Calculus (3rd Edition)

Published by W. H. Freeman
ISBN 10: 1464125260
ISBN 13: 978-1-46412-526-3

Chapter 13 - Vector Geometry - 13.1 Vectors in the Plane - Exercises - Page 651: 63

Answer

Magnitude of the force on cable 1 and cable 2 (respectively): ${F_1} \simeq 453.154$ N ${F_2} \simeq 211.309$ N

Work Step by Step

Let the gravitational acceleration be $g=10$ $m/s^2$. So, the gravitational force on the mass is ${\bf{W}} = - 500{\bf{j}}$ N. Let the forces that act on the mass be denoted by ${{\bf{F}}_1}$ and ${{\bf{F}}_2}$, respectively. By Newton's third law, the forces on cables 1 and 2 are the same magnitude but in opposite directions. So, we have ${{\bf{F}}_1} = - {F_1}\cos 65^\circ {\bf{i}} + {F_1}\sin 65^\circ {\bf{j}}$, ${{\bf{F}}_2} = {F_2}\cos 25^\circ {\bf{i}} + {F_2}\sin 25^\circ {\bf{j}}$, where ${F_1} = ||{{\bf{F}}_1}||$ and ${F_2} = ||{{\bf{F}}_2}||$. Since the system is in equilibrium, by Newton's first law, the total net force is zero. Thus, $\sum {\bf{F}} = {\bf{0}} = {\bf{W}} + {{\bf{F}}_1} + {{\bf{F}}_2} = {\bf{0}}$ So, the components of the total net forces are $ - {F_1}\cos 65^\circ + {F_2}\cos 25^\circ = 0$ $ - 500 + {F_1}\sin 65^\circ + {F_2}\sin 25^\circ = 0$ So, ${F_2} = {F_1}\frac{{\cos 65^\circ }}{{\cos 25^\circ }}$. Substituting this in the last equation above gives $ - 500 + {F_1}\sin 65^\circ + {F_1}\frac{{\cos 65^\circ }}{{\cos 25^\circ }}\sin 25^\circ = 0$ Solving this equation gives ${F_1} \simeq 453.154$ N and ${F_2} = {F_1}\frac{{\cos 65^\circ }}{{\cos 25^\circ }} = 376.244\frac{{\cos 65^\circ }}{{\cos 25^\circ }} \simeq 211.309$ N.
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.