Difference between revisions of "Forest UCM NLM AtwoodMachine"
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− | Using Newton's | + | Using Newton's third law we know that <math>T_1 = T_2</math> reducing the unkowns to 5. |
− | ;We need | + | ;We need 2 more equations! |
===External Forces on Lower pulley=== | ===External Forces on Lower pulley=== | ||
Line 52: | Line 52: | ||
− | T_3-T1-T2 = (0)a | + | :<math>T_3-T1-T2 =T_3-T1-(T1) =(0)a</math> |
+ | ::<math>T_3=2T_1</math> | ||
==Step 5: Use Newton's second law== | ==Step 5: Use Newton's second law== |
Revision as of 11:47, 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 third law we know that reducing the unkowns to 5.
- We need 2 more equations!
External Forces on Lower pulley
Consider the external forces acting on the MASSLESS lower pulley