Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 14 - Fluids - Problems - Page 412: 82

Answer

$3.826\;m/s^2$

Work Step by Step

The ratio of the air density outside the balloon to that inside is $1.39$ $\frac{\rho_{out}}{\rho_{in}}=1.39$ The ratio implies that the the density of the air inside the balloon is less dense than the air outside the balloon. Therefore, the balloon experiences an upward buoyant force $(F_b)$. Simultaneously the weight $(W)$ of the balloon acts on vertically downward direction. $F_b=\rho_{out}Vg$ and $W=\rho_{in}Vg$ where, $V$ is the volume of the balloon. The resultant upward force acting on the balloon is $F=F_b-W$ or, $\rho_{in}Va=\rho_{out}Vg-\rho_{in}Vg$ where, $a$ is the upward acceleration of the balloon. or, $\rho_{in}a=\rho_{out}g-\rho_{in}g$ or, $a=(\frac{\rho_{out}}{\rho_{in}}-1)g$ Substituting the given values, we obtain $a=(1.39-1)\times9.81\; m/s^2$ or, $\boxed{a=3.826\;m/s^2}$ Therefore, the acceleration of the rising hot-air balloon is $3.826\;m/s^2$
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