Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 11 - Work - Exercises and Problems - Page 306: 60

Answer

a) $\rm \dfrac{N}{m^3}=\rm\dfrac{kg}{s^2.m^2}$ b) $U= \frac{1}{4}qx^4$ c) $10\;\rm m/s$

Work Step by Step

a) We need to solve the given formula for $q$ so we can find its units. $$F_x=-qx^3$$ Hence, $$q=\dfrac{-F_x}{x^3}$$ where the force is measured in Newtons and the distance is measured in meters. Thus, the units of $q$ are given by $$\rm\boxed{\rm \dfrac{N}{m^3}}=\dfrac{kg.m}{s^2.m^3}=\boxed{\rm\dfrac{kg}{s^2.m^2}}$$ ___________________________________________ b) To find a formula for the potential energy of the sprong, we need to recall that $$F_x=\dfrac{-dU}{dx}$$ Thus, $$dU=-F_xdx$$ $$\int_0^UdU=\int _{x_e}^x-F_xdx$$ Hence, $$ U=-\int _{x_e}^xF_xdx=-\int _{x_e}^x(-qx^3)dx$$ $$ U=q \int _{x_e}^x x^3dx=q\dfrac{x^4}{4}\bigg| _{x_e}^x$$ $$ U= \dfrac{q}{4}\left[x^4-x_e^4\right] $$ where $x_e=0$, so that $$ \boxed{U= \frac{1}{4}qx^4}$$ ___________________________________________ c) Since the barrel is frictionless, then the energy is conserved. This means that the elastic potential energy stored in the sprong will be completely converted to a kinetic energy. Thus, $$U_i=K_f$$ Plugging from the boxed formula above. $$\frac{1}{4}qx^4=\frac{1}{2}mv^2$$ Solving for $v$; $$v=\sqrt{\dfrac{\frac{1}{2}qx^4}{m}}=\sqrt{\dfrac{\frac{1}{2}q }{m}} x^2$$ Plugging the known; $$v=\sqrt{\dfrac{\frac{1}{2}(40000) }{20\times 10^{-3}}} \times 0.10^2=\color{red}{\bf 10}\;\rm m/s$$
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