What are your favourite physics/mathematics misconceptions?

  • #1
ergospherical
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Maybe there's even a few that myself or others here still believe... bonus points if you get one of these. I'll start with one I see a lot... 😌

1. "##\mathbf{F} = m\ddot{\boldsymbol{x}}## defines force".
This is backwards, and would rid the second law of any actual content! Rather, the function ##\mathbf{F} = \mathbf{F}(\boldsymbol{x}, \dot{\boldsymbol{x}}, t)## constitutes a definition of the physical system and must be determined experimentally (e.g. the law of gravitation).

Do your worst! 😜
 
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  • #2
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Not a misconception but a confusion. We were taught r theta phi in math. But American physics now uses the r phi theta convention to be in sync with European physics.
 
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  • #3
ergospherical
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Not a misconception but a confusion. We were taught r theta phi in math. But American physics now uses the r phi theta convention to be in sync with European physics.
That reminds me, here's a test to see whether you're a physicist or a mathematician at heart...
if ##f(x,y) = xy##, what is ##f(r,\theta)##? :smile:
 
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  • #4
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##R^2 sin(\theta) cos(\theta)##

or

##1/2 R^2 sin(\theta/2)##

i think i got that right. Its been roughly 50 years.
 
  • #5
ergospherical
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Yay, you are a physicist! 🥳 although the second one ought to be ##\dfrac{1}{2}R^2 \sin{2\theta}##
(the alternative answer was ##r\theta## :smile:)
 
  • #7
PeroK
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That Newton thought the speed of light was infinite.

That classical physics was doing fine until Einstein stuck in an unwelcome oar.

That for years no one understood relativity except uncle Albert.

That QM is like Zen Buddhism.

That consciousness causes collapse.

That the classical model of the atom was hunky dory until the QM pioneers decided it should be weirder.
 
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  • #8
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To me it was clerarly ##r\theta##.

I hate that people still try to figure out what ##0^{-1}## is, or why it is forbidden. Why don't they ask why ## i ## isn't real, or why the set of all sets isn't a set, or why a bird isn't a fish? That is exactly the same quality.
 
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  • #9
PeroK
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That reminds me, here's a test to see whether you're a physicist or a mathematician at heart...
if ##f(x,y) = xy##, what is ##f(r,\theta)##? :smile:
Exchanging the roles of ##\phi## and ##\theta## in my use of spherical coordinates was a seminal moment in my transition from amateur hack mathematician to amateur hack physicist!
 
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  • #10
caz
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why a bird isn't a fish?
Amusing, a banana is a type of fish.
Terry Pratchett said:
“Yes, sir, but the Librarian likes bananas, sir."
"Very nourishin' fruit, Mr Stibbons."
"Yes, sir. Although, funnily enough it's not actually a fruit, sir."
"Really?"
"Yes, sir. Botanically, it's a type of fish, sir. According to my theory it's cladistically associated with the Krullian pipefish, sir, which of course is also yellow and goes around in bunches or shoals."
"And lives in trees?"
"Well, not usually, sir. The banana is obviously exploiting a new niche."
"Good heavens, really? It's a funny thing, but I've never much liked bananas and I've always been a bit suspicious of fish, too. That'd explain it.”
 
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  • #11
jack action
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1. "##\mathbf{F} = m\ddot{\boldsymbol{x}}## defines force".
This is backwards, and would rid the second law of any actual content! Rather, the function ##\mathbf{F} = \mathbf{F}(\boldsymbol{x}, \dot{\boldsymbol{x}}, t)## constitutes a definition of the physical system and must be determined experimentally (e.g. the law of gravitation).
I guess you will have to define "definition". According to Feynman:
The Newtonian statement above [##F = ma##], however, seems to be a most precise definition of force, and one that appeals to the mathematician; nevertheless, it is completely useless, because no prediction whatsoever can be made from a definition. One might sit in an armchair all day long and define words at will, but to find out what happens when two balls push against each other, or when a weight is hung on a spring, is another matter altogether, because the way the bodies behave is something completely outside any choice of definitions.

[...]

What is a chair? Well, a chair is a certain thing over there … certain?, how certain? The atoms are evaporating from it from time to time—not many atoms, but a few—dirt falls on it and gets dissolved in the paint; so to define a chair precisely, to say exactly which atoms are chair, and which atoms are air, or which atoms are dirt, or which atoms are paint that belongs to the chair is impossible. So the mass of a chair can be defined only approximately. In the same way, to define the mass of a single object is impossible, because there are not any single, left-alone objects in the world—every object is a mixture of a lot of things, so we can deal with it only as a series of approximations and idealizations.

