Tension in a String with Vertical Support | Physics Homework Solution

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The problem involves calculating the tension in a wire supporting a 45.0 kg ball against a vertical wall. The angle of the wire is determined to be approximately 19.471 degrees, leading to the use of the equation Cosθ = (m*g)/T to find tension. The calculated tension of 470.0 N raises questions, as it exceeds the weight of the ball, which seems counterintuitive. It is clarified that the vertical component of the tension must counterbalance the weight of the ball, necessitating a greater overall tension due to the angle. The discussion emphasizes the importance of understanding the dynamics of tension in angled supports.
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Homework Statement



A solid uniform 45.0 kg ball of radius 0.16 m is supported against a vertical, frictionless wall using a thin 0.30 m wire of negligible mass. Find the tension in the wire.

tension.png


Homework Equations



Sinθ = opposite/hypotenuse

Cosθ = (m*g)/T or T/(m*g); I'm not sure

The Attempt at a Solution



The angle is sin^(-1)(r/(r+0.30 m) = 19.471 degrees.

My textbook probably uses Cosθ = (m*g)/T to find the tension because that gives their answer OF 470.0 N. But, how can the force of the tension be greater than mg? I intuitively thought that maximum tension would be when θ = 0° and decrease to 0.00 N as θ goes to 90°.

This doesn't make any sense to me.
 
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If you will draw a free-body diagram, you will see that the vertical component of the tension must be equal and opposite of the weight of the ball. The wire is acting at an angle to the vertical, so the tension in the wire must be greater than the vertical component.

If you were to support the ball from the ceiling such that the string was at right angles to the ceiling, then the tension would equal the weight of the ball exactly.

If you were to suspend the ball from a wire running horizontally when it is not loaded, you would see that there is a large tension in the wire required to support even a small weight. This is why overhead power lines are susceptible to breaking if they ice up.
 
SteamKing said:
If you will draw a free-body diagram, you will see that the vertical component of the tension must be equal and opposite of the weight of the ball. The wire is acting at an angle to the vertical, so the tension in the wire must be greater than the vertical component.

If you were to support the ball from the ceiling such that the string was at right angles to the ceiling, then the tension would equal the weight of the ball exactly.

If you were to suspend the ball from a wire running horizontally when it is not loaded, you would see that there is a large tension in the wire required to support even a small weight. This is why overhead power lines are susceptible to breaking if they ice up.

Oh yeah, thanks!
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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