Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 10 - Fluids - Problems - Page 287: 32

Answer

(a) The density of the liquid is $1.21\times 10^3~kg/m^3$ (b) $\rho = \frac{(M-M_a)~\rho_o}{M}$

Work Step by Step

(a) Let $M$ be the mass of the aluminum. Let $\rho_a$ be the density of aluminum. We can find the volume $V$ of the aluminum as: $V = \frac{M}{\rho_a}$ $V = \frac{3.80~kg}{2.70\times 10^3~kg/m^3}$ $V = 1.41\times 10^{-3}~m^3$ Let $M_a$ be the apparent mass of the aluminum. Let $\rho$ be the density of the liquid. Note that the apparent weight is equal to the true weight of the aluminum minus the buoyant force provided by the liquid. Therefore; $M_a~g = M~g-F_B$ $F_B = M~g-M_a~g$ $\rho~V~g = M~g-M_a~g$ $\rho = \frac{M-M_a}{V}$ $\rho = \frac{3.80~kg-2.10~kg}{1.41\times 10^{-3}~m^3}$ $\rho = 1.21\times 10^3~kg/m^3$ The density of the liquid is $1.21\times 10^3~kg/m^3$. (b) Let $M$ be the mass of the object and let $M_a$ be the apparent mass. Let $\rho_o$ be the density of the object. Let $\rho$ be the density of the liquid. $M_a~g = M~g-F_B$ $F_B = M~g-M_a~g$ $\rho~V~g = M~g-M_a~g$ $\rho = \frac{M-M_a}{V}$ $\rho = \frac{M-M_a}{\frac{M}{\rho_o}}$ $\rho = \frac{(M-M_a)~\rho_o}{M}$
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