period: time needed to make a full circle.
Example
Pilot endurance test:
- r = 6m + 2m = 8m
- frequency = 2 rev/sec ∴ t = 1/2 sec
Relative Velocities
Position, Velocity, and Acceleration of an object as seen in reference to another position, velocity and acceleration in respect to each other
Draw two coordinate systems for this problem:
- xp/A = xB/A + xp/B [1]
- vp/A = vB/A + vp/B
- ap/A = aB/A + ap/B
Example
- Plane travels North at 300 km/h (with respect to the air)
- Wind is in Northeast direction at 50 km/h (with respect to ground)
- Find velocity of plane with respect to ground:
Given:
- vair/ground = (50 km/h, 45°)
- vplane/air</sub = (300 km/h, 0°)
Footnotes
- ↑ xp/A = x component of point p in reference frame A.