-- KINEMATICS --
-- PROJECTILE MOTION --
-- DYNAMICS --
-- CIRCULAR MOTION --
-- WORK & ENERGY --
-- IMPULSE & MOMENTUM --
-- CENTER OF MASS --
-- TORQUE - STATICS --
-- TORQUE - DYNAMICS --
-- TORQUE - ENERGY & MOMENTUM --
-- FLUIDS --
-- OSCILLATIONS --
-- MECHANICAL WAVES --

P01B2020 – Trains Approaching

Trains Approaching

Two trains are moving on straight tracks in opposite directions. They are approaching a single-track section of length $L$ where only one train can drive at a time. A cargo train is coming from the left at speed $v_0$, and reads the sign about the upcoming single-track section at distance $L$. It starts decelerating immediately and loses half its speed over the distance $L/2$. Simultaneously, a passenger train is coming from the right. It has priority to use the single-track and maintains constant speed of $2v_0$. Both trains are a distance $L$ away from the single-track section at time $t=0$ as shown in the figure below.

As a first approximation, both trains can be considered as point masses.

1. Without any calculation, predict whether or not there would be a collision between the two trains. Explain why.

View answer

After a distance $L/2$, the cargo train has halved its speed. As long as its acceleration remains constant, we can conclude that its speed will drop to zero after traveling a distance $L/2$ again. Thus, the cargo train will come to a full stop after traveling a distance $L$ which means that it will not enter the single-track section and there is no risk of collision between the trains.

2. Determine the acceleration of the cargo train, right after it starts decelerating.

View answer

The acceleration $a_1$ of the cargo train is such that over the distance $L/2$, its initial velocity $v_0$ decreases to $v_0/2$. Thus, we solve for $a_1$ as follows

\begin{aligned}
v^2_{fx}=v^2_{0x}+2a_x\mathrm{\Delta }x\ \ \ \ &\Rightarrow \ \ \ \ \ \frac{v^2_0}{4}=v^2_0+2a_1\cdot \frac{L}{2} \\
\\
&\Rightarrow \ \ \ \ \ a_1L=\frac{v^2_0}{4}-v^2_0 \\
\\
&\Rightarrow \ \ \ \ \ a_1=-\frac{3v^2_0}{4L}
\end{aligned}

The acceleration of the cargo train is equal to

\boxed{a_1=-\frac{3v^2_0}{4L}}

where the negative sign is consistent with the cargo train slowing down.

3. Determine how long it takes until the passenger train exits the single-track section.

View answer

To clear the single-track section, the passenger train must travel a distance $2L$ at a constant speed $2v_0$ which requires an amount of time $t_f$ equal to

\boxed{t_f=\frac{2L}{2v_0}=\frac{L}{v_0}}

4. During the time found in part 3., what is the distance traveled by the cargo train? Does that confirm your prediction made in part 1.?

View answer

The position of the cargo train as it slows down is given by

x\left(t\right)=\frac{1}{2}a_1t^2+v_{0x}t=-\frac{3v^2_0}{8L}t^2+v_0t

In the time $t_f$ it takes the passenger train to clear the single-track section, the cargo train will travel a distance equal to

\boxed{x\left(t_f\right)=-\frac{3v^2_0}{8L}t^2_f+v_0t_f=-\frac{3v^2_0}{8L}{\left(\frac{L}{v_0}\right)}^2+v_0\cdot \frac{L}{v_0}=-\frac{3L}{8}+L=\frac{5L}{8}\ <\ \ L}

This distance is less than the distance $L$ separating the cargo train from the single-track section and therefore there is no risk of collision since the passenger train will clear the single-track section before the cargo train even reaches it.