Angular Momentum and uniform flat disk of mass Problem

In summary: Now what do you want to know?In summary, a uniform flat disk of mass M and radius R rotates about a horizontal axis through its center with angular speed ωi. The angular momentum is given by Li = ωi(1/2)MR^2. A chip of mass m breaks off the edge of the disk and rises vertically above the point at which it broke off. The final angular speed of the broken disk can be found using the formula Vτ = ωiR and the distance the chip rises before starting to fall can be calculated using the formula d = (ωiR)^2/2g.
  • #1
Destrio
212
0
A uniform flat disk of mass M and radius R rotates about a horizontal axis through its center with angular speed ωi.
a) What is its angular momentum
b) A chip of mass m breaks off the edge of the disk at an instant such that the chip rises vertically above the point at which it broke off. How how above the point does it rise before starting to fall?
c) What is the final angular speed of the broken disk.

Li = Iωi
I of wheel = (1/2)MR^2
Li = ωi(1/2)MR^2

d = Vit + (1/2)at^2

i figure this velocity will be equal to sin(theta)*Vtangential (Vτ)

d = Vτi*sin(theta)*t + (1/2)gt^2

is this correct?

thanks
 
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  • #2
Destrio said:
Li = Iωi
I of wheel = (1/2)MR^2
Li = ωi(1/2)MR^2
OK.

d = Vit + (1/2)at^2

i figure this velocity will be equal to sin(theta)*Vtangential (Vτ)
You aren't given the time or the tangential speed. And it rises vertically, so what must be its direction?

Find the distance in terms of the given parameters.
 
  • #3
Li = Iωi
I of wheel = (1/2)MR^2
Li = ωi(1/2)MR^2

can i assume there is no horizontal component to the flying chip?
if so, won't Vτ = ωiR at some point

do I have to find distance in terms of R?
 
  • #4
Destrio said:
can i assume there is no horizontal component to the flying chip?
I would.
if so, won't Vτ = ωiR at some point
Yes. That's the speed of the chip as it breaks off.

do I have to find distance in terms of R?
Find it any way you can, but only in terms of the parameters given. That distance only depends on the initial speed, but that speed is in terms of ωi and R.
 
  • #5
Li = Iωi
I of wheel = (1/2)MR^2
Li = ωi(1/2)MR^2

Vτ = ωiR

i need to know when Vf = 0

so Vf = Vo + at
Vf = 0
Vo = Vτ = ωiR
-a = g
0 = ωiR - gt
gt = ωiR
t = ωiR/g

d = ωiR(ωiR/g) + (1/2)g(ωiR/g)^2
d = (ωiR)^2/g + (ωiR)^2/2g
d = 2(ωiR)^2/2g + (ωiR)^2/2g
d = 3(ωiR)^2/2g

this this correct?

thanks
 
  • #6
Destrio said:
Li = Iωi
I of wheel = (1/2)MR^2
Li = ωi(1/2)MR^2

Vτ = ωiR

i need to know when Vf = 0

so Vf = Vo + at
Vf = 0
Vo = Vτ = ωiR
-a = g
0 = ωiR - gt
gt = ωiR
t = ωiR/g
OK.
d = ωiR(ωiR/g) + (1/2)g(ωiR/g)^2
a = -g
 
  • #7
d = ωiR(ωiR/g) - (1/2)g(ωiR/g)^2
d = (ωiR)^2/2g
 
  • #8
Destrio said:
d = ωiR(ωiR/g) - (1/2)g(ωiR/g)^2
d = (ωiR)^2/2g
Good.
 

FAQ: Angular Momentum and uniform flat disk of mass Problem

What is angular momentum?

Angular momentum is a measure of an object's rotational motion around a fixed axis. It is calculated by multiplying the object's moment of inertia by its angular velocity.

How is angular momentum related to a uniform flat disk of mass problem?

In a uniform flat disk of mass problem, the angular momentum is conserved. This means that the total angular momentum of the system remains constant, even as the disk's angular velocity changes.

What is the moment of inertia of a uniform flat disk?

The moment of inertia of a uniform flat disk is equal to 1/2 times the mass of the disk multiplied by the square of its radius.

How does the mass distribution of a disk affect its angular momentum?

The mass distribution of a disk affects its moment of inertia, which in turn affects its angular momentum. A disk with more mass located at the edges will have a higher moment of inertia and therefore a higher angular momentum compared to a disk with the same mass distributed evenly.

Can a disk's angular momentum be changed without applying an external torque?

No, according to the law of conservation of angular momentum, a system's total angular momentum cannot change without an external torque acting on it. In a uniform flat disk of mass problem, the angular momentum can only be changed by applying an external torque, such as a force acting on the edge of the disk.

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