Sunday, 7 January 2024

Change in limits of integration when changing from cartesian to polar coordinates

While changing variables from x, y to r, theta in a double integral, if original limits go from -infinite to +infinite, then what would new limits go to? Please explain step by step.

When changing variables from Cartesian coordinates (x, y) to polar coordinates (r, θ) in a double integral, the limits of integration need to be adjusted accordingly. If the original limits for x and y extend from negative infinity to positive infinity, it typically implies that you are integrating over the entire plane. In polar coordinates, the corresponding region would be described using the radial coordinate (r) and the angular coordinate (θ).

Let's go through the process step by step:

Original double integral:

f ( x , y ) d x d y \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} f(x, y) \,dx\,dy

Now, let's express the Cartesian coordinates (x, y) in terms of polar coordinates (r, θ):

x = r cos ( θ ) x = r \cos(\theta) y = r sin ( θ ) y = r \sin(\theta)

Next, we need to express the differential area element d x d y dx\,dy in terms of polar coordinates. The area element in Cartesian coordinates is d x d y dx\,dy , and in polar coordinates, it becomes r d r d θ r\,dr\,d\theta . Therefore:

d x d y = r d r d θ dx\,dy = r\,dr\,d\theta

Now, substitute these expressions into the original integral:

f ( x , y ) d x d y = 0 2 π 0 f ( r cos ( θ ) , r sin ( θ ) ) r d r d θ \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} f(x, y) \,dx\,dy = \int_{0}^{2\pi} \int_{0}^{\infty} f(r \cos(\theta), r \sin(\theta)) \,r\,dr\,d\theta

In polar coordinates, the limits for r r typically start from 0 to \infty , and the limits for θ \theta range from 0 to 2 π 2\pi to cover the entire plane.

So, when changing variables from x, y to r, θ in a double integral where the original limits are from -\infty to + +\infty , the new limits become:

f ( x , y ) d x d y \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} f(x, y) \,dx\,dy

becomes

0 2 π 0 f ( r cos ( θ ) , r sin ( θ ) ) r d r d θ \int_{0}^{2\pi} \int_{0}^{\infty} f(r \cos(\theta), r \sin(\theta)) \,r\,dr\,d\theta

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