Chapter 1 - Kinematics Flashcards
Kinematics
Study of motion without looking at forces causing the motion
Terms used to describe motion (5)
Distance, displacement, speed, velocity, acceleration
Distance
Actual path followed by a moving object
Scalar quantity measured in metres (m)
Displacement
Shortest distance between 2 points (straight line), distance travelled in a particular direction
Vector quantity measured in (m)
Motion in a circle
Distance around full circle is 2πr
Displacement around full circle is 0
Velocity is 0
Distance from opposite halves is πr
Displacement is 2r
Average Speed
Scalar quantity measured in ms-1
Usually changes unless an object is moving at a constant speed, so we take an average
Velocity
Vector quantity measured in ms-1
Acceleration
Rate of flow of velocity
Vector quantity measured in ms-2
Circular motion
movement of an object along the circumference of a circle or rotation
along a circular path. This motion occurs when the vectors of velocity and acceleration are
constantly perpendicular.
Projectile motion
form of motion in which an object or particle (called a projectile) is thrown near the earth’s surface, and it moves along a curved path under the action of gravity only. The only force of significance that acts on the object is gravity, which acts downward to cause a downward acceleration.
Terminal velocity
highest velocity attainable by an object as it falls through a fluid such as air or oil.
Newton’s laws of motion
three physical laws which provide relationships between the forces acting on a body and the motion of the body.
Newtons 1st law
States that an object in motion continues to move with uniform velocity, an object at rest stays at rest, unless the object is acted upon by a resultant force
Inertia
tendency of an object to resist changes in its state of motion
What can be deduced from Newtons 1st law (3)
Inertia - tendency of an object to resist changes in its state of motion
An object can move without forces acting on it
If an object is at rest/moving with constant velocity then all forces acting in any direction have a resultant of 0