Zondrina said:
Sounds good. I'll solve without components and compare the answers.
##F_R = \sqrt{\vec{F}_1^2 + \vec{F}_2^2 - 2\vec{F}_1\vec{F}_2 cos(55°)} = 31.13N## same answer as the component hypotenuse calculation.
Using the sine law I get :
##\frac{sin(55°)}{31.13N} = \frac{sin(θ)}{22N}##
??
##θ = 35.37°##??
It seems to be more than a whole degree off from my other answer.
Again, I highly recommend moving away from the law of cosines and law of sines, and instead simply use the vector components. More on that later. But for the moment, let me correct a mistake you made with the law of sines. Your method
will work, but it's much easier to make mistakes compared to working with components.
Take a look at the original diagram. In your mind (or better yet, on paper), move the 38.0 N vector up so that its tail meets the head of the 22.0 N vector. Then we can connect the tail of the 22.0 N vector with the head of the 38.0 N vector to find the resultant force. We know that the magnitude of that vector is 31.1284468 N. (I calculated with more precision.)
We know the angle opposite the resultant vector, in this new triangle is 55
o. This is the top angle in the new triangle. But what we don't know is the bottom left angle in this new triangle. But we do know the opposite of that angle is the 38.0 N vector, not the 22.0 N vector, and this angle is relative to North.
\frac{\sin 55}{31.1284468} = \frac{\sin \theta}{38.0}
So \theta = 89.624326^o. But that's East of North. If we want to express that as North of East, we have to subtract it from 90 degrees.
90
o - 89.624326
o = ~0.376
o, North of East.
[Edit: And the only reason this is easy at all is because one of the original vectors was already pointing due North. If both of the original vectors were at arbitrary angles, the best you could do using the law of sines or law of cosines is find the angle relative so some other arbitrary angle. That adds even more steps in the process to the final solution.]
But it's so much easier and saves time by just working from components from the beginning.
You know that \sin \theta = \frac{\mathrm{opposite}}{\mathrm{hypotenuse}}
You know that \cos \theta = \frac{\mathrm{adjacent}}{\mathrm{hypotenuse}}
You know that \tan \theta = \frac{\mathrm{opposite}}{\mathrm{adjacent}}
And since you already broken everything down into its x- and y- components,
y-component = opposite
x=component = adjacent
magnitude of resultant = hypotenuse