jakecar said:
Ok I got the right answers using those equations for the forces in the x and y directions but how did you get those equations? I can't figure it out... Thanks!
Sum up the forces.
When the chandelier is displaced 0.1m, the 4m rope is at some angle.
The forces acting on the chandelier can be broken into those along the x-axis and those along the y-axis.
Picture a right triangle. The hypotenuse is the rope and it's 4m long. The vertical side is where the rope would be if it were hanging straight down. And the base, or horizontal side, is 0.1m.
I'm assuming that the chandelier is not swinging or moving; just that there is a force acting on it to displace it 0.1m, and keep it there.
That force is denoted by F_x.
There has to be another force horizontally to counteract F_x, otherwise the mass would accelerate. The only other forces are the weight, which is mg, and the tension in the 4m rope, which is T.
mg is perpendicular to F_x. But T is at an angle \theta, which can be determined by the dimensions of the triangle.
Since T is at an angle, it has both an x- and a y-component.
T's x-component is Tsin(\theta), and the x-component is Tcos(\theta).
So now we have two forces along the y-axis, and two forces along the x-axis. Since the mass is stationary, the forces have to be equal.
y-axis: Tcos(\theta)=mg
x-axis: Tsin(\theta)=F_x
Solve for F_x
Dividing one equation by the other gives:
mgtan(\theta)=F_x