Understanding the Concept of Infinity as a Reference in Physics: Explained

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Discussion Overview

The discussion revolves around the concept of using infinity as a reference point in physics, particularly in the contexts of electrostatics and gravitational potential energy. Participants explore the implications and physical meaning of this choice, questioning its legitimacy and utility in calculations.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants express confusion about using infinity as a reference point, questioning how it can be meaningful when its location is unknown.
  • Others argue that "a point at infinity" is simply a point far enough away that further distance makes negligible difference to the system, suggesting it has a physical meaning in certain contexts.
  • One participant mentions that the potential energy approaches a maximum or minimum at infinity, depending on the nature of the charges involved.
  • There is a discussion about defining electric potential, with one definition provided for a point charge, indicating that it tends to zero as distance approaches infinity.
  • Some participants challenge the idea of using infinity as a reference point, suggesting that it is more about the finite value at which functions converge rather than a physical location.
  • Questions arise regarding the use of arbitrary constants in potential calculations, with some participants noting that these constants do not affect physical outcomes, as only potential differences are significant.
  • One participant emphasizes that the electrostatic potential is determined up to an arbitrary constant, which can be chosen for convenience, such as setting the potential to zero at infinity.
  • Another point raised is that while theorists may use infinity in equations, experimentalists cannot measure at infinity, leading to a distinction between theoretical and practical considerations.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the legitimacy of using infinity as a reference point. Multiple competing views exist regarding its physical meaning and the implications of using arbitrary constants in potential calculations.

Contextual Notes

The discussion highlights limitations in understanding the physical significance of infinity and the arbitrary nature of potential constants. There is an ongoing exploration of the relationship between theoretical constructs and experimental measurements.

Nader AbdlGhani
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I'm facing a problem in my physics course which is accepting that infinity can be a reference point in both Electrostatics (calculating the voltage of a point) and Matter Properties (calculating the gravitational potential energy), how come we use a reference point which we don't know where it is, keep in mind that I don't have any problems dealing with infinity when we plug it in a mathematical relation, what I want is to understand the physical concept of choosing infinity as a reference.
 
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Nader AbdlGhani said:
I want is to understand the physical concept of choosing infinity as a reference.
There is no general physical concept. It's often just a convenient convention
 
Nader AbdlGhani said:
I'm facing a problem in my physics course which is accepting that infinity can be a reference point in both Electrostatics (calculating the voltage of a point) and Matter Properties (calculating the gravitational potential energy), how come we use a reference point which we don't know where it is, keep in mind that I don't have any problems dealing with infinity when we plug it in a mathematical relation, what I want is to understand the physical concept of choosing infinity as a reference.

"A point at infinity" is simply a point far enough away that going any further would make a negligible difference to the system. E.g. the point at infinity is far enough away that the potential energy is a maximum (for GPE or attractive charges) or a minimum (for repulsive charges).
 
A.T. said:
There is no general physical concept. It's often just a convenient convention
Ok then, I can't get over that "convenient convention", and please tell me, what makes it legit ?
 
PeroK said:
"A point at infinity" is simply a point far enough away that going any further would make a negligible difference to the system. E.g. the point at infinity is far enough away that the potential energy is a maximum (for GPE or attractive charges) or a minimum (for repulsive charges).
Thanks for your reply, but can you tell me how we are able to calculate for instance the voltage of a point charge having a charge Q, it's coordinates are (X,Y) while setting our reference point as infinity ?
 
Nader AbdlGhani said:
Thanks for your reply, but can you tell me how we are able to calculate for instance the voltage of a point charge having a charge Q, it's coordinates are (X,Y) while setting our reference point as infinity ?

Voltage is the difference in electric potential, so the question is how to define electric potential. One definition of electric potential for a point charge ##Q## is:

##U = \frac{Q}{4\pi \epsilon_0 r} \ ##, where ##r## is the distance from the charge.

This gives a function of ##r## that tends to ##0## as ##r \rightarrow \infty##. And, in many ways, this is the most natural and useful definition, given the relationship between ##U## and ##r##. I'm not sure I would say this uses ##\infty## as a reference point, though.

