Archived Centripetal Acceleration and string tension Question

AI Thread Summary
A 6.0 kg object is swung in a circle with a speed of 12 m/s, using two 5.0 m strings, leading to different tensions in the strings. The radius of the circular motion is determined to be 3 m, resulting in a centripetal acceleration of 48 m/s². The vertical tension components balance the weight of the object, while the horizontal components provide the necessary centripetal force. By solving the system of equations derived from the tension components, the tensions are found to be T1 = 276.75 N and T2 = 203.25 N. The difference in tension is attributed to the equilibrium of forces acting on the object in the vertical direction.
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Homework Statement


A 6.0kg object is attached to two 5.0m-long strings and swung around in a circle at 12 m/s. Determine the tension in the two strings, and explain why the tensions are not the same.

Given:
m=6.0kg
v=12m/s
length of string= 5.0m

Homework Equations



ƩF=m.a
ac=v^2/R

The Attempt at a Solution



There was a diagram that goes with the question but i couldn't simply draw it. Basically its a 8.0m pole with two 5.0 m strings attached to a 6.0kg ball. the strings and the pole form a isosceles triangle. I used the 3,4,5 triangle rule to find the radius which is 3, then ac=v^2/R to find the acceleration which came out to be 48m/s^2. After, used sin law to find angle between ball and radius. When i wrote my ƩF statement one came out to be ƩFy=Tasin37°-Tbsin37°-Fg other statement is ƩFx=Tacos37°+Tbcos37°. Is it possible to substitute these two equations eventhough they're acting in different directions?
 
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Diagram.gif


The radius found in the OP is right (3 m). The centripetal acceleration is also correct (48 m / s2). The OP uses symbols like Ta, Tb etc. and takes sin law, without giving a diagram, so I'll not comment on that part. I really do not understand, what he/she means by

"Is it possible to substitute these two equations eventhough they're acting in different directions?"Anyway, I'll use a Cartesian coordinate system rather than the sin law used in the OP.
The diagram is shown above.

We take the horizontal and vertical components of the two tensions T1 and T2 (see Fig. 2).
We first calculate sin(θ) and cos(θ) [Fig. 1]:
sin(θ) = 3 / 5 and cos(θ) = 4 / 5.

For the vertical components, because there is no motion on the vertical direction, we'll have:
T₁cos(θ) = T₂cos(θ) + mg, so: T1 - T2 = mg / cos(θ) = 6.0 x 9.8 / 0.8 ## kg \frac{m}{s^{2}}## = 73.5 N.

For the horizontal components of tension, we see that their sum is the centripetal force for the circular motion of the sphere.
So, T1 sin(θ) + T2 sin(θ) = m v2 / R , so, T1 + T2 = m v2 / R sin(θ) = 6.0 x 122 / 3 x 0.6 kgr (m/s)2 / m = 480 N.

Now, having T1 - T2 and T1 + T2 we solve the simple system of equations:
T1 - T2 = 73.5 N
T1 + T2 = 480 N

We get T1 = 276.75 N and T2 = 203.25 N.

We see that the tensions are not equal. This is explained, if we take into account the equilibrium on vertical axis (i.e. the weight of the sphere).
 
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