Cable tension statics problem

In summary, one must use correct arithmetic and trigonometry to correctly solve for the tension in the given situations.
  • #1
Shay10825
338
0
1.) A uniform rod AB is 1.2 m long and weighs 16 N. It is suspended by vertical strings AC and BD. A block P weighing 96 N is attached at E, .3 m from A. The tension in the string BD is?
http://img116.exs.cx/img116/2822/STATICS1.jpg
I did:

(.3m)(96N)+ (.9m)(16N) - (1.2 m)(x) = 0
x=36N

But the answer is 32 N

What did I do wrong??

2.) A 960 N block is suspended as shown. The beam is weightless and is hinged to the watt at A. The tensions in the cable BC is?
http://img116.exs.cx/img116/364/statics2.jpg

I did:

(4m)(960N)=t
t=3840

The answer is 1600 N.

~Thanks
 
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  • #2
In your first answer, you got the arithmetic wrong - I used the same pivot point you did and got 32N.

In your second, you need to do a little trigonometry. The vertical component of the tension is 960N. Figure out what the total tension needs to be to get a vertical component of that magnitude. (Hint: you can get the angle at B with an Arctangent function.)
 
  • #3


In the first problem, you have correctly set up the equation for the sum of forces in the vertical direction. However, you have made a mistake in calculating the moment arm for the weight of the rod (16N). The moment arm should be 0.6m, not 0.9m. This gives you a final answer of 32N, which is the correct answer.

In the second problem, you have correctly set up the equation for the sum of moments about point A. However, you have not taken into account the weight of the beam itself. The weight of the beam creates a clockwise moment about point A, which needs to be subtracted from the total moment in order to find the tension in the cable. The correct equation should be:

(4m)(960N) - (2m)(x) - (2m)(160N) = 0

Solving for x gives you a tension of 1600N, which is the correct answer.
 

What is a cable tension statics problem?

A cable tension statics problem involves analyzing the forces acting on a cable system that is in a state of static equilibrium. This means that the forces acting on the cable are balanced, resulting in no movement or acceleration. These types of problems are commonly encountered in engineering and physics, particularly in structural design and construction.

What are the main factors that affect cable tension?

The main factors that affect cable tension are the weight of the cable, the load or weight that is being supported by the cable, and the angle at which the cable is being pulled. The length and material of the cable can also play a role in determining its tension.

How is cable tension calculated?

Cable tension can be calculated using the principles of statics and the laws of physics, specifically the equations for forces and moments. The tension in a cable is equal to the sum of the forces acting on it in the direction of the cable, and it can also be affected by the angle at which the forces are applied. It is important to consider all the forces acting on the cable, including external loads and any internal forces within the cable itself.

What are some common applications of cable tension statics problems?

Cable tension statics problems are commonly encountered in a variety of applications, including the design and construction of bridges, cranes, suspension systems, and other types of structures. They are also important in the analysis of cable and wire systems used in engineering and technology, such as power lines, elevator cables, and suspension cables for large structures.

What are some common challenges in solving cable tension statics problems?

Solving cable tension statics problems can be challenging due to the complexity of the cable system and the different factors that can affect tension. It is important to accurately determine all the forces acting on the cable and properly apply the equations for static equilibrium. Additionally, the material properties of the cable and its response to external loads may need to be taken into consideration for more accurate calculations.

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