This is from a practice exam, I've been sitting here thinking about it for over an hour and can't convince myself of an answer, or write down any relevant exact equations.
A bar of uniform density ρ, length L, and negligible width is suspended by two inextensible ropes of negligible mass.
The second rope is cut, what is the tension of the other rope shortly after cutting? What is the tension's rate of change?
I've been trying to work it out with numbers g=10m/s2, ρ=30kg/m and L=1m just to keep it simple. Obviously before the rope is cut the tension of both ropes is T1=T2=150N and after the bar falls down and is stationary, then T1=300N so there is some smooth function of the tension (I think). The angle between the first rope and the bar is 90deg and increases to 180deg, and the force due to gravity can be divided into normal and tangential forces. The normal force increases the angular momentum, and the normal force is a maximum the moment the rope is cut. I'm having trouble putting this all together, but I think I am on the right track. Thanks in advance.
edit: As stated below, this is the force of gravity components FN=ρLgSin(θ) and FT=−ρLgCos(θ)
I still have trouble applying angular momenta to this problem.
Answer
Assume horizontal Rod
Sum of forces equals acceleration of center of gravity
T−mg=m¨yC
Sum of moments about center of gravity equals mass moment of inertia times angular acceleration
TL2=I¨θ
As the bar rotates by a small angle θ the center of gravity height is found by y=−L2θ or by differentiating twice, ¨y=−L2¨θ
Together it all comes as
T=mg−mL2¨θTL2=(m12L2)¨θ
Solve the above for T and ¨θ. Hint the value does not have to be more than mg2.
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