• Caveman@lemmy.world
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    3 days ago

    The thing is that it’s legit a fraction and d/dx actually explains what’s going on under the hood. People interact with it as an operator because it’s mostly looking up common derivatives and using the properties.

    Take for example f(x) dx to mean "the sum (∫) of supersmall sections of x (dx) multiplied by the value of x at that point ( f(x) ). This is why there’s dx at the end of all integrals.

    The same way you can say that the slope at x is tiny f(x) divided by tiny x or d*f(x) / dx or more traditionally (d/dx) * f(x).

  • someacnt@sh.itjust.works
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    2 days ago

    But df/dx is a fraction, is a ratio between differential of f and standard differential of x. They both live in the tangent space TR, which is isomorphic to R.

    What’s not fraction is \partial f / \partial x, but likely you already know that. This is akin to how you cannot divide two vectors.

  • socsa@piefed.social
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    2 days ago

    The world has finite precision. dx isn’t a limit towards zero, it is a limit towards the smallest numerical non-zero. For physics, that’s Planck, for engineers it’s the least significant bit/figure. All of calculus can be generalized to arbitrary precision, and it’s called discrete math. So not even mathematicians agree on this topic.

  • chortle_tortle@mander.xyz
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    4 days ago

    Mathematicians will in one breath tell you they aren’t fractions, then in the next tell you dz/dx = dz/dy * dy/dx

  • benignintervention@lemmy.world
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    4 days ago

    I found math in physics to have this really fun duality of “these are rigorous rules that must be followed” and “if we make a set of edge case assumptions, we can fit the square peg in the round hole”

    Also I will always treat the derivative operator as a fraction

  • rudyharrelson@lemmy.radio
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    4 days ago

    Derivatives started making more sense to me after I started learning their practical applications in physics class. d/dx was too abstract when learning it in precalc, but once physics introduced d/dt (change with respect to time t), it made derivative formulas feel more intuitive, like “velocity is the change in position with respect to time, which the derivative of position” and “acceleration is the change in velocity with respect to time, which is the derivative of velocity”

    • Prunebutt@slrpnk.net
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      4 days ago

      Possibly you just had to hear it more than once.

      I learned it the other way around since my physics teacher was speedrunning the math sections to get to the fun physics stuff and I really got it after hearing it the second time in math class.

      But yeah: it often helps to have practical examples and it doesn’t get any more applicable to real life than d/dt.

      • exasperation@lemmy.dbzer0.com
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        3 days ago

        I always needed practical examples, which is why it was helpful to learn physics alongside calculus my senior year in high school. Knowing where the physics equations came from was easier than just blindly memorizing the formulas.

        The specific example of things clicking for me was understanding where the “1/2” came from in distance = 1/2 (acceleration)(time)^2 (the simpler case of initial velocity being 0).

        And then later on, complex numbers didn’t make any sense to me until phase angles in AC circuits showed me a practical application, and vector calculus didn’t make sense to me until I had to actually work out practical applications of Maxwell’s equations.

  • vaionko@sopuli.xyz
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    4 days ago

    Except you can kinda treat it as a fraction when dealing with differential equations

  • shapis@lemmy.ml
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    4 days ago

    This very nice Romanian lady that taught me complex plane calculus made sure to emphasize that e^j*theta was just a notation.

    Then proceeded to just use it as if it was actually eulers number to the j arg. And I still don’t understand why and under what cases I can’t just assume it’s the actual thing.

    • jsomae@lemmy.ml
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      2 days ago

      e𝘪θ is not just notation. You can graph the entire function ex+𝘪θ across the whole complex domain and find that it matches up smoothly with both the version restricted to the real axis (ex) and the imaginary axis (e𝘪θ). The complete version is:

      ex+𝘪θ := ex(cos(θ) + 𝘪sin(θ))

      Various proofs of this can be found on wikipeda. Since these proofs just use basic calculus, this means we didn’t need to invent any new notation along the way.

      • shapis@lemmy.ml
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        2 days ago

        I’m aware of that identity. There’s a good chance I misunderstood what she said about it being just a notation.

        • jsomae@lemmy.ml
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          2 days ago

          It’s not simply notation, since you can prove the identity from base principles. An alien species would be able to discover this independently.

    • frezik@lemmy.blahaj.zone
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      4 days ago

      Let’s face it: Calculus notation is a mess. We have three different ways to notate a derivative, and they all suck.

    • carmo55@lemmy.zip
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      3 days ago

      It is just a definition, but it’s the only definition of the complex exponential function which is well behaved and is equal to the real variable function on the real line.

      Also, every identity about analytical functions on the real line also holds for the respective complex function (excluding things that require ordering). They should have probably explained it.

      • shapis@lemmy.ml
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        3 days ago

        She did. She spent a whole class on about the fundamental theorem of algebra I believe? I was distracted though.

    • marcos@lemmy.world
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      4 days ago

      And it denotes an operation that gives you that fraction in operational algebra…

      Instead of making it clear that d is an operator, not a value, and thus the entire thing becomes an operator, physicists keep claiming that there’s no fraction involved. I guess they like confusing people.