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A mass falling while attached to a massive pulley.
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Composition Setup
A bucket for collecting water from a well is suspended by a rope which is wound around a pulley. The empty bucket has a mass of 2.0 kg, and the pulley is essentially a uniform cylinder of mass 3.0 kg on a frictionless axle. Suppose a person drops the bucket (from rest) into the well.
We will consider two different methods to obtain the solution.
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Method 1: Dynamics
Method 1: Dynamics
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Systems:
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The pulley and the bucket are treated as separate objects. The bucket can be treated as a , but the pulley must be treated as a .
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The pulley and the bucket are each subject to external influences from the rope () and from the earth (gravity). The pulley is also subject to a from the axle, but we will choose the axle as the axis of rotation so the axle produces no torque (it has zero ).
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Model:
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and
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Approach:
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The system is subject to external forces from the earth acting on the bucket and the pulley (gravity) and from the axle acting on the pulley (contact force). If we choose the axis of rotation to coincide with the axle of the pulley, then the axle's force and gravity acting on the pulley each produce no torque. We need only consider the effects of gravity acting on the bucket.
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Model:
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Method 2: Dynamics
Method 2: Dynamics
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littledeck
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Part A
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Part B
Part B
What is the bucket's speed after falling 5.0 m down the well?
Solution
Again, we will use two methods.
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Method 1: Kinematics
Method 1: Kinematics
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System:
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Bucket as .
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Interactins:
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External influences from the earth (gravity) and the rope (tension).
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Model:
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One-Dimensional Motion with Constant Acceleration.
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Method 1: Kinematics
Method 1: Kinematics
Method1
Method1
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Method 2: Energy
Method 2: Energy
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sysb2
System:
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Treat the bucket, pulley and the earth as a single system.
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Interactions:
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Internal interactions of gravity (conservative) and tension from the rope (non-conservative) plus an external influence from the normal force on the pulley (non-conservative).