Quantcast
Loading [MathJax]/jax/output/CommonHTML/jax.js

LM 8_1 The velocity vector Collection

Last modified by
on
Sep 29, 2022, 12:50:17 AM
Created by
on
Oct 18, 2019, 1:17:59 AM
Equations
Tags
UUID
1f5273cb-f145-11e9-8682-bc764e2038f2

8.1 The velocity vector by Benjamin Crowell, Light and Matter  licensed under the Creative Commons Attribution-ShareAlike license.

 

8.1 The velocity vector

For motion with constant velocity, the velocity vector is

              v=ΔrΔt   [Only for constant velocity]

The Δr vector points in the direction of the motion, and dividing it by the scalar Δt only changes its length, not its direction, so the velocity vector points in the same direction as the motion. When the velocity is not constant, i.e., when the x-t, y-t, and z-t graphs are not all linear, we use the slope-of-the-tangent-line approach to define the components vx, vy, and vz, from which we assemble the velocity vector. Even when the velocity vector is not constant, it still points along the direction of motion.

Vector addition is the correct way to generalize the one-dimensional concept of adding velocities in relative motion, as shown in the following example:

Example 1: Velocity vectors in relative motion

You wish to cross a river and arrive at a dock that is directly across from you, but the river's current will tend to carry you downstream. To compensate, you must steer the boat at an angle. Find the angle θ, given the magnitude,|vWL|, of the water's velocity relative to the land, and the maximum speed, |vBW|, of which the boat is capable relative to the water.

The boat's velocity relative to the land equals the vector sum of its velocity with respect to the water and the water's velocity with respect to the land,

                                vBL=vBW+vWL.

If the boat is to travel straight across the river, i.e., along the y axis, then we need to have vBL,x=0. This x component equals the sum of the x components of the other two vectors,


                               vBL,x=vBW,x+vWL,x

or

                                0=-|vBW|sinθ+|vWL|.

Solving for θ, we find

                                sinθ=|vWL|/|vBW|,

 so 

                                 θ=sin-1(|vWL||vBW|).

Solved problem: Annie Oakley — problem 8

Discussion Questions

A   Is it possible for an airplane to maintain a constant velocity vector but not a constant |v|? How about the opposite - a constant |v| but not a constant velocity vector? Explain.

B   New York and Rome are at about the same latitude, so the earth's rotation carries them both around nearly the same circle. Do the two cities have the same velocity vector (relative to the center of the earth)? If not, is there any way for two cities to have the same velocity vector?

8.1 The velocity vector by Benjamin Crowell, Light and Matter  licensed under the Creative Commons Attribution-ShareAlike license.

Calculators and Collections

  • Comments
  • Attachments
  • Stats
No comments
This site uses cookies to give you the best, most relevant experience. By continuing to browse the site you are agreeing to our use of cookies.