2566: Decorative Constants
- This was the first comic that came out after the Countdown in header text started.
Explanation[edit]
This explanation may be incomplete or incorrect: Created by a DECORATIVE BOT - What is the formula 4-15 representing when removing the two decorative constants? - Do NOT delete this tag too soon. If you can address this issue, please edit the page! Thanks. |
This is another one of Randall's Tips, this time a Math Tip.
Randall gives an example of a complex looking equation labeled 4-15:
- T = 𝔻m_{0}(r_{out} − r_{in})^{μ̅}
But since 𝔻 and μ̅ are "decorative", the equation can be reduced to
- T = m_{0}(r_{out} − r_{in})
Here T is the net rate, m_{0} the unit mass and (r_{out} − r_{in}) the flow balance.
The decorative symbols can be interpreted as constants 𝔻 = μ̅ = 1, in which case the implied operations of multiplication and exponentiation make sense. The 𝔻 is double-struck ("blackboard bold", thus in the comic only the vertical line is double). Mathematicians, who are always searching for more symbols^{[citation needed]}, have taken to distinguishing things represented by the same letter by using different fonts, such as 𝑑, 𝐝, 𝒅, 𝐷, 𝐃, 𝑫, 𝒹, 𝒟, 𝖉, 𝕯, ∂, 𝕕, and 𝔻. The double-struck font is easier to write on a blackboard than a proper bold letter and often represents a set, such as ℝ for the set of real numbers or ℂ for the set of complex numbers. 𝔻 can represent the unit disk in the complex plane, the set of decimal fractions, or the set of split-complex numbers.
μ is the Greek lowercase mu and has many uses in mathematics and science. Here it has a bar, μ̅, which could indicate a number of things, including the complex conjugate. Intriguingly, μ is the symbol in statistics for the population mean, and the overbar represents the sample mean, so this could represent a random variable which is the average of a sample of means μ_{i} of different populations in some larger ensemble of populations.
Using a special version both of D and μ to even further spice up the formula all leads up to the math tip:
- If one of your equations ever looks too simple, try adding some purely decorative constants.
Other examples of well known equations that are profound but look simple include
- E = mc^{2} (Special Relativity),
- PV = nRT (the Ideal Gas Law),
- F = ma (Newton's Second Law),
- V = IR (Ohm's Law), and
- G_{μν} + Λ g_{μν} = κT_{μν} (Einstein field equations).
Of these, only the Einstein field equations have been spiced up with decorative indices (which actually hide a system of ten nonlinear partial differential equations).
In the title text Randall mentions the Drag equation, which is attributed to Lord Rayleigh. In fluid dynamics, the drag equation is a formula used to calculate the force of drag experienced by an object due to movement through a fully enclosing fluid. The equation is F_{d} = ½ρu^{2}c_{d}A. Here F_{d} is the drag force, ρ the mass density of the fluid, u the relative flow velocity, c_{d} the drag coefficient and A is the area.
Randall jokes that the factor of ½ in the equation is meaningless and purely decorative, since the drag coefficients, c_{d}, are already unitless and could just as easily be half as big thus leaving out the ½ in front of the equation. The ½ is thus just an example of a "decorative constant." The usual reason for including the factor of ½ is that it is part of the formula for kinetic energy that appears in the derivation of the drag equation, i.e. ½ρu^{2}. However, modern treatments are so condensed that this factor of ½ is often smuggled in with no explanation.
Since we can choose the constants to be whatever we want, it could be possible to absorb the ½ into the drag coefficient c_{d}, but that does not mean it is unmotivated, since it comes from the kinetic energy. Still, Randall quotes Frank White's Fluid Mechanics textbook, which two times calls it "a traditional tribute to Euler and Bernoulli." According to White, the factor of ½ rather comes from the calculation of the projected area of the object being dragged. Randall has brought up this point before, in his book, "How To"
The line from White probably refers to renowned mathematicians Leonhard Euler and Daniel Bernoulli. Euler who is held to be one of the greatest mathematicians in history worked directly with Daniel and was a friend of the Bernoulli family, that produced eight mathematically gifted academics.
Daniel Bernoulli is known for modifying the definition of vis viva (what we now call kinetic energy) from mv^{2} to ½mv^{2}, as motivated by the derivation from the impulse equation. In 1741, he wrote
- [Define vis viva] esse ½ mvv = ∫pdx.
That is, "define vis viva to be ½ mv^{2} = ∫pdx," where p is the force (from pressione) and dx is the differential of position (infinitesimal displacement). Today, this equation says that the kinetic energy imparted to an object at rest equals the work done on it.
In the drag equation ½ ρu^{2} represents the dynamic pressure due to the kinetic energy of the fluid, and hence the 1/2 makes sense to keep in the equation, and could thus easily be argued not to represent a decorative constant.
The title text is pretty much word-for-word a repeat from Randall's book How To. In Chapter 11: How to Play Football, he misuses the drag equation, and mentions this fact in more depth, in a footnote.
