Recent content by Gbox

  1. Gbox

    Ladder Operators: Commutation Relation & Beyond

    a. ##L_{+}^{\dagger}=(L_x+iL_y)^{\dagger}=L_x-iL_y=L_{-}## b.##[L_{+},L_{-}]=[L_x+iL_y,L_x-iL_y]=(L_x+iL_y)(L_x-iL_y)-(L_x-iL_y)(L_x+iL_y)=## ##=L_x^2-iL_xL_y+iL_yL_x+L_y^2-(L_x^2+iL_xL_y-iL_yL_x-L_y^2)## ##=L_x^2-iL_xL_y+iL_yL_x+L_y^2-L_x^2-iL_xL_y+iL_yL_x+L_y^2##...
  2. Gbox

    Finding inveriance size, equilibrium and fluctuations

    So I answered 1 and 2, got: 1. ##\vec(r)(\theta,\phi)=l(sin \theta cos \phi, sin \theta sin \phi, -cos \theta)## 2. ##L=\frac{ml^2 (\dot{\theta}^2+\dot{\phi}^2 sin^2 \theta)}{2}+mglcos \theta## 3. a ##mlsin \theta -mgsin \theta =l^2 \ddot{\theta}## , b. ##ml^2 \ddot{\phi}=0## 4. I know...
  3. Gbox

    Prove: angular momentum is preserved

    Do you mean ##-\frac{\partial H}{\partial \phi}=m(x\dot{y}-y\dot{x})## Where ##x=rsin\theta cos\phi, y=rsin\theta sin\phi##?
  4. Gbox

    Prove: angular momentum is preserved

    3. Find the hamilton equations 4. using 3. prove the the angular momentum in the z axis ##L_z=m(x\dot y-xy\dot)## is preserved. I got in ##3##: How can I prove 4?
  5. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    Not it is just that my background is in math (done linear algebra 1+2) so I am checking each step form math (and now physics) point of view
  6. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    I mean here: Why you have ## a, b, -a, b## and not ##a,b,c,d##?
  7. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    I am maybe confused with the dirac notations, but how did you get to this expression?
  8. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    Thanks! So mathematically, are we doing a basis change? as how else can we arrive to ##\left| v_1 \right>= \frac{1}{\sqrt{2}} \left| x \right>+\frac{1}{\sqrt{2}}\left| y \right>## And ## \left| v_2 \right>= -\frac{1}{\sqrt{2}}\left| x \right>+\frac{1}{\sqrt{2}} \left| y \right>## Using the...
  9. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    Thanks, I do not understand the physics the led to the two equations. maybe I will go a step back ##\left| x \right>## and ##\left| y \right>## are the state of the system after a measure is done? The eigenvectors of ##A## are the state of the system before the mesure? So now we are...
  10. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    Why ##\left| v_1 \right>= \frac{1}{\sqrt{2}} \left| x \right>+\frac{1}{\sqrt{2}}\left| y \right>## And ## \left| v_2 \right>= -\frac{1}{\sqrt{2}}\left| x \right>$+\frac{1}{\sqrt{2}} \left| y \right>## ? We took the dot product of the eigenvalues of ##A##? Did we use the fact that ##\left|...
  11. Gbox

    What are energy values and how do they relate to eigenvectors in quantum states?

    Summary: Finding state at t=0, energy values and more So this is my first question in quantum mechanics (please understand). 1. So we have a system, and to describe the state of the system we have to measure, A is an hermitian matrix, that each physical measurable quantity has. To find the...
  12. Gbox

    Engineering Diode circuit with AC excitation source

    Why is the left hand diode is conducting? the capacitors do not affect the voltage? do not they both charge to the same voltage and the diode is not conducting?
  13. Gbox

    Engineering Diode circuit with AC excitation source

    Homework Statement Graph ##V_{out}## Homework EquationsThe Attempt at a Solution When ##V_{in}=V## C1 is positive on the left and negative on the right, and C2 is negative on the the down side and positive on the upper side so there is no Vout?
  14. Gbox

    Graph displacement as function of time

    I have a lot of constant so rather than at ##t=0## the answer says something like slope of about ##\frac{1}{t^2}## and frequency of about ##t^3## how did the get to it?
  15. Gbox

    Graph displacement as function of time

    Homework Statement let there be ##\beta(t+\tau)^{-2}e^{-3}cos(at^{3})## where ##\beta##, ##\tau## and ##a## are constants Homework Equations ##\beta(t+\tau)^{-2}e^{-3}cos(at^{3})## The Attempt at a Solution I know the graph is going up and down exponential but how can I draw it more...
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