Doc Al said:
(1) Without being given the amount of sag, you cannot solve for the tension in the cable segments.
(2) Don't assume that the tension is constant throughout the cable--in fact it cannot be.
AnneP, this is way too much problem for a 12th grade math problem, so rest easy on that point.
I had previously said that cable tension is constant but Doc Al has pointed out that this cannot be. This is an interesting point. In many circumstances, such as when a load is transferred from one point to another over a cable, the load is applied to the cable through a pulley. Assuming that the load is moving slowly, so that the laws of statics apply (no acceleration), then the cable tension is the same on both sides of the pulley (as I suggested). The subtly in this situation is, however, that the downward load must have a side wise component; otherwise, the load will simply roll to the lowest point on the cable and stop there. To be in equilibrium at some place other than the lowest point, the downward force must actually be along the angle bisector between the two sides of the cable as they leave the pulley, thus creating a line of symmetry about the downward force vector. In short then, if the load is purely vertical, as it appears to be in this problem, then I was in error and Doc Al is correct; the tensions cannot be the same on the two sides of the load.
I hesitate to say, however, that the problem cannot be solved. One of the critical points is to understand that the connection point moves both downward and laterally. Let the long side be to the left and the short side be to the right of the load. Then denote the displacement of the load point as S downward and D to the right. The following additional notations are used:
TL = Load to the left
TR = Load to the right
LLo = original length on the left side = 6 m
LRo = original length on the right side = 4 m
W = applied load = 12 N
EL = elongation on the left
ER = elongation on the right
AE = product of cross sectional area with Young's modulus for the wire
The following equations are available:
Horiz Force Sum = - TL * (LLo+D)/sqrt((LLo+D)^2+S^2) + TR * (LRo-D)/sqrt((LRo-D)^2+S^2) = 0
Vert Force Sum = TL * S/sqrt((LLo+D)^2+S^2) + TR * S/sqrt((LRo-D)^2+S^2) = 0
EL = TL*LLo/AE = sqrt((LLo+D)^2+S^2) - LLo
ER = TR*LRo/AE = sqrt((LRo-D)^2+S^2) - LRo
It is necessary to specify AE because this describes the stiffness of the wire. A very high AE value will mean a very stiff wire and a very small deflection (small S, smaller D), whereas a lower value for AE will give larger values for both S and D.
Just as a matter of interest, I have run out solutions for this system of equations for the given information and using AE = 650309 N. The resulting tensions are only slightly different from each other:
TL = 223.99 N
TR = 224.05 N