EDIT: This is the long way to do it... skip down to my 2nd post for a shorter more intuitive method. Understand the math in this explanation though because it can still be applied to other problems if need be...
OK... I made a couple pictures in Latex for you. If you understand how to do problem 281, then you can figure out 280:
Here is the problem (This answer is for 281, but again, 280 is done similarly):
OK the object is not swinging back and forth, it's not accelerating left to right, it's perfectly still. It is in equilibrium. This means that the component of the tension acting in the X direction for T1 (denoted by the red line for T1) cancels out the x component for T2 (not shown). This component is given by basic trig relationships as T1Cosθ1 and T2Cosθ
2 for T1 and T2 respectively. If you read EK, they go over this basic trig relationship ad nauseam. So now we have the following equation:
The components of the tension in the y direction also cancel. These are given by the T1, T2, and T3. T3 is simply the weight (mass* gravity). For problem 281, this is 1000 N. T3 acts downward, and partial components of T1 and T2 act upward. The component for T1 is represented by the blue line in the picture, and is given by T1Sinθ1 and T2Sinθ2 for T2 (not shown in the diagram). So now we get the following equation:
Now we have 2 equations and 2 unknowns. We can simply plug and chug. We simply need values for the angles as given by the following:
So now we plug these in and get the following for the x component:
(Here we can see that T1 = T2)