Struggling with Angular Momentum in Spherical Coordinates?

In summary, the conversation discusses the conversion of momentum operators from Cartesian to spherical coordinates using given relations. The process involves a tedious calculation and the use of the derivative operators in spherical coordinates, which can be derived from those in Cartesian coordinates. It is also suggested to approach the problem by expressing spherical coordinates as a function of Cartesian coordinates. This conversation is discussing a problem from a pdf with 3 pages.
  • #1
Domnu
178
0
In http://web.utk.edu/~tbarnes/website/qm1/qm1hw_2006/hw1_2006/hw1_2006.pdf , on page 82, where it converts the momentum operators from Cartesian to spherical coordinates, I am a bit confused on how they get from 5.74-5.76 to 5.80-5.82 using the given relations. Could someone help me? Thanks a bunch :smile:
 
Last edited by a moderator:
Physics news on Phys.org
  • #2
That pdf has 3 pages.
 
  • #3
Ah, yes the link I meant was this: http://farside.ph.utexas.edu/teaching/qm/389.pdf
 
Last edited by a moderator:
  • #4
That's a long and tedious calculation that starts by noting that if f depends on x,y,z and eacho of those depend on the spherical coordinates, we can write down the derivatives with respect to the spherical coordinates...

[tex]\frac{\partial f}{\partial \theta}=\frac{\partial f}{\partial x}\frac{\partial x}{\partial \theta} +\frac{\partial f}{\partial y}\frac{\partial y}{\partial \theta} +\frac{\partial f}{\partial z}\frac{\partial z}{\partial \theta}[/tex]

...and so on. This shows that the derivative operators in spherical coordinates are linear combinations of the derivative operators in cartesian coordinates, so you get a system of equations which is possible to solve by the method of of adding a (well-chosen) multiple of one equation to another (lots of times).
 
  • #5
Hmm... could an easier way be

[tex]\frac{\partial f}{\partial z}=\frac{\partial f}{\partial \theta}\frac{\partial \theta}{\partial z} +\frac{\partial f}{\partial \phi}\frac{\partial \phi}{\partial z} +\frac{\partial f}{\partial r}\frac{\partial r}{\partial z}[/tex] ?

You can compute [tex]\partial \theta / \partial z,[/tex] for example, by differentiating implicitly with [tex]z = r \cos \theta[/tex]... would this work?
 
  • #6
Unfortunately no. There is a formula for the derivative of the inverse of the map [itex](r,\phi,\theta)\mapsto (x,y,z)[/itex], but figuring out what to put into it involves a procedure that's equivalent to the one I described. However, I forgot that it's actually quite easy to express [itex](r,\phi,\theta)[/itex] as a function of (x,y,z) instead of the other way round. Maybe it's easier to start out that way. http://en.wikipedia.org/wiki/Spherical_coordinates
 
  • #7
Domnu said:
Hmm... could an easier way be

[tex]\frac{\partial f}{\partial z}=\frac{\partial f}{\partial \theta}\frac{\partial \theta}{\partial z} +\frac{\partial f}{\partial \phi}\frac{\partial \phi}{\partial z} +\frac{\partial f}{\partial r}\frac{\partial r}{\partial z}[/tex] ?

You can compute [tex]\partial \theta / \partial z,[/tex] for example, by differentiating implicitly with [tex]z = r \cos \theta[/tex]... would this work?
Yes, this will work. Look at the last term, with df/dr.
The term dr/dz = z/ sqrt(x*x+Y*y+z*z), or [tex] \cos \theta[/tex].

The theta term requires [tex]\frac{\partial \theta}{\partial z}[/tex]
with z= r [tex] \cos \theta[/tex], from which you can compute the desired formula in spherical coords(hold r constant), and so on This is pretty much the standard way to do the problem -- grind it out.
Regards,
Reilly Atkinson
 
Last edited:

FAQ: Struggling with Angular Momentum in Spherical Coordinates?

What is angular momentum?

Angular momentum is a physical quantity that describes the rotation of an object around a fixed point. It is a vector quantity, meaning it has both magnitude and direction.

How is angular momentum calculated?

Angular momentum is calculated by multiplying the moment of inertia of an object by its angular velocity. The moment of inertia is a measure of an object's resistance to changes in its rotation, while angular velocity is the rate at which an object rotates around a fixed point.

What is the conservation of angular momentum?

The conservation of angular momentum is a fundamental law of physics that states that the total angular momentum of a system remains constant unless an external torque is applied. This means that the angular momentum of a system can neither be created nor destroyed, but can only be transferred from one object to another.

What are some real-world applications of angular momentum?

Angular momentum has many practical applications in various fields, including astronomy, mechanics, and engineering. For example, it is crucial in understanding the movement of planets and stars in space, the motion of spinning objects such as tops and gyroscopes, and the stability of rotating machinery.

How does angular momentum relate to angular velocity?

Angular velocity and angular momentum are closely related, as angular momentum is directly proportional to the product of an object's moment of inertia and its angular velocity. This means that a change in one of these quantities will result in a corresponding change in the other.

Back
Top