2008 us physics olympiad pendulum in electric field

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SUMMARY

The discussion centers on solving question B2 from the 2008 US Physics Olympiad, specifically regarding the motion of a pendulum in an electric field. The key concepts include the derivation of simple harmonic motion (SHM) and the period of oscillation. The participant initially struggled with setting up the differential equation and understanding the forces involved. Ultimately, the solution involves recognizing the effective gravitational force acting at an angle due to the electric field, leading to the correct mathematical formulation of SHM.

PREREQUISITES
  • Understanding of simple harmonic motion (SHM)
  • Familiarity with pendulum dynamics
  • Knowledge of electric fields and forces
  • Ability to set up and solve differential equations
NEXT STEPS
  • Study the derivation of the period of a pendulum under varying forces
  • Learn about the effects of electric fields on charged pendulums
  • Explore coordinate transformations in physics problems
  • Practice setting up differential equations for oscillatory motion
USEFUL FOR

Students preparing for physics competitions, educators teaching mechanics, and anyone interested in the dynamics of pendulums influenced by external forces.

timetraveller123
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1. Homework Statement

i was solving the 2008 semi final us physics olympiad paper when i got stuck on question B2 in part 2
http://www.aapt.org/Programs/contests/upload/olympiad_2008_semi-final_soln.pdf
the link takes you a pdf with questions and solution however i don't understand the soution to B2 i get part ai) but not part aii) how do you prove the motion is simple harmonic and i am not sure how they derive the period in that way

Homework Equations


T = 2π/ω
f = q E
V = Ed
f = mg
sin θ ≈ tan θ ≈ θ

The Attempt at a Solution


i tried to turn the coordinate system such that the equilibrium is in a vertical position but failed miserably i also tried taking a force approach and also failed i have no idea how to start please help
 
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vishnu 73 said:
i tried to turn the coordinate system such that the equilibrium is in a vertical position but failed miserably i also tried taking a force approach and also failed i have no idea how to start please help
Please show us your attempt. If you just say that you attempted it we have no way of knowing where you went wrong.

vishnu 73 said:
sin θ ≈ tan θ ≈ θ
Note that this is true only for small angles. The way the problem is stated, there is no guarantee that ##\theta_0## or ##\theta## is small. What is small in the problem is the difference ##\theta - \theta_0##.
 
Orodruin said:
Please show us your attempt. If you just say that you attempted it we have no way of knowing where you went wrong.Note that this is true only for small angles. The way the problem is stated, there is no guarantee that ##\theta_0## or ##\theta## is small. What is small in the problem is the difference ##\theta - \theta_0##.
the problem is i know no way of how to start
i don't even how to set up the differential equation for this problem and i meant θ - θ0 is small not the actual angle itself
the reason why i say that is that because the force due to electric field and gravity are constant throughout the motion then why should there be a restoring force unlike the spring oscillator in which there is a restoring force thus there is SHM
 
Last edited:
vishnu 73 said:
the problem is i know no way of how to start
i don't even how to set up the differential equation for this problem and i meant θ - θ0 is small not the actual angle itself
the reason why i say that is that because the force due to electric field and gravity are constant throughout the motion then why should there be a restoring force unlike the spring oscillator in which there is a restoring force thus there is SHM

Well, you said that you wanted to try to write the problem in a rotated coordinate system. What do you get when you do that?

Also, the gravitational force on a standard pendulum is constant - yet it performs SHM for small angles. Do you understand why?
 
Orodruin said:
Well, you said that you wanted to try to write the problem in a rotated coordinate system. What do you get when you do that?

Also, the gravitational force on a standard pendulum is constant - yet it performs SHM for small angles. Do you understand why?

oh wait i forgot that while force remains the same the tangential components and the radial components of the force change let me try again give me some time
 
OK now i get the solution what it essentially means is that there is combined effective "gravity" pointing not directly down but at an angle of θo and then when you do the coordinate transformation such that the effective "gravity" is pointing directly down you get the equation from then on its just mathematical manipulation am i right?
 

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