Answer 2nd Question Part 1: Mechanics Ques.

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The discussion focuses on solving a mechanics problem involving a sphere and a platform, emphasizing the need for correct equations to account for their interactions. Participants confirm the use of equations related to friction, acceleration, and moment of inertia, while clarifying that the sphere rolls backward relative to the accelerating platform. The importance of free body diagrams is highlighted, with corrections made regarding the direction of friction and the forces acting on both the sphere and the platform. Additionally, there are discussions about rotational kinetic energy and the correct approach to calculating it based on the center of rotation. Overall, the conversation aims to refine the understanding of mechanics principles in this context.
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need your help tiny-tim pleaseeee:)
 
hi winichris! :wink:
winichris said:
Is this the correct approach of the first part of the 2nd question?

yes, that looks fine :smile:
 
tiny-tim said:
hi winichris! :wink:


yes, that looks fine :smile:
THANKS.

For the part 2bi:

let f be the frictional force acting on the sphere pointing towards right.

Setting the below 3 equations, then i can solve for a,α and f right?
fR=Iα
a=Rα
f=Ma

But the moment of inertia found from part a is about diameter.
In part b, the moment of inertia should be in the center, so I need the use the part a result and times 2? (because i rarely remember that moment of inertia about diameter = moment of inertia about center /2)
 
hi winichris! :smile:
winichris said:
let f be the frictional force acting on the sphere pointing towards right.

Setting the below 3 equations, then i can solve for a,α and f right?
fR=Iα
a=Rα
f=Ma

those three equations would be fine if the platform was not accelerating

you need to adjust a=Rα, and you need a fourth equation, F=ma for the platform :wink:

(call the acceleration of the platform "A")
But the moment of inertia found from part a is about diameter.
In part b, the moment of inertia should be in the center, so I need the use the part a result and times 2? (because i rarely remember that moment of inertia about diameter = moment of inertia about center /2)

no, you're rambling :rolleyes:

this is a (hollow) sphere, and the diameter is through the centre, isn't it? :biggrin:

(you're thinking about the perpendicular axis theorem, it only applies to "2D" bodies, eg a disc)
 
tiny-tim said:
hi winichris! :smile:


those three equations would be fine if the platform was not accelerating

you need to adjust a=Rα, and you need a fourth equation, F=ma for the platform :wink:

(call the acceleration of the platform "A")
My professor said the velocity of the platform and the velocity of the sphere are the same.
So I think their acceleration will be the same, right?


tiny-tim said:
no, you're rambling :rolleyes:

this is a (hollow) sphere, and the diameter is through the centre, isn't it? :biggrin:

(you're thinking about the perpendicular axis theorem, it only applies to "2D" bodies, eg a disc)
Ok then i can just use the part a result! thx
 
winichris said:
My professor said the velocity of the platform and the velocity of the sphere are the same.

no, that's rubbish :redface:

the sphere will roll backwards relative to the platform: its velocity and acceleration will be less than that of the platform
 
tiny-tim said:
no, that's rubbish :redface:

the sphere will roll backwards relative to the platform: its velocity and acceleration will be less than that of the platform
Let A be acceleration of platform, a be acceleration of sphere
M be mass of sphere, m be mass of platform

4 equations:
fR=Iα
(A-a)=Rα<--i am not sure whether this adjustment is correct or not..
f=Ma
F=mA<--use F=mA or F+f=mA?
 
winichris said:
fR=Iα
f=Ma

yes :smile:
(A-a)=Rα<--i am not sure whether this adjustment is correct or not..

(a-A)=Rα :wink:

(because a-A is the acceleration relative to the platform)
F=mA<--use F=mA or F+f=mA?

definitely F+f = mA (or is it F-f = mA ?) …

a free body diagram would show both forces on the platform :wink:
 
  • #10
tiny-tim said:
yes :smile:


(a-A)=Rα :wink:

(because a-A is the acceleration relative to the platform)
As you mentioned before, A>a, so α will be negative?

tiny-tim said:
definitely F+f = mA (or is it F-f = mA ?) …

a free body diagram would show both forces on the platform :wink:
friction should be point towards right, so should be F+f=mA instead of F-f=mA?
 
  • #11
winichris said:
As you mentioned before, A>a, so α will be negative?

yup, the sphere will roll backward, and get left behind :wink:
friction should be point towards right

friction from the sphere on the platform?
 
