Convert Triple Integral to Spherical Coordinates Calculator
This calculator converts triple integrals from Cartesian coordinates to spherical coordinates. Spherical coordinates are often more convenient for problems with spherical symmetry, such as calculating mass or charge distributions in a sphere.
Introduction
Triple integrals are used to calculate volumes, masses, and other quantities in three-dimensional space. Converting these integrals to spherical coordinates can simplify calculations for problems with spherical symmetry.
Spherical coordinates (r, θ, φ) are defined as:
- r: radial distance from the origin
- θ: azimuthal angle in the xy-plane from the positive x-axis
- φ: polar angle from the positive z-axis
The conversion from Cartesian coordinates (x, y, z) to spherical coordinates is given by:
x = r sinφ cosθ
y = r sinφ sinθ
z = r cosφ
Conversion Process
To convert a triple integral from Cartesian to spherical coordinates, follow these steps:
- Identify the limits of integration in Cartesian coordinates
- Convert the limits to spherical coordinates
- Determine the Jacobian determinant for the coordinate transformation
- Rewrite the integrand in terms of spherical coordinates
- Set up the integral in spherical coordinates
The Jacobian determinant for the transformation from Cartesian to spherical coordinates is:
J = r² sinφ
This means that dV = r² sinφ dr dθ dφ
Formula
The general formula for converting a triple integral from Cartesian to spherical coordinates is:
∫∫∫ f(x,y,z) dx dy dz = ∫∫∫ f(r sinφ cosθ, r sinφ sinθ, r cosφ) r² sinφ dr dθ dφ
Where:
- f(x,y,z) is the integrand in Cartesian coordinates
- r is the radial distance from the origin
- θ is the azimuthal angle in the xy-plane
- φ is the polar angle from the positive z-axis
Worked Example
Let's convert the following triple integral from Cartesian to spherical coordinates:
∫∫∫ (x² + y² + z²) dx dy dz
over the region where x² + y² + z² ≤ 1
In spherical coordinates, x² + y² + z² = r², so the integrand becomes r².
The limits of integration become:
- 0 ≤ r ≤ 1
- 0 ≤ θ ≤ 2π
- 0 ≤ φ ≤ π
The Jacobian determinant is r² sinφ, so the integral becomes:
∫₀^{2π} ∫₀^π ∫₀^1 r² * r² sinφ dr dφ dθ
This simplifies to:
∫₀^{2π} ∫₀^π ∫₀^1 r⁴ sinφ dr dφ dθ
The integral evaluates to (4π)/5.