Notices
 

[QUE/CM-01013] Variable Mass Problems

For page specific messages
For page author info

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 : 

n

4727:Diamond Point

0
 
X