Recent content by Bullwinckle

  1. B

    Euler, Tait, Gyroscope: Rotations that cover it all

    This is great! This I understand. I follow your "proof" that... $$\hat{R}=\hat{R}_3(\alpha) \hat{R}_1(\beta) \hat{R}_3(\gamma).$$ is a parameterization of the rotation group SO(3) And I can easily intuit similar proof for the Tait angles (and ditto for the gyroscope) So is that the issue...
  2. B

    Euler, Tait, Gyroscope: Rotations that cover it all

    Thank you Vanhees, But may I elaborate in the context of your response? How do I KNOW that the Tait or Euler or Gyro are parameterizations of the rotation group? Surely I can rotate about the local 3-axis three times. And I know, obviously, that it will not cover all the rotations. The Tait...
  3. B

    Euler, Tait, Gyroscope: Rotations that cover it all

    I understand that a gyroscope undergoes precession, nutation, spin. And that the order of the rotations are such that the precession and spin share a common "local axis." I also understand there are, for totally different purposes, Euler angles to model rotations. In this case, the order of the...
  4. B

    Why the Inconsistent Use of Δ in Physics?

    Oh, one more thing... Are you saying that books use this: ΔL = mv1 - mv2 Simply to prepare students to solve problems over a finite time difference that is not infinitesimally small? So, here, the Δ is being used for a PRACTICAL purpose?
  5. B

    Why the Inconsistent Use of Δ in Physics?

    Hello, Sometimes in introductory physics, I see this: After defining P as the momentum, we show: dP/dt = F Then, later, I see this ΔL = mv1 - mv2 So my question is really simple: WHY is there no consistency? Why do we sometimes use the Δ symbol? Is there something about how the...
  6. B

    Product rule for vector derivative

    Say I have a position vector p = e(t) p(t) Where, in 2D, e(t) = (e1(t), e2(t)) and p(t) = (p1(t), p2(t))T And if I conveniently point the FIRST base vector of the frame at the particle, I can use: p(t) = (r1(t), 0)T I want the velocity, so I take v = d(e(t))/dt p(t) + e(t) d(p(t))/dt...
  7. B

    Work/Energy and Impulse/Momentum

    OK, so are you not also stumbling over this: dr = v dt (to progress from the second to third term) Is that not taking this: dr/dt = v And multiplying by dt? Now I feel I am back at square-1 Or, are your words "parametrization" the key. Is this allowed in a parametrization? Is there...
  8. B

    Work/Energy and Impulse/Momentum

    If we take F=ma and multiply both sides by dt, we get Fdt = ma dt And then: Fdt = mdv And then: Impulse = change in momentum. OK; I get that. I get a similar process for Work/Energy multiplying F=ma by ds on both sides as follows Fds = ma ds And using a ds = v dv to get Fds = m v...
Back
Top