Solving the Falling Pencil: How Small is the Degree Difference?

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Discussion Overview

The discussion revolves around the theoretical scenario of an ideal pencil balanced on its tip and the conditions under which it falls over. Participants explore the relationship between the initial angle of the pencil and the time it takes to fall, specifically questioning how small the angle difference from vertical can be if the pencil takes 15 minutes to hit the ground.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that an object balanced on a point is inherently unstable and will begin to fall immediately if it is not perfectly vertical.
  • Others suggest that the time it takes to fall could be analyzed using Newton's laws for a rotating system, considering the torque due to gravity acting on the pencil's center of mass.
  • A participant mentions that the scenario described could be treated as a stability-analysis problem, questioning how small the perturbation must be for the mean time to fall to be 15 minutes.
  • One participant proposes a model similar to an inverted pendulum to estimate the time it takes for the pencil to fall, suggesting that the math involves solving integrals related to angular displacement.
  • Another participant emphasizes that under ideal conditions, the pencil would either fall immediately or not at all, referencing concepts like Norton's dome to illustrate the complexities of balanced objects.
  • Some participants express skepticism about the feasibility of the 15-minute fall time, suggesting it seems excessively long for a balanced pencil.
  • There are discussions about numerical methods and approximations to estimate the initial angle, with some participants suggesting computational approaches to solve the problem.

Areas of Agreement / Disagreement

Participants generally disagree on the implications of the scenario, with some asserting that the pencil would fall immediately while others explore the possibility of a delayed fall under idealized conditions. The discussion remains unresolved regarding the exact relationship between the angle and the fall time.

Contextual Notes

Participants acknowledge that the discussion is framed under ideal conditions, excluding real-world factors such as air resistance and vibrations. There is also uncertainty regarding the mathematical treatment of the problem, with various models proposed but no consensus on the correct approach.

Who May Find This Useful

This discussion may be of interest to those studying dynamics, stability analysis, or mathematical modeling in physics, as well as individuals curious about theoretical scenarios involving balance and motion.

malicor
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hi,

i've got a little complicated question, let's see if i can formulate it in an understandable way.

imagine there's an (ideal) pencil, standing on its (ideal) tip. if it would stand at 90degree to the (ideal) table, it would never fall.

now the question is, if it doesn't stand at 90degrees, and therefor does fall after an amount of time, and that amount is 15 minutes, how big is the difference of the degree to the table to 90degrees.
(it should be pretty small, i said, it's less than 10^-1000000, a friend of me bets it's more.)

can anyone help ? (needn't be an exact calculation, an estimation would do)

regards, malicor
 
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An object balanced on a point is "unstable" - any change at all from exactly balanced will cause it to start falling immediately. The amount of time to hit the ground can be worked out for ideal conditions - gravity provides a torque at the pencil's center of mass which depends on the current angle. The pencil rotates about it's point.

This is Newton's Laws for a rotating system - write it out and solve for initial angular displacement.

IRL: even an ideal pencil, perfectly balanced, will be subject to small random forces - vibrations, air-gusts etc. How long it takes to begin falling is a matter for statistics.
 
malicor said:
hi,

i've got a little complicated question, let's see if i can formulate it in an understandable way.

imagine there's an (ideal) pencil, standing on its (ideal) tip. if it would stand at 90degree to the (ideal) table, it would never fall.

now the question is, if it doesn't stand at 90degrees, and therefor does fall after an amount of time, and that amount is 15 minutes, how big is the difference of the degree to the table to 90degrees.
(it should be pretty small, i said, it's less than 10^-1000000, a friend of me bets it's more.)

can anyone help ? (needn't be an exact calculation, an estimation would do)

regards, malicor

You're asking if an object, ideally balanced, takes 15 minutes before it falls over, how off true was it?

There is no way to answer this.

Under ideal conditions, it will either fall immediately or never. Anything less than ideal conditions comes down to the margin of error in the object, the environment or the accuracy of setup.
 
There are several ways to treat it - it's just not clear which one applies here. It looks like malicor and friend have a misconception to overcome first.

The pencil described would start to fall immediately - because it is off center.
But there would be a hang-time effect (15mins seems a tad long for this).

If it starts perfectly balanced, then it is a stability-analysis problem and you can ask about the mean-time to start falling under a very small perturbation - then ask how big the perturbation has to be for the mean-time to be 15mins.

The exercise normally given to students is for an irregular object spinning about it's middle axis - how long before it tumbles?

But as you say - IRL, for a pencil: all bets are off.
 
In the case of a pencil, it would start to slide and fall more quickly about half way over.

