gracedescent said:
Correct, out of the scope. I only need the accelration. Only problem, I totally agree with your remark on the normal force. But you need a mass to figure out this. In this case the skiers mass and force is omitted. I only was given the initial velocity, kinetic coefficient, and angle of descent.
n = mgcos
and this Fg opposite to the friction?
well, this = mgsin
However, note that in the above the mass drops out.
Ergo, why I thought that the equation would be:
s= vi2/2gsin[tex]\Theta[/tex]uk
Then again... mgsin[tex]\Theta[/tex] - ffk = max=ma
So, a = gsin[tex]\Theta[/tex]-ffk
Correct?
So,
s= vi2/2gsin-ffk
I think... maybe not, still.
If I do not have the mass where as g is constant I am stuck, right?
The mass is irrelevant. You are only asked about velocities and accelerations. As all of your accelerations are tied into the gravitational acceleration, which is uniform regardless of mass, you can use a rearranged form of Newton's second law to find the acceleration.
[tex]\vec a=\frac{\vec F}{m}[/tex]
Also, you have a mistake in your very final line.
Starting from [tex]v_f^2=v_0^2+2ad[/tex]
Isolating [tex]d[/tex] provides us with:
[tex]d=\frac{v_f^2-v_0^2}{2a}[/tex]
Our final velocity is 0, since we're looking for the stopping distance, and the net acceleration of the mass can be found using Newton's second law:
[tex]\vec a=\frac{\vec F}{m}[/tex]
The net force in the direction of the slope is, as you've found:
[tex]\Sigma \vec F=mg\sin{\theta}-F_{friction}[/tex]
[tex]\Sigma \vec F=mg\sin{\theta}-\mu_k*N[/tex]
Find [tex]N[/tex], and the problem should become trivial.
Try drawing an FBD, and everything should become clear. Break gravity down into its components, and remember that the mass is at equilibrium in the direction perpendicular to the slope.