Finding the Tensions using the sum of moments

In summary, the problem involves finding the tensions in cables BD and BE in order to achieve a zero couple exerted on the tower by the fixed support at point A. This can be solved by taking the sum of the moments about point A, where the moment about A from each cable tension is the x component multiplied by the distance from A to the point of application. This results in two equilibrium equations, which can be solved using the substitution method to find the x and z components of the unknown cable tensions. Additional geometry and trigonometry will then be needed to determine the cable tensions in the guys.
  • #1
Isimanica
15
0

Homework Statement


The tower is 70 m tall. If the tension in cable BC is
2 kN, and you want to adjust the tensions in cable
BD and BE so that the couple exerted on the tower
by the fixed support at A is zero.

A) Determine the tensions in cable BD and BE
by applying the sum of the moments about
point A .

The Coordinates in meters
B(0,70,0)
A(0,0,0)
C(-50,0,0)
D(20,0,50)
E(40,0,-40)



Homework Equations



M=Fd

The Attempt at a Solution



Well I know that I have to solve by taking the sum of the moments about A. That means that the Moment about A of Tension BC + Moment about A of Tension BD + Moment about A of Tension BE = 0
and The moment about A of Tension BC is nothing more than the Fx of Tension BC about the distance from point A to B. So That means I find the angle that Tension BC makes to the tower get my Fx and times it by the tower distance. So now what do I need to do next. Looking for the next step.
 
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  • #2
You are correct so far. Note that the moment about A from the cable tension BC is about the z axis (the axis into the plane), that is, M_z (from the force BC) is (F_x)(y). Also note that for equilibrium, the sum of all moments M_z from all the cable forces must be 0, and the sum of all moments M_x from all the cable forces about the x-axis must be zero. In general, M_z = F_x(y) + (F_y)(x), and M_x = (F_y)z + F_z(y), (and M_y = F_x(z) + F_z(x), which you don't need in this problem, since x and z are 0). So just determine those F_x and F_z components of each cable force, and solve the resulting equilibrium equations for the unknown values.
 
  • #3
So what I need to do to find the Tensions of BE and BD I need to set up the Tension times the Perpendicular distance to point A?
Do I need to take the tensions and place them as if they are only in the x-z plane?
I guess what I am trying to figure out is how do I need to go about to get the distance relative to the tensions?
I can see that I have two equations from M about the z axis and M about the x axis. Requiring the use of the substitution method of one of the moments above.
 
  • #4
Isimanica said:
So what I need to do to find the Tensions of BE and BD I need to set up the Tension times the Perpendicular distance to point A?
Do I need to take the tensions and place them as if they are only in the x-z plane?
I guess what I am trying to figure out is how do I need to go about to get the distance relative to the tensions?
I can see that I have two equations from M about the z axis and M about the x axis. Requiring the use of the substitution method of one of the moments above.
Yes, that's a good way of doing it. Look at the guyed tower in a plan view from the top. Each cable tension BE and BD will have an x and z component, which are geometrically/trigonometrically related. The equations will simplify a bit since the x and z lever arms are 0. When you solve the simultaneous equilibrium of moments equations, you'll get the x and z components of the unknown cable tensions. Then you'll have to use more geometry/trig to get the cable tensions in the guys. It's kind of tough to keep it straight. And watch your plus and minus signs.
 
  • #5


I would suggest that you first draw a free body diagram of the tower to visualize the forces acting on it. This will help you determine the direction of each tension and the distances involved. Then, you can use the equation M=Fd to calculate the moment about point A for each tension. Since the net moment should be zero, you can set up an equation with the moments and solve for the tensions in BD and BE. Additionally, you can also use the equations for equilibrium (ΣF=0) to check your solution. It is important to double check your calculations and make sure they make sense in the context of the problem.
 

1. What is "Finding the Tensions using the sum of moments"?

"Finding the Tensions using the sum of moments" is a method used in physics and engineering to calculate the tensions in a system of connected objects or structures by using the principle of moments.

2. How does the sum of moments method work?

The sum of moments method involves using the principle of moments, which states that the sum of all forces acting on an object must equal zero in order for the object to be in equilibrium. By setting up equations of moments for each object in the system, the tensions can be solved for using algebraic manipulation.

3. What are the key assumptions made when using the sum of moments method?

The key assumptions made when using the sum of moments method include: the objects in the system are in static equilibrium, the forces acting on the objects are coplanar (lie in the same plane), and the objects are connected by rigid, massless strings or rods.

4. When is the sum of moments method most useful?

The sum of moments method is most useful when dealing with systems that have multiple objects connected by strings or rods, as it allows for the calculation of individual tensions in each string or rod. It is also useful in situations where the forces acting on an object are not known, but the resulting moments can be measured or calculated.

5. Are there any limitations to the sum of moments method?

Yes, the sum of moments method has some limitations. It is only applicable to systems in static equilibrium, and it assumes that the objects in the system are connected by rigid, massless strings or rods. Additionally, it does not take into account any external forces acting on the system, such as friction or air resistance.

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