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Exam 3 Analysis in Mechanical Engineering 11/16/93
Closed book Van Dommelen 2:45-4:00

Show all reasoning. One book of mathematical tables may be used.

1.
The direction of the field lines of a two-dimensional electrostatic field is given by:

\begin{displaymath}
E_y {\rm d} x - E_x {\rm d} y = 0\end{displaymath}

Find an algebraic expression for the field lines of the field:

\begin{displaymath}
E_x = e^x \cos (y) + x - y\end{displaymath}

\begin{displaymath}
E_y = -e^x \sin (y) - x - y\end{displaymath}

2.
For the RCL circuit shown below, the voltage across the condensator satisfies

\begin{displaymath}
{{\rm d}^2 V\over {\rm d} t^2} + {R\over L} {{\rm d} V\over {\rm d} t}
+ {1\over LC} V = e(t)\end{displaymath}

Assuming that the resistance R=3, capacitance C=0.5 and inductance L=1, and the applied voltage is e(t)= - e-t/(1+et), find the voltage across the condensator.


\begin{figure}
\centering\epsffile{figures/aim93x3.ps2}\end{figure}

3.
A projectile is fired through a constant area, but variable density duct. Assuming the velocity variation is linear with distance, the equation of motion for the projectile is

\begin{displaymath}
\ddot x = a {(x - \dot x)^2 \over x}\end{displaymath}

where a is a constant that cannot be scaled out. Assuming that a=1, find an algebraic expression relating the projectile velocity $\dot x$ to its position x. Verify that the projectile never catches up with the stream: projectile velocity does not become equal to position at large x.



'Author: Leon van Dommelen'