Mass and Kinetic Energy

Topics: Mass, Classical mechanics, Energy Pages: 4 (965 words) Published: February 5, 2013
Disk With Weight:

A 15 kg uniform disk of radius R = 0.25 m has a string wrapped around it, and a m = 3 kg weight is hanging on the string. The system of the weight and disk is released from rest.

a) When the 3 kg weight is moving with a speed of 2.2 m/s, what is the kinetic energy of the entire system? KETOT= KEwheel+KEweight
= (1/2)(I)(w2)+(1/2)(m*v2)
=(0.5* v2)(m+1/2M)
=0.5*(2.2^2)*(3+(.5*15)) J

b) If the system started from rest, how far has the weight fallen? H = KETOT/MG
= 0.5*(2.2^2)*(3+(.5*15))/(3*9.8) m

c) What is the angular acceleration at this point?
Remember that a = αR, or α = a/R

Solve for acceleration by using vf2=vi2+2ax (vf=2.2, vi=0, x=(answer in part b)) That gives you the linear a… we want angular acceleration so we just divide our linear acceleration by the radius:


Sphere on Incline:

A solid sphere of uniform density starts from rest and rolls without slipping a distance of d = 3.7 m down a θ = 33° incline. The sphere has a mass M = 4.2 kg and a radius R = 0.28 m.

For this one, you have to do part © first… and don’t forget that ur working with a sphere, so u gotta look up the moment of inertia (I) in order to get the correct answer…

a) Of the total kinetic energy of the sphere, what fraction is translational? U just divide the translational found in part (b) by KEtotal ((1/2)mv2 + (1/2)Iω2) 0.71

b) What is the translational kinetic energy of the sphere when it reaches the bottom of the incline? (1/0.7)*9.8*(3.7sin(33))*.5*4.2

c) What is the translational speed of the sphere as it reaches the bottom of the ramp? You can find the velocity by using the conservation of energy theorem thing: KEi + Ui = KEf + Uf

h = d*sin(θ)
Mgh= KEtrans + KErot
= (1/2)mv2 + (1/2)Iω2
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