Solid Sphere Impulse: Find Velocity, Angular Velocity, & Kinetic Energy

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Homework Help Overview

The problem involves a uniform solid sphere that receives an impulse while floating in space. Participants are tasked with deriving formulas for the linear velocity, angular velocity, and total kinetic energy of the sphere as functions of its radius, mass, and the applied impulse.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between linear and angular velocities, questioning the meaning of the derived velocity formula and its relation to the center of mass. They explore the concepts of angular impulse and its connection to the impulse applied to the sphere.

Discussion Status

The discussion is ongoing, with participants providing insights into the relationships between linear momentum, angular momentum, and impulse. Some guidance has been offered regarding the interpretation of angular impulse and its implications for solving for angular velocity.

Contextual Notes

Participants express uncertainty about the validity of certain relationships, such as V = ωR, and the implications of the sphere being initially stationary. There is a focus on clarifying definitions and assumptions related to the problem setup.

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Homework Statement



A uniform solid sphere has radius R and mass M. It is initially at rest but is
free to move, floating in space with nothing touching it. It suddenly receives
an impulse J at a tangent to its surface.

As a function of R, M and J, find formulae for:

(a) the linear velocity of the sphere,
(b) its angular velocity around its centre of mass
(c) its total kinetic energy after the impulse.




Homework Equations


L=Iω,J=MV,V=ωR


The Attempt at a Solution



a) All particles on the sphere have the same angular velocity and different linear velocities depending on their distance from the centre.

J=ΔP=M(V-u)=MV so V=J/M Whose velocity is this ? ( V=J/M) .Is it the C.o.M ?

b) L=Iω <=> ω=L/I = 5L/(2MR2) But how can i move from here ?

c) well if i knew how to solve b) then c) is an easy one !
 
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ZxcvbnM2000 said:
a) All particles on the sphere have the same angular velocity and different linear velocities depending on their distance from the centre.

J=ΔP=M(V-u)=MV so V=J/M Whose velocity is this ? ( V=J/M) .Is it the C.o.M ?
Good. That's the velocity of the COM.

b) L=Iω <=> ω=L/I = 5L/(2MR2) But how can i move from here ?
What's the angular impulse?
 
ΔL=IΔω but since it was stationary at first then ΔL=Iω

It seems to be simple but i still can't understand how to relate these two :S
 
Last edited:
Actually no :S
 
ZxcvbnM2000 said:
ΔL=IΔω but since it was stationary at first then ΔL=Iω
Nothing wrong with that, but what is ΔL in terms of J?
 
Hmm dL=Iω=J*R=MVR but i realized that V=ωR is not valid , why is that ?
 
ZxcvbnM2000 said:
Hmm dL=Iω=J*R=MVR but i realized that V=ωR is not valid , why is that ?
The angular impulse is J*R. Now you can solve for ω.

As to whether V = ωR is valid, that depends on what you mean by V. (In any case, you don't need it here.)
 

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