How Do You Compute Derivatives in Spherical Coordinates Using the Chain Rule?

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SUMMARY

This discussion focuses on computing partial derivatives in spherical coordinates using the chain rule. The transformations for spherical coordinates are defined as x = ρ cos(θ) sin(φ), y = ρ sin(θ) sin(φ), and z = ρ cos(φ). The partial derivatives df/dρ, df/dθ, and df/dφ are expressed in terms of df/dx, df/dy, and df/dz using the chain rule. The general form of the chain rule is also reiterated, emphasizing its application in multivariable calculus.

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  • Understanding of multivariable calculus
  • Familiarity with spherical coordinates
  • Knowledge of the chain rule in calculus
  • Ability to compute partial derivatives
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  • Study the application of the chain rule in multivariable functions
  • Learn about transformations between Cartesian and spherical coordinates
  • Explore examples of computing derivatives in different coordinate systems
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Tony11235
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Let f: [tex]\Re^3 \rightarrow \Re[/tex] be differentiable. Making the substitution

[tex]x = \rho \cos{\theta} \sin{\phi}, y = \rho \sin{\theta} \sin{\phi}, z = \rho \cos{\phi}[/tex]

(spherical coordinates) into f(x,y,z), compute (partially) df/d(rho), df/d(theta), and df/d(phi) in terms of df/dx, df/dy, and df/dz.

I'm just not sure I understand the question. Does it involve pulling out a very long chain rule?
 
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Tony11235 said:
Let f: [tex]\Re^3 \rightarrow \Re[/tex] be differentiable. Making the substitution

[tex]x = \rho \cos{\theta} \sin{\phi}, y = \rho \sin{\theta} \sin{\phi}, z = \rho \cos{\phi}[/tex]

(spherical coordinates) into f(x,y,z), compute (partially) df/d(rho), df/d(theta), and df/d(phi) in terms of df/dx, df/dy, and df/dz.

I'm just not sure I understand the question. Does it involve pulling out a very long chain rule?
It involves the chain rule, not sure what you mean about the very long part.
[tex]\frac{\partial f}{\partial\rho}=\frac{\partial f}{\partial x} \ \frac{\partial x}{\partial\rho}+\frac{\partial f}{\partial y} \ \frac{\partial y}{\partial\rho}+\frac{\partial f}{\partial z} \ \frac{\partial z}{\partial\rho}[/tex]
[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]
[tex]\frac{\partial f}{\partial\phi}=\frac{\partial f}{\partial x} \ \frac{\partial x}{\partial\phi}+\frac{\partial f}{\partial y} \ \frac{\partial y}{\partial\phi}+\frac{\partial f}{\partial z} \ \frac{\partial z}{\partial\phi}[/tex]
The general form of the chain rule being
[tex]\frac{\partial f}{\partial x}=\sum_{k=1}^n \frac{\partial f}{\partial u_k} \ \frac{\partial u_k}{\partial x}[/tex]
where
[tex]f=f(u_1(x),u_2(x),...,u_{n-1}(x),u_n(x))[/tex]
 

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