MHB How is the Gradient of u(r,θ) Calculated?

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The discussion focuses on calculating the gradient of the function u(r, θ) defined as u(r, θ) = r cos(θ)[1 - (1/r)^2]. The gradient is derived using the formula for the gradient in spherical coordinates, which involves computing partial derivatives with respect to r and θ. The participants suggest converting the function into Cartesian coordinates, specifically u = x(1 - 1/(x^2 + y^2)), to simplify the gradient calculation. The final gradient expression is confirmed as 1 + (2x^2)/(x^2 + y^2)^2 - 1/(x^2 + y^2), (2xy)/(x^2 + y^2)^2. This approach allows for a clearer understanding of the gradient in a more familiar coordinate system.
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I have
$$
u(r,\theta) = r\cos(\theta)\left[1 - \left(\frac{1}{r}\right)^2\right]
$$
and the gradient is
$$
1 + \frac{2 x^2}{(x^2 + y^2)^2} - \frac{1}{x^2 + y^2}, \frac{2 x y}{(x^2 + y^2)^2}
$$
How was this obtained?
 
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dwsmith said:
I have
$$
u(r,\theta) = r\cos(\theta)\left[1 - \left(\frac{1}{r}\right)^2\right]
$$
and the gradient is
$$
1 + \frac{2 x^2}{(x^2 + y^2)^2} - \frac{1}{x^2 + y^2}, \frac{2 x y}{(x^2 + y^2)^2}
$$
How was this obtained?

Hi dwsmith, :)

The gradient of a scalar field \(f\) in spherical coordinates is given by,

\[\nabla f(r, \theta, \phi) = \frac{\partial f}{\partial r}\mathbf{e}_r+\frac{1}{r}\frac{\partial f}{\partial \theta}\mathbf{e}_\theta+\frac{1}{r \sin\theta}\frac{\partial f}{\partial \phi}\mathbf{e}_\phi=\left(\frac{\partial f}{\partial r},\,\frac{1}{r}\frac{\partial f}{\partial \theta},\,\frac{1}{r \sin\theta}\frac{\partial f}{\partial \phi}\right)\]

Therefore,

\[\nabla u(r, \theta)=\left(\frac{\partial u}{\partial r},\,\frac{1}{r}\frac{\partial u}{\partial \theta},\,0\right)\]

Calculate the partial derivatives and convert them into Cartesian coordinates. Hope you can continue.

Kind Regards,
Sudharaka.
 
Probably the easiest way is to switch u in terms of x and y, $\it{ i.e.}$

$u = x \left( 1 - \dfrac{1}{x^2+y^2}\right)$,

then calculate the gradient the usual way.
 

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