Difference between revisions of "Forest UCM NLM AtwoodMachine"
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:<math>T_3-T1-T2 =T_3-T1-(T1) =(0)a</math> | :<math>T_3-T1-T2 =T_3-T1-(T1) =(0)a</math> | ||
::<math>T_3=2T_1</math> | ::<math>T_3=2T_1</math> | ||
+ | |||
+ | |||
+ | Now we have 4 unkwons and 3 equations | ||
+ | |||
+ | ===relative acceleration=== | ||
+ | |||
+ | let | ||
+ | |||
+ | :<math>a_r =</math> acceleration of <math>m_1</math> with respect to the lower pulley | ||
+ | |||
+ | with respect to the earth | ||
+ | |||
+ | :<math>a_1 = a_r - a_3</math> : <math>a_3 =</math> acceleration of lower pully as well as <math>m_3</math> | ||
+ | |||
+ | |||
+ | similarly | ||
+ | |||
+ | :<math>a_2=-a_r-a_3</math> | ||
==Step 5: Use Newton's second law== | ==Step 5: Use Newton's second law== |
Revision as of 11:52, 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
Now we have 4 unkwons and 3 equations
relative acceleration
let
- acceleration of with respect to the lower pulley
with respect to the earth
- : acceleration of lower pully as well as
similarly