Difference between revisions of "Forest UCM NLM AtwoodMachine"
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Line 38: | Line 38: | ||
;for mass 3 | ;for mass 3 | ||
:<math>T_3 - m_3 g = m_3 a_3</math> | :<math>T_3 - m_3 g = m_3 a_3</math> | ||
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+ | |||
+ | If we know the mass of all the objects in the system then we are left with three unkown Tensions and three unknown acceleratios. In total we currently have 6 unkowns and 3 equations. | ||
+ | |||
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+ | Using Newton's first law we know that T_1 = T_2 | ||
+ | |||
+ | ;We need three more equations! | ||
+ | |||
+ | ===External Forces on Lower pulley=== | ||
+ | |||
+ | Consider the external forces acting on the MASSLESS lower pulley | ||
+ | |||
+ | |||
+ | T_3-T1-T2 = (0)a | ||
==Step 5: Use Newton's second law== | ==Step 5: Use Newton's second law== |
Revision as of 11:45, 22 August 2014
Simple Atwood's machine
Double Atwood's machine
The problem
Determine the acceleration of each mass in the above picture.
Step 1: Identify the system
- Each block is a separate system with two external forces; a gravitational force and the rope tension.
Step 2: Choose a suitable coordinate system
- A coordinate system with one axis that defines the posive direction as up is one possible orientation.
Step 3: Draw the Free Body Diagram
Step 4: Define the Force vectors using the above coordinate system
- for mass 1
- for mass 2
- for mass 3
If we know the mass of all the objects in the system then we are left with three unkown Tensions and three unknown acceleratios. In total we currently have 6 unkowns and 3 equations.
Using Newton's first law we know that T_1 = T_2
- We need three more equations!
External Forces on Lower pulley
Consider the external forces acting on the MASSLESS lower pulley
T_3-T1-T2 = (0)a