  • #12
  • #13
no, that's not a free body diagram, it's showing two bodies and an internal force between them

free body diagrams don't have internal forces

do a free body diagram for the sphere … which way does the friction go?

then do a free body diagram for the platform :smile:
 
  • #14
tiny-tim said:
no, that's not a free body diagram, it's showing two bodies and an internal force between them

free body diagrams don't have internal forces

do a free body diagram for the sphere … which way does the friction go?

then do a free body diagram for the platform :smile:

http://imageshack.us/photo/my-images/839/32859543.png/

Is the above free body diagram of sphere and platform correct?

I am not quite sure about whether the friction on platform should be point to right or left..
 
  • #15
winichris said:
Is the above free body diagram of sphere and platform correct?

yes! :smile:

(very good free body diagrams :wink:)

the top diagram shows that the friction from the platform must be to the right

(and, btw, that the rotation must be anti-clockwise)

and so Newton's third law tells us that the reaction force, the friction on the platform, must be to the left :smile:

(and so the sphere slows the platform down, exactly as if it wasn't rolling)
 
  • #17
  • #18
oooh, sorry … two errors :frown:

i] rotational kinetic energy is
either 1/2 Iωc.o.rotation2

or 1/2 Iωc.o.mass2 + 1/2 mvc.o.mass2
ie if you use the centre of rotation, you can forget about 1/2 mv2

(in the previous question, the end of the rod was attached to a ring which was moving, so it wasn't the centre of rotation, here it's fixed, so it is)

you've done 1/2 Iωc.o.rotation2 + 1/2 mvc.o.mass2 :redface:

ii] ω is in radians per second, so time = radians/ω,

but you haven't used radians :redface:
 
  • #19
tiny-tim said:
oooh, sorry … two errors :frown:

i] rotational kinetic energy is
either 1/2 Iωc.o.rotation2

or 1/2 Iωc.o.mass2 + 1/2 mvc.o.mass2
ie if you use the centre of rotation, you can forget about 1/2 mv2

(in the previous question, the end of the rod was attached to a ring which was moving, so it wasn't the centre of rotation, here it's fixed, so it is)

you've done 1/2 Iωc.o.rotation2 + 1/2 mvc.o.mass2 :redface:

ii] ω is in radians per second, so time = radians/ω,

but you haven't used radians :redface:
So for energy:
mga = 0.5Iω2 to find ω is enough?

Then moment of inertia used above should be 1/12m(2a)2 or 1/12m(2a)2+ma2?
(As when the hinge breaks, the center of rotation change to center of rod?)

For time used: it should be 2pi/ω?
 
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  • #20
hi winichris! :smile:
winichris said:
So for energy:
mga = 0.5Iω2 to find ω is enough?

Then moment of inertia used above should be 1/12m(2a)2 or 1/12m(2a)2+ma2?

to find the energy for the first part:

yes, mga = 0.5Iω2 to find ω is enough (ie no 1/2 mv2 is needed),

provided you use the centre of rotation, (ie I = 1/12m(2a)2+ma2)
(As when the hinge breaks, the center of rotation change to center of rod?)

(this is the second part)

why does the centre of rotation matter? :confused:

the rotation will be constant in the second part

(and anyway, no, it isn't in the centre of the rod, it probably isn't even in the rod at all)
For time used: it should be 2pi/ω?

well, it's angle/ω, and the angle is 90°, so that's π/2ω :wink:
 
  • #21
tiny-tim said:
hi winichris! :smile:


to find the energy for the first part:

yes, mga = 0.5Iω2 to find ω is enough (ie no 1/2 mv2 is needed),

provided you use the centre of rotation, (ie I = 1/12m(2a)2+ma2)


(this is the second part)

why does the centre of rotation matter? :confused:

the rotation will be constant in the second part

(and anyway, no, it isn't in the centre of the rod, it probably isn't even in the rod at all)


well, it's angle/ω, and the angle is 90°, so that's π/2ω :wink:
Thanks!
I get 2 last problems about heat, hope you can help me:)

https://www.physicsforums.com/showthread.php?p=3881230#post3881230
 
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  • #22
not really my scene

i'll let someone else have a go! :smile:
 
  • #23
tiny-tim said:
not really my scene

i'll let someone else have a go! :smile:

ok.thx anyway, u help me a lot!
 
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