You could equally well define:

##U = U_0 + \frac{Q}{4\pi \epsilon_0 r} \ ##, where ##U_0## is some constant.

If ##Q## is negative (or if ##Q## is positive and ##U_0## is negative), you will have some radius ##r_0## where ##U(r_0) = 0##. But, it's not really making ##r_0## special.
 
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PS How you define ##U(r)## doesn't change the critical fact that the function ##U(r)## never attains its max or min, but tends to one of these as ##r \rightarrow 0## and the other as ##r \rightarrow \infty##. In a sense, ##r \rightarrow \infty## has a physical meaning whether you like it or not!
 
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Nader AbdlGhani said:
how come we use a reference point which we don't know where it is
This might be the core of your confusion: We aren't using the position as reference, just the finite value at which some function converges.
 
PeroK said:
Voltage is the difference in electric potential, so the question is how to define electric potential. One definition of electric potential for a point charge ##Q## is:

##U = \frac{Q}{4\pi \epsilon_0 r} \ ##, where ##r## is the distance from the charge.

This gives a function of ##r## that tends to ##0## as ##r \rightarrow \infty##. And, in many ways, this is the most natural and useful definition, given the relationship between ##U## and ##r##. I'm not sure I would say this uses ##\infty## as a reference point, though.

You could equally well define:

##U = U_0 + \frac{Q}{4\pi \epsilon_0 r} \ ##, where ##U_0## is some constant.

If ##Q## is negative (or if ##Q## is positive and ##U_0## is negative), you will have some radius ##r_0## where ##U(r_0) = 0##. But, it's not really making ##r_0## special.
Hello. Why are we giving it an arbitrary constant in the first place?
 
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PeroK said:
Voltage is the difference in electric potential, so the question is how to define electric potential. One definition of electric potential for a point charge ##Q## is:

##U = \frac{Q}{4\pi \epsilon_0 r} \ ##, where ##r## is the distance from the charge.

This gives a function of ##r## that tends to ##0## as ##r \rightarrow \infty##. And, in many ways, this is the most natural and useful definition, given the relationship between ##U## and ##r##. I'm not sure I would say this uses ##\infty## as a reference point, though.

You could equally well define:

##U = U_0 + \frac{Q}{4\pi \epsilon_0 r} \ ##, where ##U_0## is some constant.

If ##Q## is negative (or if ##Q## is positive and ##U_0## is negative), you will have some radius ##r_0## where ##U(r_0) = 0##. But, it's not really making ##r_0## special.
Hello. Why do we use the arbitrary constant may I ask? What function does it serve? Is it the initial electric potential at that reference point?
 
  • #11
ayans2495 said:
Hello. Why do we use the arbitrary constant may I ask? What function does it serve? Is it the initial electric potential at that reference point?
Mathematically, the potential when differentiated gives the electric field. And an anti-derivative has an arbitrary constant.

Physically, only the difference in potential is important, so you can add a constant without changing the physics. And, yes, this is equivalent to choosing a certain reference point as having zero potential.
 
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  • #12
ayans2495 said:
Hello. Why do we use the arbitrary constant may I ask? What function does it serve? Is it the initial electric potential at that reference point?
None. That's an important point. The electrostatic potential is only determined up to an arbitrary additive constant without any physical significance. Only potential differences are related to physical observables. That's why you can choose the additive constant arbitrarily, and it is usually convenient to choose it such that the potential goes to zero at infinity.
 
  • #13
Nader AbdlGhani said:
I'm facing a problem in my physics course which is accepting that infinity can be a reference point in both Electrostatics (calculating the voltage of a point) and Matter Properties (calculating the gravitational potential energy), how come we use a reference point which we don't know where it is, keep in mind that I don't have any problems dealing with infinity when we plug it in a mathematical relation, what I want is to understand the physical concept of choosing infinity as a reference.
It's a reference for theorists, not for experimentalists. We cannot measure at infinity, but we can put ##r\to \infty## in equations.
 
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  • #14
We cannot measure the absolute electric potential anyway, as stressed above, but only potential differences ("voltages") between two points separated by a finite distance in the lab. So theory and experiment are in no contradiction here but perfectly match (as it should be)!
 
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