Why Multiply By Extra r In Polar Coordinates?

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Why do you multiply by an extra “r” when converting a double integral in polar coordinates?

Let me answer a commonly asked question, “Why do you need to always multiply by an extra “r” term when converting to polar coordinates?”

The answer is simple, it’s because it’s a transformation of multiple variables (2 variables to 2 new variables).

Remember when you did substitution involving 1 variable to 1 new variable? For example, if you let \(u = {x^2}\), then \(du = 2xdt\).

But if you’re using polar coordinates, which is, \(x = rcos (\theta )\) and \(y = rsin (\theta )\), then you need to find the Jacobian, which is the determinant of all the partial derivatives.

You can’t just differentiate it as before to change the variable.

\[J = \left| {\begin{array}{*{20}{c}}{\frac{{\partial x}}{{\partial r}}}&{\frac{{\partial x}}{{\partial \theta }}}\\{\frac{{\partial y}}{{\partial r}}}&{\frac{{\partial y}}{{\partial \theta }}}\end{array}} \right|\]

\[J = \left| {\begin{array}{*{20}{c}}{\cos (\theta )}&{ – r\sin (\theta )}\\{\sin (\theta )}&{r\cos (\theta )}\end{array}} \right|\]

\[J = \cos (\theta ) \cdot r\cos (\theta ) – ( – r\sin (\theta )) \cdot \sin (\theta ))\]

\[J = r{\cos ^2}(\theta ) + r{\sin ^2}(\theta )\]

And recall the identity:

\[{\cos ^2}(\theta ) + {\sin ^2}(\theta ) = 1\]

Simplifying our Jacobian:

\[J = r\]

What exactly does the Jacobian mean in the transformation?

It’s just the factor you need to multiply by when you do a transformation change of coordinates.

In other words,

\[dxdy = rdrd\theta \]

And that’s why you multiply by an extra “r” term when you do a polar coordinates transformation!

Try the next example problem where you solve a double integral using polar coordinates!

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