2.5. The Kinematic Equations http://www.ck12.org
Kinematic Equations
1.vavg=∆∆xt, always true
2.aavg=∆∆vt, always true
3.vf=at+vi, constant acceleration only
4.vavg=(vf+ 2 vi), constant acceleration only
5.x=^12 at^2 +vit+xi, constant acceleration only
6.vf^2 =vi^2 + 2 a∆x, constant acceleration only
The link below shows an example using the kinematic equations for horizontal motion under acceleration.
http://demonstrations.wolfram.com/BrakingACar/
- Displacement is the difference between the ending position and starting position of motion. It is a vector
quantity. - Velocity is the rate of change of position. It is vector quantity.
- Average speed can be computed finding the total distance divided by the total time or by a weighted average.
- The slope of a line in the position-time plane represents velocity.
- The area in the acceleration-time plane represents a change in velocity.
- Area in the velocity-time plane represents a change in position (displacement).
- The slope of a line in the velocity-time plane represents acceleration.
- The gravitational acceleration near the surface of the earth is very close to 9. 8 m/s^2.
- The kinematic equations of motion in one dimension are:
1.vavg=∆∆xt, always true
2.aavg=∆∆vt, always true
3.vf=at+vi, constant acceleration only
4.vavg=(vf+ 2 vi), constant acceleration only
5.x=^12 at^2 +vit+xi, constant acceleration only
6.vf^2 =vi^2 + 2 a∆x, constant acceleration only