PhDorBust
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A garden roller with external radius a is pulled along a rough horizontal path by force F which acts at a point on its axle and is inclined at an angle alpha with the horizontal.
Given that resultant force is at a right angle to F, what is the acceleration of the roller? Express in terms of radius a, alpha, and radius of gyration k.
My set-up (and failure):
Let H be resultant force, f_s is frictional force
Forces in x-dir:
Hsin( \alpha) = Fcos( \alpha) - f_s
Forces in y-dir:
-Hcos( \alpha) = Fsin( \alpha) - mg
Rotational equation of motion:
af_s = \frac{mk^2}{a} \ddot{x}
Assume no slipping:
\ddot{x} = a \ddot{ \theta}
Solve for x-acceleration:
\ddot{x} = \frac{a^2 F - a^2 mgsin( \alpha)}{mk^2 cos( \alpha)}
Correct answer:
\ddot{x} = \frac{ga^2 sin( \alpha) cos( \alpha)}{k^2 + a^2 sin^2 (\alpha)}
Where am I going wrong? I don't see why F isn't in the answer...
Given that resultant force is at a right angle to F, what is the acceleration of the roller? Express in terms of radius a, alpha, and radius of gyration k.
My set-up (and failure):
Let H be resultant force, f_s is frictional force
Forces in x-dir:
Hsin( \alpha) = Fcos( \alpha) - f_s
Forces in y-dir:
-Hcos( \alpha) = Fsin( \alpha) - mg
Rotational equation of motion:
af_s = \frac{mk^2}{a} \ddot{x}
Assume no slipping:
\ddot{x} = a \ddot{ \theta}
Solve for x-acceleration:
\ddot{x} = \frac{a^2 F - a^2 mgsin( \alpha)}{mk^2 cos( \alpha)}
Correct answer:
\ddot{x} = \frac{ga^2 sin( \alpha) cos( \alpha)}{k^2 + a^2 sin^2 (\alpha)}
Where am I going wrong? I don't see why F isn't in the answer...