Tangential and radial acceleration

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SUMMARY

The discussion centers on the concepts of tangential and radial acceleration in a physical pendulum scenario involving a triangle with fixed-length rods and attached masses. The initial condition states that the system starts at rest, leading to zero radial acceleration due to the fixed lengths of the rods. Participants clarify that while radial acceleration is absent at the moment of release, tangential acceleration can still be present as the system begins to swing. The analogy of a book on a table illustrates that gravitational forces exist without causing movement in a static scenario.

PREREQUISITES
  • Understanding of basic physics concepts such as acceleration, forces, and motion.
  • Familiarity with the principles of pendulum motion and angular acceleration.
  • Knowledge of circular motion and the distinction between radial and tangential acceleration.
  • Basic grasp of gravitational forces and their effects on stationary objects.
NEXT STEPS
  • Study the principles of angular acceleration in physical pendulums.
  • Learn about the relationship between tangential and radial acceleration in circular motion.
  • Explore examples of fixed-length pendulum systems and their motion dynamics.
  • Investigate the effects of gravitational forces on stationary and moving objects.
USEFUL FOR

Students of physics, educators explaining dynamics, and anyone interested in understanding the mechanics of pendulum systems and the interplay between different types of acceleration.

magnas
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Hi,
I am reviewing a problem with the associated solution and there is something i don t understand.
Imagine a triangle with vertices l, masses m are attached to the two end of the vertices and on the top end vertice there is a pivot so that the triangle can swing. We start with the triangle at rest and one of the rod is vertical.
Question: what is the accelerations of the masses (the two following words are in italics) just after it is released?
What i don t understand is the following:
"since v=0 at the start , the radial accelerations are zero"(quote from the solution). And then, the problem is treated as there is no radial acceleration at all, while considering a tangential acceleration. How can we consider a tangential acceleration without a radial/centripetal acceleration?
If this is possible, could you explain me and clarify with an example?
Thank you.
 
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magnas said:
Hi,
I am reviewing a problem with the associated solution and there is something i don t understand.
Imagine a triangle with vertices l, masses m are attached to the two end of the vertices and on the top end vertice there is a pivot so that the triangle can swing. We start with the triangle at rest and one of the rod is vertical.
Question: what is the accelerations of the masses (the two following words are in italics) just after it is released?
What i don t understand is the following:
"since v=0 at the start , the radial accelerations are zero"(quote from the solution). And then, the problem is treated as there is no radial acceleration at all, while considering a tangential acceleration. How can we consider a tangential acceleration without a radial/centripetal acceleration?
If this is possible, could you explain me and clarify with an example?
Thank you.

So you have something that looks like this?
attachment.php?attachmentid=53984&stc=1&d=1355690605.gif


If the 'rods' forming the triangle are of fixed length, then the masses are constrained to follow the circular arc indicated, and there's no change in length of r possible. So no radial acceleration. This is not to say that centripetal forces will not happen, just that they cannot make the masses accelerate due to the fixed lengths of the triangle.

It's like a book lying on a table; There's a gravitational force acting on it, and g is still in business, but still the book does not move downwards.

You might consider treating the object as a physical pendulum and determine its angular acceleration first.
 

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