Engineering Mechanics: Statics & Dynamics (14th Edition)

Published by Pearson
ISBN 10: 0133915425
ISBN 13: 978-0-13391-542-6

Chapter 2 - Force Vectors - Section 2.4 - Addition of a System of Coplanar Forces - Problems - Page 42: 50

Answer

$\vec {F_1}=(9.64\hat i+11.49\hat j)\;kN$ $\vec {F_2}=(-24\hat i+10\hat j)\;kN$ $\vec {F_3}=(31.18\hat i-18\hat j)\;kN$

Work Step by Step

First, we resolve each force into its $x$ and $y$ components by using the parallelogram law: Let $F_{1x}$ and $F_{1y}$ are the $x$ and $y$ components of $\vec {F_1}$ force, in which $F_1=15\;kN$. Thus we have $F_{1x}=15\sin40^\circ\;kN\approx 9.64\;kN$ $F_{1y}=15\cos40^\circ\;kN\approx 11.49\;kN$ Let $F_{2x}$ and $F_{2y}$ are the $x$ and $y$ components of $\vec {F_2}$ force, in which $F_2=26\;kN$. Using proportional parts of similar triangles and considering the directions, we have $\frac{F_{2x}}{26\;kN}=-\frac{12}{13}$ or, $F_{2x}=-26\;kN\Big(\frac{12}{13}\Big)=-24\;kN$ Similarly, $\frac{F_{2y}}{26\;kN}=\frac{5}{13}$ or, $F_{2y}=26\;kN\Big(\frac{5}{13}\Big)=10\;kN$ Let $F_{3x}$ and $F_{3y}$ are the $x$ and $y$ components of $\vec {F_3}$ force, in which $F_3=36\;kN$. Thus we have $F_{3x}=36\cos30^\circ\;kN\approx 31.18\;kN$ $F_{3y}=-36\sin30^\circ\;kN\approx -18\;kN$ Having determined the magnitudes and directions of the components of each force, we can express each force as a Cartesian vector. $\vec {F_1}=(9.64\hat i+11.49\hat j)\;kN$ $\vec {F_2}=(-24\hat i+10\hat j)\;kN$ $\vec {F_3}=(31.18\hat i-18\hat j)\;kN$ where $\hat i$ and $\hat j$ are the unit vectors along positive $x$ and $y$ axes.
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