Normal force on a mass sliding inside a hoop at 27 degrees

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Homework Statement

A mass M of 5.20E-1 kg slides inside a hoop of radius R=1.40 m with negligible friction. When M is at the top, it has a speed of 5.27 m/s. Calculate size of the force with which the M pushes on the hoop when M is at an angle of 27.0 degrees.

Picture attached at the bottom.


The attempt at a solution

E at the top of the circle should equal the energy at that particular part of the circle. So,

mg(2r) + (1/2)mvtop2 = mg(r-rcosθ) + (1/2)mv^2
m's cancel, so
g(2r) + (1/2)vtop2 = g(r-rcosθ) + (1/2)v^2
2(g(2r) + (1/2)vtop2 - g(r-rcosθ) = v^2

a = v^2/r

F = ma


When I plug everything in, I get
2(39.831) = v^2
v^2 = 79.66

a = 79.66/1.4
a = 56.90

F = (.52)(56.90)
F = 29.59 N

This answer is incorrect.

Please, can someone let me know where I'm going wrong?
 
Attachments
  • Free-body diagram of a small block sliding on the inside of a circular hoop, with a dashed vertical radius from the centre down to the bottom and a dashed line at angle θ from the vertical, and an arrow showing the direction of motion along the hoop.
    prob25_1015hoop2.gif
    1,008 bytes · Views: 705
Last edited:
You've calculated the force due to the circular motion, but what other force is also working on the mass?
 
gneill said:
You've calculated the force due to the circular motion, but what other force is also working on the mass?

Okay. I'm forgetting the force of gravity acting on the mass, aren't I?

Should I add mgcosθ to my answer? Is that all I'm missing?
 
Becca93 said:
Okay. I'm forgetting the force of gravity acting on the mass, aren't I?

Should I add mgcosθ to my answer? Is that all I'm missing?

That looks right. Since the hoop has "negligible friction", only the component of the force due to gravity that is normal to the hoop's surface should matter -- the other component acts to accelerate the mass tangentially.