Analyizing the dynamics of a pendulum hanging in an accelerating car

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SUMMARY

The discussion centers on analyzing the dynamics of a pendulum hanging in an accelerating car, specifically deriving the maximum angle \varphi_{max} through which the weight swings using an inertial reference frame. The established equation for maximum angle is \varphi_{max} = 2*arctan(A/g), where 'A' is the acceleration of the car and 'g' is the acceleration due to gravity. Participants debated the appropriate reference frame for analysis, clarifying that the challenge is to solve the problem using Newton's 2nd Law in an inertial frame, as opposed to a non-inertial frame typically used in textbooks.

PREREQUISITES
  • Understanding of Newton's 2nd Law of Motion
  • Familiarity with inertial and non-inertial reference frames
  • Basic knowledge of potential and kinetic energy concepts
  • Ability to draw and interpret free body diagrams
NEXT STEPS
  • Study the derivation of \varphi_{max} = 2*arctan(A/g) using Newton's 2nd Law
  • Research the differences between inertial and non-inertial reference frames
  • Explore energy conservation principles in pendulum motion
  • Practice drawing free body diagrams for pendulum systems in various reference frames
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Physics students, educators, and anyone interested in classical mechanics, particularly those studying pendulum dynamics and reference frame analysis.

gatechphysics
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Homework Statement



A small weight of mass 'm' hangs from a string in an automobile. Initially, the car is at rest with the weight hanging vertically. Then, the car SUDDENLY accelerates to a rate 'A'. Find the maximum angle \varphi_{max} through which the weight swings by analyzing the motion of the pendulum WITHIN AN INERTIAL REFERENCE FRAME.

Homework Equations



In my book they derive the solution to this problem using an analysis within a NON-INERTIAL reference frame. The answer is:

\varphi_{max} = 2*arctan(A/g) (1)

If you instead try to find the static angle the pendulum makes with the vertical in a car that is already accelerating at a constant rate A you will find that the static angle is half of the maximum angle given by equation (1).

The problem we are being asked though is to try and derive equation (1) using a non-inertial frame and I cannot figure out how to carry out the calculation.

The Attempt at a Solution



I am assuming that the best way to solve this problem is to use a classic Newton's 2nd Law analysis using an inertial reference frame that is stationary with respect to the car. Or is it better to solve this problem using an energy approach? Note that when I say an energy approach I do NOT mean forming the Lagrangian and solving that way. In my class we have only been doing classical analyses using Newton's formulation of mechanics so Lagrangian and Hamiltonian analyses are not acceptable for my class. By energy approach I simply mean that the weight increases in potential energy as it approaches the max angle, thus the corresponding increase in the kinetic energy of the bob must equal the increase in grav. potential so maybe there is a way to connect the kinetic energy of the bob with the acceleration of the car?

By the way this is not a homework question. Instead my professor challenged us to attempt to solve this problem in an inertial frame. I hope that I am not posting this question in the wrong forum. If I am I am sorry but I am new here so just let me know and I will move it.
 
Last edited:
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In the part 2 you say "derive equation (1) using a non-inertial frame" which contradicts what you said in part 1. So I am confused now. Basically what specific reference frame are you deriving this in... Outside of the car, inside of the car, or the bob's frame of reference.
 
nickjer said:
In the part 2 you say "derive equation (1) using a non-inertial frame" which contradicts what you said in part 1. So I am confused now. Basically what specific reference frame are you deriving this in... Outside of the car, inside of the car, or the bob's frame of reference.

Sorry. It should be "inertial frame". In my textbook the solution is given for a non-inertial frame. The challenge was posed to us to try to solve this problem within an inertial frame. Thanks for letting me know about that typo. I will edit it right away.
 
gatechphysics said:


1. Homework Statement


A small weight of mass 'm' hangs from a string in an automobile. Initially, the car is at rest with the weight hanging vertically. Then, the car SUDDENLY accelerates to a rate 'A'. Find the maximum angle \varphi_{max} through which the weight swings by analyzing the motion of the pendulum WITHIN AN INERTIAL REFERENCE FRAME.

Homework Equations



In my book they derive the solution to this problem using an analysis within a NON-INERTIAL reference frame. The answer is:

\varphi_{max} = 2*arctan(A/g) (1)

If you instead try to find the static angle the pendulum makes with the vertical in a car that is already accelerating at a constant rate A you will find that the static angle is half of the maximum angle given by equation (1).

The problem we are being asked though is to try and derive equation (1) using a inertial frame and I cannot figure out how to carry out the calculation.

The Attempt at a Solution



I am assuming that the best way to solve this problem is to use a classic Newton's 2nd Law analysis using an inertial reference frame that is stationary with respect to the car. Or is it better to solve this problem using an energy approach? Note that when I say an energy approach I do NOT mean forming the Lagrangian and solving that way. In my class we have only been doing classical analyses using Newton's formulation of mechanics so Lagrangian and Hamiltonian analyses are not acceptable for my class. By energy approach I simply mean that the weight increases in potential energy as it approaches the max angle, thus the corresponding increase in the kinetic energy of the bob must equal the increase in grav. potential so maybe there is a way to connect the kinetic energy of the bob with the acceleration of the car?

By the way this is not a homework question. Instead my professor challenged us to attempt to solve this problem in an inertial frame. I hope that I am not posting this question in the wrong forum. If I am I am sorry but I am new here so just let me know and I will move it.

It wouldn't allow me to edit my original post so please note the corrected sentence in bold in the above quote.
 
I thought the inertial reference frame was outside the car and not inside the car since that frame was accelerating. I only ask because you also say "I am assuming that the best way to solve this problem is to use a classic Newton's 2nd Law analysis using an inertial reference frame that is stationary with respect to the car."

Also, I recommend drawing a free body diagram to help you solving this.
 
Last edited:
nickjer said:
I thought the inertial reference frame was outside the car and not inside the car since that frame was accelerating. I only ask because you also say "I am assuming that the best way to solve this problem is to use a classic Newton's 2nd Law analysis using an inertial reference frame that is stationary with respect to the car."

Also, I recommend drawing a free body diagram to help you solving this.

I don't understand your question. If the frame was inside the car it would cease to be an inertial frame. The question is to solve the problem in an inertial frame. Not necessarily any particular inertial frame. Given this, I was simply assuming in the quote above that an inertial frame that was stationary with respect to the car (e.g. a reference frame attached to the surface of the Earth which sees the pendulum and car accelerating past at a rate A) was the best inertial frame to work within. This assumption might be incorrect.
 

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