From relative position to relative velocity
The relative position \(x_{AB}\) tells where A is, seen from B. As the two bodies move, \(x_{AB}\) changes. The rate of change of \(x_{AB}\) is the relative velocity of A with respect to B. It is the velocity that an observer riding on B measures for A.
\[ x_{AB} = x_A - x_B \]
Why. the relative position, both positions measured in the ground frame at the same instant.
\[ \dfrac{dx_{AB}}{dt} = \dfrac{dx_A}{dt} - \dfrac{dx_B}{dt} \]
Why. differentiate both sides with respect to time. The rate of change of a difference is the difference of the rates.
\[ v_{AB} = v_A - v_B \]
Read it. each rate of change of a position is a velocity. The left side is the velocity of A seen from B.
The result is one subtraction. The velocity of A seen from B is the velocity of A minus the velocity of B, both measured in the same frame. Seen from A, the velocity of B is \(v_{BA} = v_B - v_A = -v_{AB}\). If A moves away from B at \(5\,\text{m/s}\), then B moves away from A at \(5\,\text{m/s}\) in the opposite direction.
Signs do the work
On a line a velocity is a signed number. Choose one direction as positive and give every velocity its sign before you subtract. Then the one formula covers every case. The relative speed is the magnitude \(|v_{AB}|\), the rate at which the distance between the two bodies changes.
Fig 2.1 has three cases. When both move the same way, the relative velocity is the difference of the two speeds. When they move in opposite directions, \(v_B\) is negative, so subtracting it adds the speeds. When B is faster than A in the same direction, \(v_{AB}\) is negative: seen from B, the body A falls behind.
Train A moves east at \(72\,\text{km/h}\). Train B moves west at \(54\,\text{km/h}\) on the next track. Find the velocity of A relative to B and of B relative to A, in m/s.
Take east as positive. \(v_A = +72\,\text{km/h} = +20\,\text{m/s}\). \(v_B = -54\,\text{km/h} = -15\,\text{m/s}\).
\(v_{AB} = v_A - v_B\) and \(v_{BA} = -v_{AB}\).
\(v_{AB} = 20 - (-15) = +35\,\text{m/s}\). \(v_{BA} = -35\,\text{m/s}\).
A passenger in B sees train A rush east at \(35\,\text{m/s}\). A passenger in A sees train B rush west at \(35\,\text{m/s}\). Each sees the other much faster than the ground does.
A car moves at \(20\,\text{m/s}\) and a bus moves at \(12\,\text{m/s}\), both towards the east on a straight road. Find the velocity of the car relative to the bus, in m/s, with east positive.
Sit in one body and watch the others
The formula \(v_{AB} = v_A - v_B\) gives a rule for changing frames. To see everything from B, subtract \(v_B\) from every velocity in the ground frame. B itself gets \(v_B - v_B = 0\), so B is at rest. The ground, whose velocity is zero, gets \(-v_B\), so the ground moves backwards under B.
Train A moves at \(+15\,\text{m/s}\) and train B at \(-10\,\text{m/s}\). Ravi stands on the platform. In the frame of train A, what are the velocities of train B and of Ravi?
In Fig 2.2 the first chip shows the ground frame. The other two chips show the same four seconds from train A and from train B. Look at what changes and what does not. The velocities change: every arrow loses the velocity of the chosen train. The order of events does not change. The trains cross each other at the same moment in all three frames.
Let a body B move along a line at a steady velocity \(v_B\). To describe motion as seen from B, subtract \(v_B\) from the velocity of every body, including the ground. In that frame B is at rest.
In the same scene, train A moves at \(+15\,\text{m/s}\), train B at \(-10\,\text{m/s}\), and Ravi stands on the platform. In the frame of train B, what is the velocity of Ravi?
Relative acceleration
The same step works once more. The rate of change of \(v_{AB}\) is the relative acceleration of A with respect to B.
\[ a_{AB} = a_A - a_B \]
The three equations of motion from the first chapter hold for relative motion too, when \(a_{AB}\) is constant. Replace every quantity by its relative version: \(u_{AB}\), \(a_{AB}\) and the change in \(x_{AB}\).
The most useful case is \(a_A = a_B\). Then \(a_{AB} = 0\), so \(v_{AB}\) never changes. Each body may speed up or slow down, but the gap between them changes at a steady rate. Lesson 5 uses this for two balls in the air.
Two cars start side by side. Car A starts at \(10\,\text{m/s}\) and car B at \(4\,\text{m/s}\), and both speed up at \(2\,\text{m/s}^2\) in the same direction. Which statements are correct?
A fast bowler runs in at about \(7\,\text{m/s}\) before letting the ball go. The arm throws the ball forward relative to the bowler. The speed that the speed gun shows is measured in the ground frame. So the ball's ground speed is its speed relative to the bowler plus the bowler's own speed at release. That is why a bowler who stops dead at the crease bowls slower. It is also why coaches work on the run-up, not only on the arm.
- Adding the speeds when the bodies move in the same direction.Give each velocity its sign and subtract. Same direction gives a difference of speeds; opposite directions give a sum.
- Mixing frames in one subtraction, such as a velocity measured from a train minus a velocity measured from the ground.Both velocities in \(v_A - v_B\) must be measured in the same frame, usually the ground frame.
- Forgetting that the ground moves in the frame of a moving body.In the frame of B, the ground moves at \(-v_B\).