Difference between revisions of "Forest UCM NLM AtwoodMachine"
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== Step 4: Define the Force vectors using the above coordinate system== | == Step 4: Define the Force vectors using the above coordinate system== | ||
+ | |||
+ | since the system is one dimensional I will omit the vector notation | ||
+ | |||
+ | :<math>T_1=</math> Tension in the rope attached to mass <math>m_1</math> | ||
+ | :<math>T_2=</math> Tension in the rope attached to mass <math>m_2 = T_1</math> | ||
+ | :<math>T_3=</math> Tension in the rope attached to mass <math>m_3</math> | ||
+ | :<math>F_g</math> = force of gravity on each mass <math>= m_1 g</math> or <math>m_2 g</math> or <math>m_3 g</math> | ||
+ | |||
+ | ==Step 5: Use Newton's second law== | ||
;for mass 1 | ;for mass 1 |
Revision as of 11:58, 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
since the system is one dimensional I will omit the vector notation
- Tension in the rope attached to mass
- Tension in the rope attached to mass
- Tension in the rope attached to mass
- = force of gravity on each mass or or
Step 5: Use Newton's second law
- 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
assuming that
is moving upwards with respect to the earth- : acceleration of lower pully as well as
similarly
- : if is accelerating upwards then is accelerating downwards