A counterweight of mass m = 4.30 kg is attached to a light cord that is wound around a pulley as shown in the figure below. The pulley is a thin hoop of radius R = 7.00 cm and mass M = 1.60 kg. The spokes have negligible mass. (a) What is the net torque on the system about the axle of the pulley? magnitude N · m direction (b) When the counterweight has a speed v, the pulley has an angular speed ω = v/R. Determine the magnitude of the total angular momentum of the system about the axle of the pulley. ( kg · m)v (c) Using your result from (b) and tau with arrow = dL with arrow/dt, calculate the acceleration of the counterweight. (Enter the magnitude of the acceleration.) m/s2
given
m = 4.30 kg
R = 7.00 cm
M = 1.60 kg
a )
total = wheel + counterweight
= r X F
we have r = - R i and F = - T j
= ( - Ri ) X ( - T j )
= R T k ( since i X j = k )
b )
total angular momentum
Ltotal = Lwheel + Lcounterweight
we have L = I
now Lwheel = M R2 => M R v
Lcounterweight = ( - Ri - Qj ) X ( - m v j )
Lcounterweight = m R v k
Ltotal = ( m + M ) R v k
c )
given
= dL / dt
the equation is used here is = m g R
dL /dt = ( m + M ) R dv / dt
m g R = ( m + M ) R a ( since a = dv/dt )
a = m g / ( m + M )
d )
given
m = 4.30 kg
R = 7.00 cm
M = 1.60 kg
using a = m g / ( m + M )
a = 4.3 X 9.8 / ( 4.3 + 1.6 )
a = 7.14 m/sec2
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