Mechanics Lab | A Simple Pendulum & a Small Magnet Underneath

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Homework Help Overview

The discussion revolves around the mechanics of a simple pendulum and the influence of a magnetic force acting on it. The original poster presents measurements of the period and distance of the pendulum, expressing uncertainty about how to incorporate the magnetic force into the period formula.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the relationship between the pendulum's period and the magnetic force, questioning how to integrate the magnetic force into the existing period formula. There are discussions about the need for additional parameters such as the mass of the bob and the length of the pendulum.

Discussion Status

Participants are actively engaging with the problem, providing references to derivations and discussing the necessary components for the calculations. Some guidance has been offered regarding the relationship between forces and the period, though there remains a lack of consensus on how to proceed with the integration of the magnetic force and its relation to distance.

Contextual Notes

There is mention of needing the mass of the bob and the length of the pendulum, but the original poster expresses confusion about their relevance. The discussion also highlights the challenge of combining forces with different units, as well as the need for a linear relationship to graph the results.

Curious_Student
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Homework Statement
A pendulum made of an iron bob which is hanged at the bottom tip of a rod (rods' mass can be neglected) where connected to an angular ratio sensor, mesuring with a MultiLab program (just the period of time according to its' harmonic motion, taking avg. of 10 swings-cycles pick-to-pick, devided by 10). Underneath the pendulums' bob there is a small magnet which applies a force in addition to the gravity downwards and impacts the period of time when swinging.
I placed the small magnet underneath on an hydraulic stand for adjusting the distance between the magnet and bob (intervals of 1 mm because the magnet is weak), so that the length of the pendulum is constant, unchanged.

The Quest: is to find pendulums' Period Time dependence on distance between bob and the magnet, then find magnets' force as function of the distance, from measured periiod times.
Relevant Equations
Considering it as a simple mathematical pendulum:

T= 2pi*root(l/g)
linear: T^2 = 4pi^2/g*l


This is all the info. I got, no such magnetic formulas.
I think the way they direct is to treat the Magnetic Force as a Variable (x) and adding it and the distance, somehow.. to the formula above,
Because as we did before (finding period time as function of length T^2(l)), I was told to do in a similar way, building a linear graph and finding the value from the relation.

But im stuck..
How can I add the magnets' force and its' distance into this formula?
Anything else conastant (length,pi,g..)

If anybody can to just throw me a clue.. I am really confused.
I have measurements of period time and distances that's all:
T (sec)​
D (m)​
0.9​
0.008​
0.91​
0.009​
0.97​
0.01​
0.98​
0.011​
1.06​
0.012​

I thought about adding the magnetic force like: T=2π*√l/(g+x) but have no clue how to integrate the distance there,
I don't know even how to start..

Appreciate any kind of help,
Thanks in advance!
 
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gneill said:
Take a look at the derivation of the period of a simple pendulum. For example here:

http://dev.physicslab.org/Document.aspx?doctype=3&filename=OscillatoryMotion_PendulumSHM.xml

See if you can't find a way to work the magnetic force into that. I think you can assume that over the range where the magnetic force is effective it is parallel to the gravitational force.
I see, but I am sorry, still don't get it .. how to find the magnetic force and its' vertical distance relation as a function of the period time? all i have is the period time and distance correlation measurements..
Can you be more specific please? and yes I would take the magnet force as parallel
to g force only.
 
You'll need the mass of the bob, or at lest the period of the pendulum when there's no magnet operating; the mass of the bob can be extracted from that information. You'll also need the length of the pendulum.

If you look at the page I referenced, the restoring force is give by ##m g \sin(\theta)##. If you add a value for the magnetic force, ##F_m## then that restoring force becomes: ##\left(m g + F_m \right) \sin(\theta)## . Complete the derivation in the same fashion they did. Solve for ##F_m##.
 
I do have the mass of the bob, but it cancles out:
1578769069534.png
so why do i need it? and how to deal the length if its constant?
If I understand you right, you suggest to add Fm to dominator as: T= 2π√[l/(g+Fm)] like I've mentioned and to rescue Fm right? but where should the distance from the magnet be placed into consideration.
I should find some linear relation, to form a graph for T(magnet distance) and get the Fm from there somehow. Still don't get it.. I'm sorry.
 
g is an acceleration while Fm is a force. You cannot sum them in that fashion.

In the derivation where they introduce the restoring force:

##M g \sin(\theta) = k_s L \theta##

you introduce the additional magnetic force:

##\left( M g + F_m \right) \sin(\theta) = k_s L \theta##

then carry on. The final expression for the period will involve L, M, Fm, and g.

Solve it for Fm then you can plot Fm versus D.
 
gneill said:
g is an acceleration while Fm is a force. You cannot sum them in that fashion.

In the derivation where they introduce the restoring force:

##M g \sin(\theta) = k_s L \theta##

you introduce the additional magnetic force:

##\left( M g + F_m \right) \sin(\theta) = k_s L \theta##

then carry on. The final expression for the period will involve L, M, Fm, and g.

Solve it for Fm then you can plot Fm versus D.
ok, thank you
 

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