A sprinkler wagon wets asphalt on a hot summer day. the power of the mottor is barely great enough to over the combined friction of the ground and the wheels, of the air, and the axle bearings. The vehicle therefore behaves as if under no forces. Let $m$ be the mass of the water in the water tank at any instant plus the constant mass of the empty vehicle. Let the amount of water squirted out per unit time $\mu = -\dot{m}$ , be its exit velocity towards rear, $q$, a seen from the wagon, or $v-q$ as seen from the street, $v$ be the speed of the vehicle. Then using Newton's second law the rate of change of momentum og the water + wagon = Force on the wagon. or, \begin{eqnarray}
\dot{p} = 0 \\
\frac{d}{dt}(m v) =0\\
\dot{m} v + m \frac{dv}{dt} =0 \\
or, m \frac{dv}{dt}= \mu v
\end{eqnarray} It would then appear that the acceleration of the wagon is independent of the
exit velociy $q$. This is paradoxical. Give your comments.
Source:Sommerfeld
Exclude node summary :
Exclude node links:
4727:Diamond Point