Distance and Constant Velocity Problems

Since the velocity is constant (zero acceleration), the vector straight-line distance travelled is in the same direction as the velocity vector. Typically the problem has a mixture of distance and velocity vectors. Since diagrams must always use vectors of the same type, it is best to convert velocities to distances using the simple relationship D = Vt where t is the travel time. The distances combine to form simple polygons. For instance if three vectors are involved, one has a triangle as shown below.


The key to solving the problem is to realize that each vector can be decomposed into its x and y components as shown below.



The x and y components of the vectors are then related by simple equations. Notice in Figure 1 that the tail of D3 is at the nose of D2, that is D3 is added to D2.  Since the tail of D1 is at the tail of D2 and the nose of D1 is at the nose of D3 we have the vector equation D1 = D2 + D3. This vector equation has two parts for us to work with D1x = D2x + D3x and D1y = D2y + D3y.

Example

Two vehicles leave the same spot at the same time. Vehicle 1 travels at 25 km/h at f = 25° west of north. Vehicle 2 travels at 18 km/h at b = 40° west of north. They stop at the same time and are now 200 km apart.

  1. How long where they travelling for?
  2. If vehicle 1 turns to face vehicle 2, what direction would it be looking in?

We first sketch our diagram with the given information. It looks much like Figure 1.

Our equations are

                                              –25tsin(25°)  = 18tcos(40°)t – 200cos(a)                                       [1a]

                                               25tcos(25°)  = 18tsin(40°)t + 200sin(a)                                        [1b]

To solve we should collect terms with t on the same side

                                            –t{25sin(25°) + 18cos(40°)} = –200cos(a)                                      [2a]

                                               t{25cos(25°) – 18sin(40°)} = 200sin(a)                                        [2b]

and simplify

                                                           t{24.3543} = 200cos(a)                                                     [3a]

                                                           t{11.0875} = 200sin(a)                                                     [3b]

To solve this we either eliminate t or a – but we don’t have a by itself, we have cos(a) and sin(a). In cases like this we usually need to use one of the trigonometric identities: tan(a) = sin(a)/cos(a), cos2(a) + sin2(a) = 1, or sin(2a) = 2 sin(a)cos(a). The first identity is useful here. Taking the ratio of equation [2b] to [2a]


With this value of a we use equation [3a] or [3b] to find t = 3.40 hours.

So vehicles travelled 3.40 hours and vehicle 1 would have to look at 24.5° west of north to see vehicle 2.