Pendulum Point of Suspension & Acceleration: Time Period Explanation

  • Thread starter nishant
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In summary, the question of whether a pendulum's time period will increase or decrease when its point of suspension is moving upwards with acceleration is a matter of perspective. While some use pseudo force to calculate this, it should only be used when the observer is also moving with the point of suspension. In reality, the acceleration of the pendulum is the determining factor, and according to general relativity, it can be treated as if it were in a gravitational field of "g+a." However, this does not take into account the effects of air resistance. Alternatively, one could use Newton's laws with an inertial frame of reference to arrive at the same result. Overall, the time period of the pendulum can be calculated using the formula T
  • #1
nishant
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if a pendulum's point of suspension is moving upwards with acceleration {a},then the time period of the simple pendulum will increase or decrease?{many people are using pseudo force to calculate this question,but that is to be used only when we are also moving with the point of suspension,but no where in the actual question is it written theat way?"
 
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  • #2
The point of view is not important here. The fact that the pendulum is accelerating is key. General relativity says that we can not tell the difference between the effects of being in a gravitational field and the effects of actual acceleration. If the pendulum accelerates upward, then the pendulum will behave exactly as it would in a gravitational field of "g+a."

Of course this will be ignoring the effects of air resistance.
 
  • #3
OK, if you want to prove it the hard way you can apply Newton's laws with the observer in an inertial frame of reference. Vertically, Ty - mg = ma. Use this to determine Tx in terms of displacement and you'll arrive at the same result

[tex]T = 2\pi \sqrt{\frac{L}{g + a}}[/tex]

On the other hand virtual gravity (grav. acceleration = g+a) is a convenient abstraction that you could use.
 

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