Many of the objects we encounter in everyday life are in motion or have parts
that are in motion. Motion is the rule, not the exception. The physical laws that govern the motion of these objects
are universal, i.e. all the objects move according to the same rules,
and one of the goals of this class is to understand these rules.
When an object moves, its position changes as a function of time.
The position of an object is given relative to some agreed upon reference point. It is not enough to just specify the distance from the reference point. We also have to specify the direction. Distance is a scalar quantity, it is a number given in some units. Position is a vector quantity. It has a magnitude as well as a direction. The magnitude of a vector quantity is a number (with units) telling you how much of the quantity there is and the direction tells you which way it is pointing. A unit vector is a direction indicator. It is a dimensionless vector with magnitude 1, used to specify a direction. In text, vector quantities are usually printed in boldface type or with an arrow above the symbol. Thus, while d = distance, d = displacement.
Scalars and Vectors (Please explore!)
A convenient way to specify the position of an object
is with the help of a coordinate system.
We choose a fixed point, called the origin
and three directed lines, which pass through the origin and are
perpendicular to each other. These lines are called the coordinate axes
of a three-dimensional rectangular (Cartesian) coordinate system and are labeled
the x-, y-, and z-axis. Three numbers with units specify the position of a
point P. These numbers are the x-, y-, and z-coordinates of the point P.
The coordinates of the point P in the
diagram to the right are (a, b, c).
The coordinates of the point P are the components of the position vector. A unit vector pointing in the x-direction has a x-component of 1 and y- and z- components of zero. It is denoted by i. Similarly, a unit vector pointing in the y-direction is denoted by j, and a unit vector pointing in the z-direction is denoted by k. Unit vectors are direction indicators.
The components of any vector add up to form the vector itself.
The position vector of a point P with coordinates (a, b, c) may be written in terms of its components as r = ai + bj + ck.
|The magnitude of the position vector is its length r. It depends on the choice of the origin of the coordinate system. It is the straight-line distance of P from the origin.
Position vector of the Nielsen Physics Building on a small map with the lower left corner as the origin.
A change in position is called a displacement. The diagram below shows the positions P1 and P2 of a player at two different times.
The arrow pointing from P1 to P2 is the
Its magnitude is the straight-line distance between P1 and P2.
The components of the displacement vector from P1 to P2 are (x2 - x1) along the x-axis, (y2 - y1) along the y-axis.
The displacement vector d from P1 to P2 may be written as d = (x2 - x1)i + (y2 - y1)j.
The displacement d is (x2 - x1) units in the x-direction plus (y2 - y1) units in the y-direction.
The magnitude of the displacement is d = ((x2 - x1)2 + (y2 - y1)2)½. This follows from the Pythagorean theorem.
The distance between two points P1 with coordinates (x1, y1, z1) and P2 with coordinates (x2, y2, z2) is
d = ((x2 - x1)2 + (y2 - y1)2 + (z2 - z1)2)½.
The triple of real numbers dx = (x2 - x1), dy = (y2 - y1), dz = (z2 - z1) are called the Cartesian components of d.
Link: Distance and Displacement (Please explore!)
A football quarterback runs 15.0 m
straight down the playing field (in the
positive x direction) in 2.50 s.
He is then hit and pushed 3.00 m
straight backward in 1.75 s. He
breaks the tackle and runs straight
forward another 21.0 m in 5.20 s.
Calculate his displacement vector and
the total distance traveled.
Choose your coordinate system so the player starts at x = 0. After 2.5 s, he ends up at x = 15 m.
He then moves backward 3 m, and ends up at x = 12 m after another 1.75 s.
He moves forward 21 m in the next 5.2 s and ends up at x = 12 m + 21 m = 33 m.
His displacement vector is d = (33 m)i, i.e. 33 m forward.
His total distance traveled is 15 m + 3 m + 21 m = 39 m.
Note: The total distance traveled is NOT the straight-line distance from the start to the end point if an object does not move in a straight line without changing direction.
While traveling along a straight interstate highway you notice that the mile marker reads 260. You travel until you reach the 150-mile marker, and then retrace your path to the 175-mile marker. What is the magnitude of your resultant displacement from the 260-mile marker?
The resultant displacement is the vector d, the sum of two vectors d1 and d2 which point in opposite directions. The magnitude of the resultant displacement vector is (260 - 175) miles = 85 miles.
The tip of a helicopter blade is
5.00 m from the center of rotation.
For one revolution of the blade,
calculate the displacement vector and
the total distance traveled for the tip
of the blade.
After one revolution, the tip returns to is original position. Its displacement vector d = 0.
The total distance traveled by the tip equals the circumference of a circle of radius r = 5 m.
Circumference = 2πr = 31.42 m.
The total distance traveled by the tip is 31.42 m.
The displacement vector has the same magnitude and direction, independent of the choice of origin of the coordinate system. The magnitude and direction of the displacement vector, however, depend on the reference frame in which the coordinate system is anchored and at rest.
A car has moved forward a distance of 6 m, while a child has moved forward from the back seat to the front seat a distance of 1 m.