A nonuniform bar is suspended at rest in a horizontal position by two massless cords as shown. One cord makes the angle θ = 36.9° with the vertical; the other makes the angle \(\phi\) = 53.1° with the vertical. If the length L of the bar is 6.10 m, compute the distance x from the left end of the bar to its center of mass.
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I'm not sure @Michele_Laino
Net force = 0:\[T_1 \cos \theta + T_2 \cos \phi=mg\]\[T_1 \sin \theta = T_2 \sin \phi\]Net torque about any point is zero. I'm going to take that point as the center of mass.\[T_1 \cos \theta(x) = T_2 \cos \phi (L-x)\]
And 37-53-90 are the angles of the 3-4-5 (or similar derivative) triangles.
so from first equations, i suppose, we have T1 and T2
Yeah, and then we plug and play those values in the equation for torque.
Awesome! let me plugin the numbers... it feels nice to see the textbook answer match with mine
Which textbook is this?
Hey, we don't know mass of the rod ?
Net force = 0:\[T_1 \cos \theta + T_2 \cos \phi=\color{red}{m}g\]\[T_1 \sin \theta = T_2 \sin \phi\]
You're right... this is not as straightforward as I thought. If we try to calculate net torque about other points, maybe it's possible.\[T_2 \cos \phi (L) = mg(x)\]\[T_1 \cos \theta (L) = mg(L-x)\]Again, dunno if anything changes.
Ah lol, I have a copy. Never opened the question bank.
it is a good book at the moment, i am reviewing Chapter 12 Equilibrium and Elasticity
I think we can express both T1 and T2 in terms of m, then plug it in the third eqn
Haha, well, it works.\[mg =\left(\cos \phi + \cot \theta \sin \phi \right) T_2 \]
\[\frac{mg}{T_2} = \frac{L\cos \phi }{x}\]
\[x = \frac{L\cos \phi}{ \cos \phi + \cot \theta \sin \phi }\]
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