Calculate Angle of 3.50 kg Mass on 1.59 m String Revolving at 2.99 m/s

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A 3.50 kg mass suspended from a 1.59 m string revolves horizontally at a speed of 2.99 m/s, and the goal is to calculate the angle between the string and the vertical. The centripetal acceleration is expressed as a_c = v^2/r, and the forces acting on the mass are analyzed using tension components. The discussion highlights the need to derive a quadratic equation to solve for the angle θ, with suggestions to express tan(θ) in terms of known quantities and to isolate trigonometric functions. Various methods are proposed, including rewriting equations and substituting variables to ultimately derive the angle. The final solution yields an angle of approximately 41.1°.
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Homework Statement


A mass of 3.50 kg is suspended from a 1.59 m long string. It revolves in a horizontal circle as shown in the figure.
The tangential speed of the mass is 2.99 m/s. Calculate the angle between the string and the vertical.

Homework Equations


a_c = v^2/r
F = m*a_c
tanθ=sinθ/cosθ
sin^2θ=1-cos^2θ

The Attempt at a Solution


Vertical: T*cos(θ)-m*g=0 → T=(m*g)/cos(θ)
Horizontal: T*sin(θ) = m*a_c
Combined the two: ((m*g)/cos(θ))sin(θ)=m*a_c → m*g*tan(θ)=m*a_c → g*tan(θ)=a_c
we know that a_c=v^2/r, plug that into get g*tan(θ)=v^2/r
r=L*sin(θ) → g*tan(θ)=v^2/(L*sin(θ))

I cannot get past this point and the notes on the problem say that a quadratic equation needs to be solved at some point.
 

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gummybeargirl said:

Homework Statement


A mass of 3.50 kg is suspended from a 1.59 m long string. It revolves in a horizontal circle as shown in the figure.
The tangential speed of the mass is 2.99 m/s. Calculate the angle between the string and the vertical.

Homework Equations


a_c = v^2/r
F = m*a_c
tanθ=sinθ/cosθ
sin^2θ=1-cos^2θ

The Attempt at a Solution


Vertical: T*cos(θ)-m*g=0 → T=(m*g)/cos(θ)
Horizontal: T*sin(θ) = m*a_c
Combined the two: ((m*g)/cos(θ))sin(θ)=m*a_c → m*g*tan(θ)=m*a_c → g*tan(θ)=a_c
we know that a_c=v^2/r, plug that into get g*tan(θ)=v^2/r
r=L*sin(θ) → g*tan(θ)=v^2/(L*sin(θ))

I cannot get past this point and the notes on the problem say that a quadratic equation needs to be solved at some point.

You wrote r in terms of θ and proceeded to try to solve for θ. It left to a bit of a dead end, so now try to solve for r

See if you can write tan(θ) in terms of known quantites and r (it can be done) then you'll be able to solve it
 
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Good work so far. Continue from your last equation. Try isolating the trig functions on one side of the equation and all the constants on the other side. Let x = cosθ and see if you can get a quadratic equation in x.
 
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TSny said:
Good work so far. Continue from your last equation. Try isolating the trig functions on one side of the equation and all the constants on the other side. Let x = cosθ and see if you can get a quadratic equation in x.

I don't think that will work. The equation becomes:

\frac{v^{2}}{gL}=\frac{sin^{2}(θ)}{cos(θ)}There is another way to solve for θ (involving the quadratic equation) if you solve for r and then use r to find θ (once you know r, θ is trivial)EDIT: actually you're right you could solve it that way... (solution removed) sorry about that you are correct
 
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Nathanael said:
I don't think that will work. The equation becomes:

\frac{v^{2}}{gL}=\frac{sin^{2}(θ)}{cos(θ)}

I understand where this equation comes from, but I am not sure how you would go about solving that for θ.

Nathaneal said:
There is another way to solve for θ (involving the quadratic equation) if you solve for r and then use r to find θ (once you know r, θ is trivial)

I don't understand at all what I would use to solve for r or how this would result in a quadratic equation.
I am struggling with every aspect of this problem.
 
Nevermind! I figured it out, thank you all so much for you guidance in this problem.
 
I know you said you figured it out now, but I'll still show you the other methods.

gummybeargirl said:
I understand where this equation comes from, but I am not sure how you would go about solving that for θ.
You could rewrite sin^2(θ) as 1-cos^2(θ) (from pythagorean theorem) and then the equation becomes:
\frac{v^2}{gL}=\frac{1-cos^2(θ)}{cos(θ)}=\frac{1}{cos(θ)}-cos(θ)
Multiply both sides by cos(θ) and rearrange and you'll get a quadratic equation (with x=cos(θ)) which can be solved for cos(θ):
cos^2(θ)+\frac{v^2}{gL}cos(θ)-1=0
There will only be one root with an absolute value of less than one, so simply take the arccosine of it and you'll have θ
gummybeargirl said:
I don't understand at all what I would use to solve for r or how this would result in a quadratic equation.
You had written the equation g*tan(θ)=\frac{v^2}{r}
Since L^2=r^2+y^2 (where y is the unknown side of the triangle) you could use the equation L^2=r^2+(r*cot(θ))^2
(... r*cot(θ) is the unknown side ...) to rewrite tan(θ) as \sqrt{\frac{r^2}{L^2-r^2}}
Plug that expression into the "tan(θ)" part of your expression (and then square both sides and rearrange) and you'll get a quadratic equation (with x=r^2) which you can solve for r^2
The quadratic equation would be:
g^2r^4+v^4r^2-v^4L^2=0
There will be only 1 positive root, so take the square root of that to find r, then take the arcsin of (r/L) to find θUsing either method, you'll find θ=41.1° (I double checked)
 
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