Transcript[edit]
- [A small panel only with text. Written as an excerpt from a mathematical text book. Begins with a number for an equation, then follows the equation written in larger letters and symbols. And below are explanations of each term in the equation. The μ has a bar over the top and the D has a double vertical line.]
- Eq. 4-15
- T = 𝔻m_{0}(r_{out} - r_{in})^{μ̅}
- T: Net rate
- m_{0}: Unit mass
- (r_{out}-r_{in}): Flow balance
- 𝔻, μ̅: Decorative
- [Caption below the panel:]
- Math tip: If one of your equations ever looks too simple, try adding some purely decorative constants.
Discussion
I don't have any idea what to put in the actual description, but whoever does should probably note that r(in) - r(out) equals zero, not one. And multiplying by a constant 0 absolutely changes the value! GreatWyrmGold (talk) 21:59, 10 January 2022 (UTC)
- r_{out} and r_{in} are different values. The subscripts represent different instances of the same variable at different point. In the same way, you might calculate something happening over a time interval t_{end} - t_{start} . 172.69.71.77 23:02, 10 January 2022 (UTC)
- Yes for sure they are two different values. On the other hand if μ is not 1 then the it is not just decorative! D on the other hand is just a proportionality constant, which may have a value other than 1. I have tried to put something in the explanation here. Quite a bit. Do not really now anything about Drag, so just took it from the wiki page. Also I hope someone can explain the formula in the image, as I'm sure it is just something about the flow, that would relate it to a drag equation. --Kynde (talk) 23:41, 10 January 2022 (UTC)
Note that the title text is pretty much word-for-word a repeat from Randall's book *How To*. In Chapter 11: *How to Play Football*, he misuses the drag equation, and mentions this fact in more depth, in a footnote. Bit of trivia! --162.158.134.79 23:13, 10 January 2022 (UTC)
- Nice, I will have to check up on that. Thanks. --Kynde (talk) 23:41, 10 January 2022 (UTC)
- Can confirm this, the book mentions that the "traditional tribute to Euler and Bernoulli" comes from Frank White's Fluid Mechanics textbook. Clam (talk) 01:08, 11 January 2022 (UTC)
- There it is, page 266 in the 1986 2nd edition: "They both have a factor ½ as a traditional tribute to Bernoulli and Euler, and both are based on the projected area..." https://books.google.com/books?id=wGweAQAAIAAJ&q=traditional -- 172.70.162.5 02:13, 11 January 2022 (UTC)
- Wait, wouldn't the values be twice as big (rather than half as big) if you left off the 1/2? 141.101.69.154 12:43, 11 January 2022 (UTC)
Of course, the c^2 im e=mc^2 is just as decorative, when using natural units where c=1.... 172.68.50.171 00:29, 11 January 2022 (UTC)
- And the resulting equation is then just e=m - or m=e which is beautiful and profound. "Mass is Energy". Without the complications, you stop thinking of it as a PROCESS for converting one into the other and get the more profound point that Mass and Energy are the exact same thing. SteveBaker (talk) 03:33, 11 January 2022 (UTC)
- I respectfully disagree. The c² isn't decorative; mc² is a measure of energy and m is not. e=mc², like f=ma, still works even if you change the size of any of the basic units (of length, time, mass) from which the units of energy and force are derived. As I see it, an equation that ties you to any definition of unit size is less profound, not more. Tom239 (talk) 17:21, 12 January 2022 (UTC)
I think the 1/2 in the drag equation is intuitive. I understand that it is technically superfluous, but F=Pd*A and Pd=1/2*rho*u^2 so the 1/2 carries over intuitively. 172.70.98.15 (talk) (please sign your comments with ~~~~)
- Agrees I had this written down in an early version of the explanation but that was edited out. Maybe I will put it in again.--Kynde (talk) 10:44, 12 January 2022 (UTC)
Drag coefficients could just as easily be half as big. This is true but how is their being unitless relevant? It's more about how defining constants is partially arbitrary. Lev (talk) 08:07, 12 January 2022 (UTC)
- If Cd had a unit, say it was an energy which represented some relevant value for a given material, then it would not be correct to say that it was half as much, just because 1/2 came into the equation. But if it has no units, then it is just a constant saying something about the material, and then the 1/2 could in principle be absorbed without changing anything. But as stated above 1/2 actually has physical meaning in the way it enters the equation. --Kynde (talk) 10:44, 12 January 2022 (UTC)
- It doesn't make any difference. For instance, Coulomb's law works fine whether we write it F = -q_{1}q_{2}/(4πε_{0}r^{2}) or F = -kq_{1}q_{2}/r^{2}. Similarly, if we had a factor of 2 in the gas law for some reason, that would just change the values of the gas constants.
Count down clock[edit]
See Countdown in header text. Discussion has been moved here Talk:Countdown_in_header_text. --Kynde (talk) 11:10, 12 January 2022 (UTC)