201902200839 Exercise 5 Chapter 2

A particle is subjected to the potential V(x)=-Fx, where F is a constant. The particle travels from x=0 to x=a in a time interval t_0. Assume the motion of the particle can be expressed in the form x(t)=A+Bt+Ct^2. Find the values of A, B, and C such that the action is a minimum.


Solution.

The solution is not mine. It was found on the Internet some years ago, to whose author(s) I lost references.

1D-case:

\mathcal{L}=T-V=\displaystyle{\frac{1}{2}}m\dot{x}^2+Fx.

Euler-Lagrange (E-L) equation:

\displaystyle{\frac{\mathrm{d}}{\mathrm{d}t}}\bigg( \displaystyle{\frac{\partial \mathcal{L}}{\partial \dot{x}}}\bigg) =\frac{\partial \mathcal{L}}{\partial x}

gives the path over which the action is stationary.

That is,

\begin{aligned} \displaystyle{\frac{\mathrm{d}}{\mathrm{d}t}}( m\dot{x}) & = F \\  \Rightarrow \ddot{x} & =\displaystyle{\frac{F}{m}}\\ \end{aligned}.

On x(t)=A+Bt+Ct^2 taking derivative twice,

\ddot{x}(t)=2C.

Equate them,

C=\displaystyle{\frac{F}{2m}}.

The event (x=0,t=0) gives

A=0.

And the event (x=a,t=t_0) gives

a=x(t_0)=Bt_0+\displaystyle{\frac{F}{2m}}t_0^2.

Express it as

B=\displaystyle{\frac{a-\frac{F}{2m}t_0^2}{t_0}}.

Thus,

x(t)=(0)+\Bigg( \displaystyle{\frac{a-\frac{F}{2m}t_0^2}{t_0}}\Bigg) t+\bigg( \displaystyle{\frac{F}{2m}}\bigg) t^2

is recovered.

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