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Sinusoidal |
![sinusoidal](2 dimensional motiona/sinusoidal.gif) |
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CYCLOID PENDULUM COMPARED TO CIRCULAR |
![CYCLOID](2 dimensional motiona/CYCLOID.gif)
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![CIRCULAR](2 dimensional motiona/CIRCULAR.gif) |
In this file you can change teh parameters (length and amplitude) and compare the motion of a cycloid and a simple pendulum |
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Neil Curve |
![Neil Curve](2 dimensional motiona/Neil-Curve.gif) |
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MAGNETIC FORCE AND ATTRACTIVE FORCE |
![Magnetic Fpucault](Magnetic-Foucault.gif) |
Motion of a charged body in a combination of a magnetic field
and a central field that can be attractive to the origin or repulsive.
by choosing intial value of velocity we can change the shape of the
orbit. |
MOTION ON A ROTATING DISK WITH CONSTANT ANGULAR VELOCITY |
![CONSTANT ANBULAR VELOCITY](excel%20dynamics_files/rotating%2520with%2520cosntant%2520angular%2520velocity.png) |
A particel starts at a distance R from the center of the disk.
The forces acting on it are frction and weght (and vertical reaction of
the disk). We observe that friction actually is a force that accelrate
the body |
MOTION ON A ROTATING DISK WITH CONTANT ANBULAR MOMENTUM |
![Motion with constant L](2 dimensional motiona/Motion-with-constant-L.gif) |
SIMILAR TOTHE ABOVE, NOW THE ANGULAR VELOCITY OF THE SYSTEM
REMAINS CONSTANT. AT FIRTST THE FRICTION ACTS AS ACCELRATING AGENT BUT
LATER IT BECOMS DECELRATING. |
FOUCAULT'S PENDULUM |
![FOUCAUTL](excel%20dynamics_files/Foucault-Pendulum.gif) |
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