Answer 2nd Question Part 1: Mechanics Ques.

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In summary, the conversation discusses a physics problem involving a rolling sphere and a platform. The participants discuss equations and adjustments needed to solve for acceleration, moment of inertia, and frictional force. They also discuss the direction of the friction force and the importance of a free body diagram in solving the problem. The conversation ends with one of the participants expressing excitement about completing the problem.
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  • #2
need your help tiny-tim pleaseeee:)
 
  • #3
hi winichris! :wink:
winichris said:
Is this the correct approach of the first part of the 2nd question?

yes, that looks fine :smile:
 
  • #4
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)
 
  • #5
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)
 
  • #6
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
 
  • #7
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
 
  • #8
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?
 
  • #9
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?
 
  • #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?
 
Last edited:
  • #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
 
Last edited by a moderator:
  • #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!
 

1. What is mechanics?

Mechanics is the branch of physics that deals with the behavior of physical bodies when subjected to forces or displacements, and the subsequent effects of those bodies on their environment.

2. What are the main principles of mechanics?

The main principles of mechanics are Newton's laws of motion, which describe how forces affect the motion of objects, and the conservation of energy and momentum, which state that energy and momentum can neither be created nor destroyed, only transferred between objects.

3. How is mechanics used in the real world?

Mechanics is used in many real-world applications, such as designing and building structures, vehicles, and machines. It is also used in fields like aerospace engineering, robotics, and biomechanics to understand and improve the performance of systems and devices.

4. What is the difference between classical mechanics and quantum mechanics?

Classical mechanics is the branch of mechanics that deals with the motion of macroscopic objects, while quantum mechanics is the branch that deals with the behavior of particles at the atomic and subatomic level. Classical mechanics follows a deterministic approach, while quantum mechanics follows a probabilistic approach.

5. What are some common applications of classical mechanics?

Some common applications of classical mechanics include designing and analyzing the motion of objects in everyday life, such as cars, airplanes, and amusement park rides. It is also used in fields like sports science, where the mechanics of human movement are studied and improved.

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