If the pencil couldn't slide, and assuming you want the time it takes for the pencil to fall down on its side, then the problem is similar to an inverted pendulum made of a solid uniform rod, which would be the equivalent of a simple inverted pendulum (all of the mass at the end of the pendulum) 2/3rd the length of the rod. The math involves solving an integral, defining θ = 0 when a pendulum is pointed straight down, you'd want to know the time it takes for the pendulum to fall from θ0 to π/2, and adjust or solve for θ0 close enough to π to get the time you're looking for, using the math from this wiki article:

Pendulum_Arbitrary-amplitude_period.htm
 
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If we took the ideal case of a pencil of length l, = .1 m, and mass m then ?,

m g l sin(θ) = 1/3 m l^2 θ,tt = m g l θ for small θ -->

θ,tt/θ = 3g/l = c^2

This is solved here,

http://www.wolframalpha.com/

with input,

d^2x/dt^2 * 1/x = c^2

and output,

x(t) = d_1*exp[c*t] + d_2*exp[-c*t] or

θ(t) = d_1*exp[c*t] + d_2*exp[-c*t]

I think we can throw out the second term.

For t = 0, θ(0) = d_1 = θ_o

θ(t) = θ_o*exp[c*t] For t = 15 minutes θ becomes of order unity -->

exp[c*t] = about exp[15,400] which implies θ_o is pretty small?

Any mistakes?
 
DaveC426913 said:
Under ideal conditions, it [an object, ideally balanced] will either fall immediately or never.

This is moot, even in Newtonian mechanics, for an arbitrary balanced object. Google for "Norton's dome". There was a recent PF thread about it.

Note, this does NOT apply to an idealised pencil toppling - Norton's dome is not spherical.
 
hello

there's some misunderstandings here, which i will try to remove

first: the whole (theoretical) experiment shall be under ideal conditions, no wind, no air gusts, (not even a real pencil, but just a mass).

second: we're looking at the amount of time from the start situation to where the 'pencil' hits the ground. of course it starts falling immediately, but the time until it 'lands' is what we're after, and this time shall be 15 minutes.

third: fifteen minutes is an awefull high amount of time, the difference of the starting degree to 90degree will be like 0,000000000000000000000000000000000000000000something

in fact we suspect it's that small, that it's less than 0,000000[... insert one million more '0']0000001

this is actual the question, is it less than 1/10^1000000 or not. (that it's small we know already)

a formula wouldn't help me much, since I'm in no way a physician (but a computer scientist), and even if i had a formula i couldn't solve it.
we're pretty sure that it'll be hard to solve exactly, because it's a that small number, but quite sure that it'll be possible to solve the question "is it less than 1/10^1000000 due to some approximation strategies)

merry xmas to all of you :)
 
http://demonstrations.wolfram.com/FallingStick/
... would be one interpretation of what you've said.
At the bottom is the equation of motion ... see how complex it gets?

In a simpler model, where you just call it a point mass on a massless but rigid pole, and the pivot is not allowed to slide, you get something more like:
[tex]r\frac{d\theta}{dt} = g\sin\theta[/tex]... where theta is measured from upright.

Solutions go something like this.

I'm in no way a physician
- indeed - nor a physicist. (A "physician" is a medical doctor.) As a computer scientist you should be able to solve it numerically using a computer program xD

Also look at a mass sliding over the top of a sphere.
https://www.physicsforums.com/showthread.php?t=147252
... as you look through these you'll notice that time is not often asked about.

One strategy would be to divide the angle of the fall into N small parts size [itex]\Delta \theta = \pi/2N[/itex], and treat the acceleration as constant over each part. This will give you N data points, for which you can get N accelerations - you can find the change in speed from acceleration and Δθ (knowing that the initial speed is zero), and so find the time to traverse each section. Add up the times for the overall time to fall.

Get a computer to do it.
 
  • #10
Spinnor said:
If we took the ideal case of a pencil of length l, = .1 m, and mass m then ?,

m g l sin(θ) = 1/3 m l^2 θ,tt = m g l θ for small θ -->

θ,tt/θ = 3g/l = c^2

This is solved here,

http://www.wolframalpha.com/

with input,

d^2x/dt^2 * 1/x = c^2

and output,

x(t) = d_1*exp[c*t] + d_2*exp[-c*t] or

θ(t) = d_1*exp[c*t] + d_2*exp[-c*t]

I think we can throw out the second term.

For t = 0, θ(0) = d_1 = θ_o

θ(t) = θ_o*exp[c*t] For t = 15 minutes θ becomes of order unity -->

exp[c*t] = about exp[15,400] which implies θ_o is pretty small?

Any mistakes?

Again using,

http://www.wolframalpha.com/

input,

exp[15400],

output,

1.36X10^6688 --> θ_o = [1.36X10^6688]^-1 = 7.35X10^-6689 radians give or take θ_o *10^100 .

I think you win the bet (but as others have said you could never do the experiment).

Edit, oops! I reread your post and your guess was much smaller then the actual value.
 
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