Bucket of water of is suspended by a rope wrapped around a pulley

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Homework Help Overview

The problem involves a 13.0 kg bucket of water suspended by a rope around a pulley, which is a solid cylinder with a mass of 17.0 kg and a diameter of 0.300 m. The bucket falls 12.0 m, and the discussion revolves around calculating the tension in the rope, the speed of the bucket upon striking the water, the time of fall, and the force exerted on the cylinder by the axle.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the relationship between the forces acting on the bucket and the pulley, including tension and gravitational forces. There are attempts to derive equations for acceleration and tension, with some questioning the assumptions made regarding forces acting on the cylinder.

Discussion Status

Several participants have provided calculations for the tension and acceleration, while others are exploring the forces acting on the cylinder. There is some uncertainty regarding the net forces and whether the tension alone accounts for the force on the cylinder. Guidance has been offered to reconsider the forces involved.

Contextual Notes

Participants are working under the assumption that the axle is frictionless, which influences the torque calculations. There is a focus on ensuring all forces acting on the cylinder are considered in the analysis.

squintyeyes
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how do you do the last part.

A 13.0 kg bucket of water of is suspended by a rope wrapped around a pulley, which is just a solid cylinder 0.300 m in diameter with mass 17.0 kg. The cylinder is pivoted on a frictionless axle through its center. The bucket is released from rest at the top of a well and falls 12.0 m to the water. Neglect the weight of the rope.

(a) What is the tension in the rope while the bucket is falling?
50.367 N
(b) With what speed does the bucket strike the water?
11.925 m/s
(c) What is the time of fall?
2.013 s
(d) While the bucket is falling, what is the force exerted on the cylinder by the axle?

Attempt
F=Mg-Ma
then implied:
a=(F-Mg)/M
which seems unsound, it should have said:
a = (Mg - F)/M
----------------------
Now, let's begin and use the previous gentleman's notation:
Mass of bucket=M
mass of cylinder=m
Tension force=F
So, regarding the bucket:
F + Ma = Mg
F = Mg - Ma
a = (Mg - F)/M
Also, regarding the cylinder:
T = Iα

(By the dot product of torque, radial vector crossed with force, r cross F, which is Frsinθ for θ = 90 degrees)
T = Iα = Fr = (1/2)(mr2)(a/r)
where α = a/r
And T = Fr because that's what torque is, just the radial distance times the force.
So
a = 2F/m
and we also have:
a = (Mg-F)/M
So 2F/m = (Mg-F)/M
2F = mg - mF/M
2F+(mF)/M = mg
F(2+m/M) = mg
F = mg/(2+m/M)
F = (167 kg*m/s2)/(2+1.31kg/kg)
F = 50.367 N
That is to say, the tension that the rope induces on the bucket is 50.5 Newtons in the upward direction (positive).
--------------
So we have solved Part (A)
F = 50.367 N
---------------
We know that:
F = Mg-Ma
So
a = (Mg - F)/M
where F = 50.367 N
So
a = [(13.0kg)(9.8m/s2) - 50.367N]/13.0kg
a = (127N - 50.367N)/13.0kg
a = 5.925 m/s2
--------------------
Now that we have a, let's find t,
a = a
v = at + vyo
y = yo + vyot + (1/2)ayt2
Counting positive y to be downward, (our acceleration will be positive then)
12.0 m = 0 + 0t + (1/2)(5.925m/s2)t2
t2 = (12.0m)/(2.963 m/s2)
t2 = 4.051 s2
t = 2.013 s
That is to say, it takes the bucket 2.10 seconds to reach the water surface below.
--------------
So we have solved Part (C)
t = 2.013 s
---------------
a = a
v = at + C
But C, the constant of integration, is the initial velocity, is zero.
so
v = at
where t =2.013 s
a = 5.925 m/s2
so
v = (5.925m/s2)(2.013s)
v = 11.925 m/s
That is to say, the bucket is traveling at 11.925 m/s when it reaches the surface of the water.
--------------
So we have solved Part (B)
v = 11.925 m/s
---------------
The force exerted on the cylinder by the axle is just the torque (which is in the z direction, like a pole coming out of the page).
We know that the torque is:
T = Iα
where moment of Inertia for a cylinder is
I = (1/2)mr2
and the angular acceleration is
α = a/r
with a = 5.925m/s2
r = 0.150 m
So
T = Iα
T = (1/2)(17.0kg)(0.150m)2[5.925m/s2]/(0.150m)
T = (8.5kg)(0.150m)(5.925m/s2)
T = 7.555 N*m
or
T = 7.555 J

T= Fr
F=T/r
F= 7.555/0.150
F= 50.367 N
 
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squintyeyes said:
The force exerted on the cylinder by the axle is just the torque (which is in the z direction, like a pole coming out of the page).
Since the axle is frictionless, it exerts no torque. (If it did exert a torque, your previous work would be incorrect since it ignored it.)

Hint: Consider the forces acting on the cylinder. What must be the net force?
 
so is it just the force of tension. that means the answer to a and d are the same.
 
squintyeyes said:
so is it just the force of tension. that means the answer to a and d are the same.
No. You're overlooking one of the forces acting on the cylinder.
 
oh would i do
force of gravity + tension = force on cylinder
mg + 50.367 =
17(9.8) + 50.367=
216.967 N
 
Good.
 
thank you for your help
 

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