amavect
Joined 1 year ago
Joined 1 year ago
Maybe you read sheet music different than how I do, but when I play euphonium or trombone, I translate from note position+features to finger+mouth position without needing to think about the note letter. More like, "I see the note located here with an accidental feature in the context of the clef and key signature therefore I use this finger position and mouth position". I would love to simplify it down to "it's located here therefore I use this finger position and mouth position".
Keep the accidentals to notate alternate finger positions for enharmonics (and microtones), but eliminate the global variables, the clefs and key signature. Heck, keep the key signature to reduce the noise of alternate fingering symbols, but PLEASE eliminate the clefs. I would also love to play treble clefs at the same sight-reading speed as bass clefs. Also, staff notation should visually repeat every octave, but it doesn't.
Conservation of E-field flux certainly implies additive-homomorphism (addition of charges equals addition of forces). But that seems a bit ahistorical because Maxwell would develop field theory 70 years after Coloumb. Either way, the axiom you choose requires empirical justification, and I think a home hobbyist could more easily demonstrate by experiment that adding charges will add the forces.
Or, if you meant F(r,1,1) = K/r^2, then yeah, conservation of E-field flux could give you an inverse square law. But again, that requires an experiment to justify the axiom.
F(r,q0,q1)
= F(r,q0*1,q1*1)
= q0*q1*F(r,1,1)
Very simple! It remains to show that F(r,1,1) = K/r^2, as intended.I figured this out by listing a bunch of mathematical properties. I couldn't see how the author jumps from zero-preserving to multiply-charges, and I still don't know how, but we can call it out of scope lol
r : distance between p and q
q0 : charge 0
q1 : charge 1
F : coulomb force function
charge-commutative: F(r,q0,q1) = F(r,q1,q0)
zero-preserving: 0 = F(r,q0,0)
additive-homomorphic: F(r,q0,q1+q2) = F(r,q0,q1)+F(r,q0,q2)
homogenous-degree-1: F(r,q0,n*q1) = n*F(r,q0,q1)
multiplicative-separability: F(r,q0,q1) = K*R(r)*Q(q0,q1)
multiply-charges: F(r,q0,q1) = K*R(r)*(q0*q1)^a
Given F(r,q0,q1) = K*R(r)*(q0*q1)^a, charge-commutative, zero-preserving, additive-homomorphic.
Induction using additive-homomorphic proves homogenous-degree-1. (For example, F(r,q0,2*q1) = F(r,q0,q1+q1) = 2*F(r,q0,q1))
Equational proof follows from homogenous-degree-1:
K*R(r)*(q0*n*q1)^a = n*K*R(r)*(q0*q1)^a
(q0*n*q1)^a = n*(q0*q1)^a
n^a*(q0*q1)^a = n*(q0*q1)^a
n^a = n
n = 0 or a = 1
n≠0, therefore a=1.So, you're right. This shows why we should use formal math, so we can agree on the result yet bicker about the interpretation. Some folks point to Cantor's diagonalization theorem to show that some unnameable things exist, when the theorem doesn't say that at all.
On the other hand, given any real number, I can name it. I'll run out of unique names, since no injective function exists from real numbers to names.
So, some unnamed real numbers will always remain (non-constructively), I can make real numbers that escape a naming scheme (constructively), and no unnameable real numbers exist.
Really, the blurb about "seems impossible to verify this by giving positive instances" contains the tension between constructive math and non-constructive math. Does an unnameable (and undefinable) thing actually exist? If a tree falls in a forest, but no one can hear it, does it make a sound?
I love approval voting the most by pure simplicity and effectiveness. How does score voting work better than STAR? I thought STAR degenerates into score voting when clone candidates run?
I haven't heard much of an argument against proportional voting before. Your article just casts doubt, but doesn't really make a decisive argument against. I actually don't like proportional voting because it reifies parties into the system, but I only support it because I think it can break the party duopoly and step towards better systems. I should rethink that.