spool comprised of a cylinder of radius a and negligible mass about which a ligh
ID: 2268950 • Letter: S
Question
spool comprised of a cylinder of radius a and negligible mass about which a light cable is wound and two disks of radius b and mass m/2 on either side is on a frictionless inclined plane is illustrated D. A below. Calculate the position of the 'spool' as a function of time if it starts from rest at x-0m and t-0s. (20) E. If the cable runs out just as the 'spool' smoothly transitions to a level surface (Vem I| surface) with a coefficient of friction , under what conditions (if any) will vcm become zero (be specific). (20)Explanation / Answer
D. given spool, cylinder of radius a, negligible mass
light cable
radii of discs = b, mass = m/2 each
position of spool as a fiunction of time = x(t)
now from force balance
let tension in the string be T
friciton = f
then from force balance
mg*sin(theta) - f - T = m*x" ( where x" = d^x/dt^2)
now,
f = mu*mg*cos(theta) ( where mu us coefficient of kinetic friction)
also, for angular acceleraiton alpha
2*0.5*(m/2)(b^2)*alpha = f*b - T*a
hence
T = [mu*mg*cos(theta)b - 0.5mb^2*alpha]/a
hence
mg*sin(theta) - mu*mg*cos(theta) - [mu*mg*cos(theta)b - 0.5mb^2*alpha]/a = m*x"
for frictionless, mu = 0
hence
g*sin(theta) + 0.5b^2*alpha/a = x"
now, alpha = theta"
if the wheel rotates by angle theta, it loses theta*a length in x direction
hence
x = theta*a
theta" = x"/a
hence
g*sin(theta) = x"(1 - b^2/2a^2)
x" = g*sin(theta)/(1 - b^2/2a^2)
integrating
x' = g*sin(theta)*t/(1 - b^2/2a^2) ( given initial speed = 0)
integrating again
x = gt^2*sin(theta)/2(1 - b^2/2a^2) ( given initial position is 0)
E. just as the cable runs out of spool
angular speed = w
linear speed = v
w = theta' = g*sin(theta)to/a(1 - b^2/2a^2)
v = x' = g*sin(theta)to/(1 - b^2/2a^2)
where to is tome after which the spool is free of string
now,
acceleration = mu*g
hence
fomr previous relations
w = v/a
assume after time t1, w becomes 0
then
final speed = U
U = v + mu*g*t1
v = mu*gt
also
from moment balance
angular deceleration = mu*g/b
hence
0 = v/a - mu*g*t1/b
hence
t1 = v*b/a*g*mu
so, U = v + mu*g*v*b/a*g*mu = v + v*b/a = v(1 + b/a)
now,
after this, theere is linear deceleration and angular acceleration
let after time t2, the linear speed = 0
hence
0 = U - mu*g*t2
t2 = U/mu*g = v(1 + b/a)/mu*g
angular speed at this instant
w = mu*g*t2/b = v(1 + b/a)/b
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