A wooden disk is set on its edge on a table top. A string is wrapped around its outer circumference and a hand is pulling on the string horizontally from the top, so that the disk rolls without slipping on the table. The center of the disk is moving with a velocity of 12.0 cm/s. What is the velocity of the hand? V hand Vcenter
A wooden disk is set on its edge on a table top. A string is wrapped around its outer circumference and a hand is pulling on the string horizontally from the top, so that the disk rolls without slipping on the table. The center of the disk is moving with a velocity of 12.0 cm/s. What is the velocity of the hand? V hand Vcenter
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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Question
![A wooden disk is set on its edge on a table top. A string is wrapped around its
outer circumference and a hand is pulling on the string horizontally from the
top, so that the disk rolls without slipping on the table. The center of the disk is
moving with a velocity of 12.0 cm/s. What is the velocity of the hand?
V hand
Vcenter](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Ff456c65b-f482-4083-8c37-6fe7d8344e1a%2F9b472e3a-414c-4e87-9541-7977a9380e0d%2Fs95o1yp_processed.png&w=3840&q=75)
Transcribed Image Text:A wooden disk is set on its edge on a table top. A string is wrapped around its
outer circumference and a hand is pulling on the string horizontally from the
top, so that the disk rolls without slipping on the table. The center of the disk is
moving with a velocity of 12.0 cm/s. What is the velocity of the hand?
V hand
Vcenter
![FORMULAS
s= r0,
1= lever arm
T = FI, where
v = ro,
Torque: t = F(sin0)r
a = ra
Equilibrium: Στ-0
Non-equilibrium:
Στ= Ια
Moments of Inertia for Various Rigid Objects of uniform composition: Point
mass: I= MR2
Moments of Inertia for Various Rigid Objects of Uniform Composition
Hoop or thin
cylindrical shell
1= MR
Solid sphere
R
Solid cylinder
or disk
Thin spherical
shell
-MR
2
MR
1=-
2
Long, thin rod
with rotation axis
through center
I MI?
Long, thin
rod with
rotation axis
through end
ML?
= r®,
1= lever arm
v = ro,
a = ra
Torque: t = F(sin0)r
T = Fl, where
%3D
Equilibrium: Στ-0
Non-equilibrium:
Στ-Ια](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Ff456c65b-f482-4083-8c37-6fe7d8344e1a%2F9b472e3a-414c-4e87-9541-7977a9380e0d%2F16tpvxi_processed.png&w=3840&q=75)
Transcribed Image Text:FORMULAS
s= r0,
1= lever arm
T = FI, where
v = ro,
Torque: t = F(sin0)r
a = ra
Equilibrium: Στ-0
Non-equilibrium:
Στ= Ια
Moments of Inertia for Various Rigid Objects of uniform composition: Point
mass: I= MR2
Moments of Inertia for Various Rigid Objects of Uniform Composition
Hoop or thin
cylindrical shell
1= MR
Solid sphere
R
Solid cylinder
or disk
Thin spherical
shell
-MR
2
MR
1=-
2
Long, thin rod
with rotation axis
through center
I MI?
Long, thin
rod with
rotation axis
through end
ML?
= r®,
1= lever arm
v = ro,
a = ra
Torque: t = F(sin0)r
T = Fl, where
%3D
Equilibrium: Στ-0
Non-equilibrium:
Στ-Ια
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