A man is attempting to raise a 7.5-m-long,
![A man is attempting to raise a 75mlong class=](https://us-static.z-dn.net/files/d43/293418a66fa7b3a6780b655b789576c9.png)
Answer:
[tex]397.44\text{ N}}[/tex] or approximately [tex]4.0\cdot 10^2\text{ N}[/tex] to two significant figures
Explanation:
Question (clarified by question poster): "With what force does the man have to pull on the rope to hold the pole motionless in this position?"
A FBD helps with identifying the forces on the pole. Call the axis parallel to the pole the x-axis. Directly perpendicular to this is the y-axis.
The force of gravity will act on the center of pole, directly down with a force of [tex]F_g[/tex]. Using basic. trig for a right triangle, the vertical component of that force is [tex]F_g\cos 30^{\circ}[/tex], in the y-direction. At the very end of the pole where the string is attached, however, the pole is creating a torque, given by [tex]\tau =rF\cos\theta[/tex]. In this case, [tex]r=3.75[/tex] (distance from center of pole to the end) and [tex]\theta = 30^{\circ}[/tex], so the torque from the pole is [tex]3.75\cdot F_g\cos 30^{\circ}[/tex].
Also in the y-direction is the vertical component of tension, [tex]T[/tex]. From right triangle trigonometry, the vertical component of the tension in the rope is [tex]T\sin 20^{\circ}[/tex]. Because the rope is also creating a torque of [tex]r=7.5[/tex] (length of pole), the force is [tex]7.5\cdot T\sin 20^{\circ}[/tex]
From Newton's 2nd Law:
[tex]\displaystyle \sum F_y=ma_y[/tex]
Since we're finding the force required to keep the pole motionless, there should be no acceleration in the y-direction. Therefore, [tex]\displaystyle \sum F_y=ma_y=0[/tex]:
[tex]\displaystyle \sum F_y=7.5T\sin20^{\circ}-3.75F_g\cos 30^{\circ}=0,\\\\7.5T\sin20^{\circ}=3.75F_g\cos 20^{\circ},\\\\T=\frac{3.75F_g\cos20^{\circ}}{7.5\sin 20^{\circ}}[/tex]
[tex]F_g=m_{pole}g=32\cdot 9.81=313.92[/tex]
Therefore,
[tex]\displaystyle T=\frac{313.92\cos30^{\circ}}{2\sin20^{\circ}}=\boxed{397.44\text{ N}}}[/tex]