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Adding the vectors, we find v PE = 8 m / s i ^ , so the person is moving 8 m/s east with respect to Earth. Graphically, this is shown in [link] .

Velocity vectors of the train with respect to Earth, person with respect to the train, and person with respect to Earth. V sub T E is the velocity vector of the train with respect to Earth. It has value 10 meters per second and is represented as a long green arrow pointing to the right. V sub P T is the velocity vector of the person with respect to the train. It has value -2 meters per second and is represented as a short green arrow pointing to the left. V sub P E is the velocity vector of the person with respect to Earth. It has value 8 meters per second and is represented as a medium length green arrow pointing to the right.
Velocity vectors of the train with respect to Earth, person with respect to the train, and person with respect to Earth.

Relative velocity in two dimensions

We can now apply these concepts to describing motion in two dimensions. Consider a particle P and reference frames S and S , as shown in [link] . The position of the origin of S as measured in S is r S S , the position of P as measured in S is r P S , and the position of P as measured in S is r P S .

An x y z coordinate system is shown and labeled as system S. A second coordinate system, S prime with axes x prime, y prime, z prime, is shifted relative to S. The vector r sub S prime S, shown as a purple arrow, extends from the origin of S to the origin of S prime. Vector r sub P S is a vector from the origin of S to a point P. Vector r sub P S prime is a vector from the origin of S prime to the same point P. The vectors r s prime s, r P S prime, and r P S form a triangle, and r P S is the vector sum of r S prime S and r P S prime.
The positions of particle P relative to frames S and S are r P S and r P S , respectively.

From [link] we see that

r P S = r P S + r S S .

The relative velocities are the time derivatives of the position vectors. Therefore,

v P S = v P S + v S S .

The velocity of a particle relative to S is equal to its velocity relative to S plus the velocity of S relative to S .

We can extend [link] to any number of reference frames. For particle P with velocities v P A , v P B , and v P C in frames A , B , and C ,

v P C = v P A + v A B + v B C .

We can also see how the accelerations are related as observed in two reference frames by differentiating [link] :

a P S = a P S + a S S .

We see that if the velocity of S relative to S is a constant, then a S S = 0 and

a P S = a P S .

This says the acceleration of a particle is the same as measured by two observers moving at a constant velocity relative to each other.

Motion of a car relative to a truck

A truck is traveling south at a speed of 70 km/h toward an intersection. A car is traveling east toward the intersection at a speed of 80 km/h ( [link] ). What is the velocity of the car relative to the truck?

A truck is shown traveling south at a speed V sub T E of 70 km/h toward an intersection. A car is traveling east toward the intersection at a speed V sub C E of 80 km/h
A car travels east toward an intersection while a truck travels south toward the same intersection.

Strategy

First, we must establish the reference frame common to both vehicles, which is Earth. Then, we write the velocities of each with respect to the reference frame of Earth, which enables us to form a vector equation that links the car, the truck, and Earth to solve for the velocity of the car with respect to the truck.

Solution

The velocity of the car with respect to Earth is v CE = 80 km / h i ^ . The velocity of the truck with respect to Earth is v TE = −70 km / h j ^ . Using the velocity addition rule, the relative motion equation we are seeking is

v CT = v CE + v ET .

Here, v CT is the velocity of the car with respect to the truck, and Earth is the connecting reference frame. Since we have the velocity of the truck with respect to Earth, the negative of this vector is the velocity of Earth with respect to the truck: v ET = v TE . The vector diagram of this equation is shown in [link] .

The right triangle formed by the vectors V sub C E to the right, V sub E T down, and V sub C T up and right is shown V sub C T is the hypotenuse and makes an angle of theta with V sub C E. The vector equation vector v sub C T equals vector C E plus vector E T is given. A compass is shown indicating north is up, east to the right, south down, and west to the left.
Vector diagram of the vector equation v CT = v CE + v ET .

We can now solve for the velocity of the car with respect to the truck:

| v CT | = ( 80.0 km / h ) 2 + ( 70.0 km / h ) 2 = 106. km / h

and

θ = tan −1 ( 70.0 80.0 ) = 41.2 ° north of east.

Significance

Drawing a vector diagram showing the velocity vectors can help in understanding the relative velocity of the two objects.

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Check Your Understanding A boat heads north in still water at 4.5 m/s directly across a river that is running east at 3.0 m/s. What is the velocity of the boat with respect to Earth?

Labeling subscripts for the vector equation, we have B = boat, R = river, and E = Earth. The vector equation becomes v BE = v BR + v RE . We have right triangle geometry shown in Figure 04_05_BoatRiv_img. Solving for v BE , we have
v BE = v BR 2 + v RE 2 = 4.5 2 + 3.0 2
v BE = 5.4 m / s, θ = tan −1 ( 3.0 4.5 ) = 33.7 ° .
Vectors V sub B W, V sub W E and V sub B E form a right triangle. A boat is shown at the vertex where the tails of V sub B W and V sub B E meet. Vector V sub B W points up. V sub W E points to the right. V sub B E points up and right, at an angle to the vertical. V sub B E is the vector sum of v sub B W and V sub W E.

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Practice Key Terms 2

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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