matineesuxxx
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Homework Statement
Assuming we know the length of the string L, radius of the swept out circle r, angle formed by string and centre of circle, \theta, and angle the swept out circle is to the horizontal, \alpha, what is the speed, v, of the mass if it is constant?
picture: http://upload.wikimedia.org/wikipedia/commons/5/53/Conical_pendulum.svg
Homework Equations
\text{F}_{\text{net}}=ma
a=\frac{v^2}{r}
The Attempt at a Solution
So in trying to solve this, I broke it down into x and y components and in the horizontal plane, I got:
\text{F}_{\text{net}} = \text{T}\,\sin(\theta + \alpha)
ma_{x} = m(a\cos \alpha) = \text{T}\, \sin (\theta + \alpha)
\implies \text{T} = \frac{ma\cos \alpha}{\sin(\theta + \alpha)}
The angle, \theta + \alpha arrises due to some geometry where if i tilt my axis so that \text{F}_{g} points directly down on the negative y-axis and \text{T} points into the first quadrant, the angle from the positive x-axis is \frac{\pi}{2}-(\theta + \alpha)
and for the vertical plane i get:
\text{F}_{\text{net}} = \text{T}\cos (\theta + \alpha) - mg
ma_{y} = m(a\sin \alpha) = \text{T} \cos (\alpha + \theta) - mg
and substituting \text{T} into our equation I get;
a\sin \alpha = \frac{a \cos \alpha}{\sin (\theta + \alpha)} \cos (\theta + \alpha) - g
since a = \frac{v^2}{r}, I substitute and isolate for v^2 to get
v^2 = \frac{gL\sin (\theta) \sin (\theta + \alpha)}{\cos (\theta + 2\alpha)}
I am just wondering if I did this properly? I mean if I let \alpha = 0, then I end up with
v = \sin \theta \sqrt{\frac{gL}{\cos \theta}}, which is what I got when I was working with a normal conical pendulum, however, I feel that as the mass starts to approach the ground then it should speed up. Is it even possible to let v be constant and is my approach correct?