Resource Lesson
Systems of Bodies
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When two or more bodies are connected by a cord and move in tandem, then they are considered to be a
system of bodies
. When working problems involving systems of bodies,
the first step is to draw
freebody diagrams
for each object. Remember, that the principle forces that we are now considering are: normals, weight, friction, tensions and generic applied forces.
since both masses are attached, they share the same kinematics properties: displacement, velocity, acceleration and time.
when writing equations for net F = ma, the direction of motion is considered to be the positive direction for the acceleration of the objects comprising the system.
Table Surface
Let's consider as our first example, two identical objects being dragged across the surface of a frictionless table by two cords.
The two freebody diagrams would look like:
left mass
right mass
In order to determine the acceleration of the system and the tension in each cord, we will need to write the equations of motion for each mass: net F
_{x}
= ma
_{x}
and net F
_{y}
= ma
_{y}
.
left mass
right mass
net F
_{x}
= ma
_{x}
T
_{1}
= ma
T
_{2}
- T
_{1}
= ma
net F
_{y}
= ma
_{y}
- mg = 0
- mg = 0
Solving the two equations for net F
_{x}
= ma
_{x}
simultaneously yields the equation:
T
_{1}
= ma
T
_{2}
- T
_{1}
= ma
-------------------
T
_{2}
= 2ma
If the numerical values for T
_{2}
and m are given, then this equation will allow you to solve for the acceleration of the system. Once the acceleration is known, then the tension in cord #1 can also be calculated.
Hanging Masses
Now suppose that the right mass is hanging off a frictionless table and the cord connecting it to the left mass passes over a "massless, frictionless" pulley.
How would this change the freebody diagrams for each mass and their equations of motion?
mass on table
hanging mass
net F
_{x}
= ma
_{x}
T = ma
------
net F
_{y}
= ma
_{y}
- mg = 0
mg - T = ma
Solving these equations simultaneously for the acceleration yields the equation:
T = ma
mg - T = ma
--------------------
mg = 2ma
a = ½g
Once again, if the numerical value for m is given then this equation will allow you to solve for the acceleration of the system. Remember that "g" represents the acceleration due to gravity, 9.8 m/sec
^{2}
. Once the acceleration is known, then the tension in the cord can be calculated.
Refer to the following information for the next six questions.
Obviously, the masses in the previous example do not have to be the same. Solve for the acceleration of the system and the tension in the cord if the hanging object has a mass of 3 kg and the mass on the table is 2 kg.
Write the equation for net F
_{x}
= ma
_{x}
for the 2 kg mass.
Write the equation for net F
_{y}
= ma
_{y}
for the 2 kg mass.
Write the equation for net F
_{x}
= ma
_{x}
for the 3 kg mass.
Write the equation for net F
_{y}
= ma
_{y}
for the 3 kg mass.
What is the acceleration of the system?
What is the tension in the cord?
Atwood Machine
Refer to the following information for the next six questions.
In our third example the two masses are attached to the ends of a single cord that passes over a massless, frictionless pulley suspended from the ceiling. This situation is called an Atwood Machine.
Write the equation for net F
_{y}
= ma
_{y}
for the 2 kg mass.
Write the equation for net F
_{y}
= ma
_{y}
for the 5 kg mass.
Why did we not need to subscript the tension variables?
Why did we not need to write the equations for net F
_{x}
= ma
_{x}
for these two bodies?
What is the acceleration of the system?
What is the tension in the cord?
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Air Resistance: Terminal Velocity
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The Box Seat
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The Jogger
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Action-Reaction #1
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Action-Reaction #2
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Equilibrium on an Inclined Plane
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Falling and Air Resistance
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Force and Acceleration
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Force and Weight
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Force Vectors and the Parallelogram Rule
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Freebody Diagrams
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Gravitational Interactions
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Incline Places: Force Vector Resultants
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Incline Planes - Force Vector Components
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Inertia
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Mobiles: Rotational Equilibrium
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Net Force
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Newton's Law of Motion: Friction
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Static Equilibrium
CP -
Tensions and Equilibrium
NT -
Acceleration
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Air Resistance #1
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An Apple on a Table
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Apex #1
NT -
Apex #2
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Falling Rock
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Falling Spheres
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Friction
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Frictionless Pulley
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Gravitation #1
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Head-on Collisions #1
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Head-on Collisions #2
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Ice Boat
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Rotating Disk
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Sailboats #1
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Sailboats #2
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Scale Reading
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Settling
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Skidding Distances
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Tensile Strength
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Terminal Velocity
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Tug of War #1
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Tug of War #2
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Advanced Properties of Freely Falling Bodies #2
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Distinguishing 2nd and 3rd Law Forces
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Force vs Displacement Graphs
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Freebody Diagrams #1
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Freebody Diagrams #4
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Work, Power, Kinetic Energy
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