Derivative of Lx^2+Ly^2+Lz^2 =?

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The discussion focuses on correcting the expressions for angular momentum components in a quantum mechanics context, specifically addressing errors in the terms for Lx and Lz. It is clarified that Lx should include cos(φ) instead of cot(φ), and Lz has a sign error. Participants seek to understand how to express Lx² + Ly² + Lz² in spherical coordinates. The conversation emphasizes the need for precise calculations and clarifications regarding the problem at hand. The thread highlights the importance of accuracy in mathematical expressions related to angular momentum.
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Thanks for your helpings...
 

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In ##L_x##, it should be ##\cos \phi##, not ##\cot \phi##. ##L_z## has the wrong sign.
 
DrClaude said:
In ##L_x##, it should be ##\cos \phi##, not ##\cot \phi##. ##L_z## has the wrong sign.

So how can i go on. In no way i coulnd't tackled it. Thanks for your help...
 
rasi said:
So how can i go on. In no way i coulnd't tackled it. Thanks for your help...
Not sure what you mean here.

Can you describe the problem you want to solve? The title of the thread is not very clear, do you mean you need to write ##L_x^2 + L_y^2 + L_z^2## in spherical coordinates ##(\theta, \phi)##?
 
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DrClaude said:
Not sure what you mean here.

Can you describe the problem you want to solve? The title of the thread is not very clear, do you mean you need to write ##L_x^2 + L_y^2 + L_z^2## in spherical coordinates ##(\theta, \phi)##?

yes. just as you said.
 
Then you need to calculate each term by applying it to itself, e.g.,
$$
L_z^2 = L_z L_z = -i \hbar \frac{\partial}{\partial \phi} \left( -i \hbar \frac{\partial}{\partial \phi} \right)
$$
 

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