The problem is as follows:
A cable goes across points A and B such that the bar will not slide as indicated in the figure from below. The mass of the bar is $2.5\,kg$. Assuming that the surface has no friction, find the tension on the wire so that the system remains in mechanical equilibrium.
The alternatives given in my book are as follows:
$\begin{array}{ll} 1.&12\,N\\ 2.&10\,N\\ 3.&14\,N\\ 4.&16\,N\\ 5.&18\,N\\ \end{array}$
What I attempted to do to solve this problem was to put the reaction force due the weight on the midpoint and using the point on $C$ as rotation axis. Therefore taking the distance for each force to that point.
Because the Normal force is not given I assumed that it was the resultant from the weight and the wire pulling to the wall as indicated in the diagram. Considering the direction of such force I did the following:
$N=w\sin 53^{\circ}+T\sin 37^{\circ}$
Then:
$-5N+10\left(T\sin37^{\circ}\right)+5\left(w\sin 53^{\circ}\right)=0$
$-5\left(w\sin 53^{\circ}+10T\sin 37^{\circ}\right)+5\left(w\sin 53^{\circ}\right)=0$
$-5\frac{4w}{5}-5\frac{3T}{5}+10T\frac{3}{5}+5\frac{4w}{5}=0$
Because $w= 2.5 \times 10 = 25$
The preceding equation would become into:
$-4 \times 25 - 3T + 6T + 4 \times 25 =0$
$3T=0$
$T= 0\,N$
Therefore I end up obtaining a zero force for the tension. What could I be doing wrong?. Can somebody help me with the appropiate calculation for the tension using my approach?.


With A as the pivot point, establish the equilibrium equations below,
$$T = N\cos 53,\>\>\>\>\>N = mg \sin 53$$
to obtain the tension
$$T = mg \cdot\cos 53\cdot\sin 53 = (2.5\times10)\cdot \frac 35\cdot\frac45 = 12N$$