Example 10.5 from College Physics, 10.2 Kinematics of Rotational Motion
Large freight trains accelerate very slowly. Suppose one such train accelerates from rest, giving its 0.350-m-radius wheels an angular acceleration of . After the wheels have made 200 revolutions (assume no slippage): (a) How far has the train moved down the track? (b) What are the final angular velocity of the wheels and the linear velocity of the train?
Work it out on paper first. Then open the solution one step at a time, and stop as soon as you can finish on your own.
In part (a), we are asked to find , and in (b) we are asked to find and . We are given the number of revolutions , the radius of the wheels , and the angular acceleration .
The distance is very easily found from the relationship between distance and rotation angle:
Solving this equation for yields
Before using this equation, we must convert the number of revolutions into radians, because we are dealing with a relationship between linear and rotational quantities:
Now we can substitute the known values into to find the distance the train moved down the track:
We cannot use any equation that incorporates to find , because the equation would have at least two unknown values. The equation will work, because we know the values for all variables except :
Taking the square root of this equation and entering the known values gives
We can find the linear velocity of the train, , through its relationship to :
The distance traveled is fairly large and the final velocity is fairly slow (just under 32 km/h).
How did it go?