Particle sliding down a frictionless sphere

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SUMMARY

A particle of mass m slides down a frictionless sphere of radius R, starting from rest at the top. The kinetic energy of the particle can be expressed as K = mgy, where y is the height in terms of R and Θ. The centripetal acceleration is determined to be ar = g, while the tangential acceleration requires a more complex analysis involving the relationship between velocity and angle. The critical angle Θ at which the particle leaves the sphere needs to be derived from the forces acting on the particle, particularly the balance of gravitational and centripetal forces.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with concepts of kinetic and potential energy
  • Knowledge of centripetal acceleration
  • Ability to analyze motion in polar coordinates
NEXT STEPS
  • Derive the expression for velocity v as a function of angle Θ
  • Explore the relationship between radial and tangential components of forces
  • Investigate the conditions for a particle to leave a curved surface
  • Study the dynamics of particles in circular motion
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Students studying classical mechanics, physics educators, and anyone interested in the dynamics of particles on curved surfaces.

attilathedud
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Homework Statement


A particle of mass m slides down a fixed frictionless sphere of radius R starting from rest at the top.
a. In terms of m, g, R, and Θ, determine each of the following for the particle while it is sliding on the sphere.
i. The kinetic energy of the particle.
ii. The centripetal acceleration of the mass.
iii. The tangential acceleration of the mass.
b. Determine the value of Θ at which the particle leaves the sphere.

Homework Equations


None given.


The Attempt at a Solution


a.
i.
Ki + Vi = Kf + Vf
0 + mgy = 1/2mv^2 + 0
gy = 1/2v^2
g(R/2) = v^2/2
v = sqrt(gR)

ii.
ar = v^2 / R
ar = gR/R
ar = g

iii.
v = r(dΘ / dt)
sqrt(gR) = R(Θ/t)
gR = (R(Θ / t)) ^ 2
t = d/v
gR = (R(Θ / d / sqrt(gR))^2
gR = R(Θsqrt(gR)/d)^2

b. Pretty sure the fact I massively screwed up part iii is making this section impossible. And having the centripetal acceleration equal gravity seems incorrect as well.

Edit: Seems like I wasn't the first one to post this. My apologies.

The forum adds the template tags to the bottom of the current post every time you hit the "Preview Post" button...
 
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attilathedud said:
i.
Ki + Vi = Kf + Vf
0 + mgy = 1/2mv^2 + 0
gy = 1/2v^2
g(R/2) = v^2/2
v = sqrt(gR)
Using energy is the right approach, but you need to find an expression for ##v## as a function of ##\theta##. Don't set ##y## to a specific value as you did here. Instead, express it as a function of ##R## and ##\theta##.
attilathedud said:
ii.
ar = v^2 / R
ar = gR/R
ar = g
This part will work out once you fix part i.
attilathedud said:
iii.
v = r(dΘ / dt)
sqrt(gR) = R(Θ/t)
gR = (R(Θ / t)) ^ 2
t = d/v
gR = (R(Θ / d / sqrt(gR))^2
gR = R(Θsqrt(gR)/d)^2
It would be simpler to resolve the weight of the particle into radial and tangential components.

attilathedud said:
b. Pretty sure the fact I massively screwed up part iii is making this section impossible. And having the centripetal acceleration equal gravity seems incorrect as well.
How would you interpret "particle leaves sphere" in terms of the forces acting on the particle?
 

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