The trick is the idealizations. To an excellent approximation of perhaps one part in 1010, the number of atoms in the chair does not change in a minute, and if we are not too precise we may idealize the chair as a definite thing; in the same way we shall learn about the characteristics of force, in an ideal fashion, if we are not too precise. One may be dissatisfied with the approximate view of nature that physics tries to obtain (the attempt is always to increase the accuracy of the approximation), and may prefer a mathematical definition; but mathematical definitions can never work in the real world. A mathematical definition will be good for mathematics, in which all the logic can be followed out completely, but the physical world is complex, as we have indicated in a number of examples, such as those of the ocean waves and a glass of wine. When we try to isolate pieces of it, to talk about one mass, the wine and the glass, how can we know which is which, when one dissolves in the other? The forces on a single thing already involve approximation, and if we have a system of discourse about the real world, then that system, at least for the present day, must involve approximations of some kind.

This system is quite unlike the case of mathematics, in which everything can be defined, and then we do not know what we are talking about. In fact, the glory of mathematics is that we do not have to say what we are talking about. The glory is that the laws, the arguments, and the logic are independent of what “it” is.
 
  • #12
caz
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That for years no one understood relativity except uncle Albert.
or Eddington and Einstein, or Eddington, Einstein and Hilbert
 
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  • #13
hutchphd
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It took 30 yrs of looking at the bow wake of a boat before I realized how it was really not the same as the shock from a supersonic aircraft.
Boats always move at (water) mach 3
 
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  • #14
ergospherical
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I guess you will have to define "definition". According to Feynman:
The content of the law is that one can always choose a function ##\mathbf{F}## such that the motion ##\boldsymbol{\gamma}(t)## which is the unique solution of ##\ddot{\boldsymbol{x}} = \dfrac{1}{m}\mathbf{F}(\boldsymbol{x}, \dot{\boldsymbol{x}}, t)##, consistent with the ##6n## initial conditions, agrees with experiment. This is to say that the form of this function ##\mathbf{F}## must be supplied from some force law.

(Defining force as ##m\mathbf{a}## is nothing but a tautology!)

It took 30 yrs of looking at the bow wake of a boat before I realized how it was really not the same as the shock from a supersonic aircraft.

##2\sin^{-1}(1/3)## is the magic number, so long as the water is deep...
proof left as an exercise to the reader 😬
 
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  • #15
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##2\sin^{-1}(1/3)## is the magic number, so long as the water is deep...
proof left as an exercise to the reader 😬
There is only one magical number, and it is ##1/137##.
 
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  • #16
berkeman
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1630187576202.png

https://i.pinimg.com/originals/ab/73/58/ab7358bb4d432a992222d6450d90d11f.png
 
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  • #17
DennisN
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Though it's not pure physics/mathematics there has been a number of huge misconceptions in the history of astronomy:
 
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  • #18
mathwonk
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wow! "alternative answer" to post #3?, Surely there is only one "correct" answer. namely, if f(x,y) = xy, and the function taking (r, theta) to (x,y), where x = r.cos(theta), y = r.sin(theta), is called g, then (fog)(r, theta) = r^2.sin(theta).cos(theta). but f(t,u) = tu, f(a,b) = ab, and f(r, theta) = r.theta.

maybe one could claim that f(x(r, theta),y(r, theta)) = r^2.cos(theta).sin(theta).

this reminds me of a difficulty i had in reading physics articles as a young person. the authors took for granted things that were not stated. mathematicians live by what they say.
 
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  • #19
ergospherical
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defo, the physicist is a lazy animal and instead of writing ##\tilde{f}(r,\theta) \equiv x(r,\theta) y(r,\theta)##, they will happily drop the tilde and pretend ##f## and ##\tilde{f}## are 'the same' :smile:
 
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  • #20
caz
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Yay, you are a physicist! 🥳 although the second one ought to be ##\dfrac{1}{2}R^2 \sin{2\theta}##
(the alternative answer was ##r\theta## :smile:)
I thought that a mathematician would first prove that f exists.
 
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  • #21
mathwonk
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this illustrates one of my over-generalizations: mathematicians are often more precise at saying what they mean, but physicists are often more likely to understand correctly what is actually going on.
 
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  • #22
phinds
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There is only one magical number, and it is ##1/137##.
No, it's 42
 
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  • #23
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this reminds me of a difficulty i had in reading physics articles as a young person. the authors took for granted things that were not stated. mathematicians live by what they say.

Exactly. The difference between mathematics and physics is not so much in what is taught, and even less in the instruments, they use. The main difference is simply that it is another language.
 
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  • #25
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That Newton thought the speed of light was infinite.
I believe that in Newton's speculations he declared this absurd. In short, he knew his model was wrong but couldn't come up with anything better. And the math worked for all practical purposes of his time. That may have been one of the reasons he was reluctant to publish the Principia.

It is fairly common for a wrong model to lead to (in this case almost) correct math. This is a good reason to not take models all that seriously.
 

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