Volume Differential
Volume differential, abbreviated as \(dV\), is an infinitesimally small element of volume used in physics, and engineering to analyze how quantities vary within a three-dimensional space. It represents the smallest meaningful “piece” of volume over which a function can be evaluated before being summed or integrated to obtain totals such as mass, charge, fluid flow, or energy.
Volume Differential (Cartesian Coordinates) Formula |
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| \( dV \;=\; dx \cdot dy \cdot dz \) | ||
| Symbol | English | Metric |
| \( dV \) = Volume Differential | \( in^3 \) | \( mm^3 \) |
| \( dx \) = Imperceptible Change in x-plane | \( in \) | \( mm \) |
| \( dy \) = Imperceptible Change in y-plane | \( in \) | \( mm \) |
| \( dz \) = Imperceptible Change in z-plane | \( in \) | \( mm \) |
The volume differential is written as \(dV\), and its specific form depends on the coordinate system being used. In Cartesian coordinates it takes the shape of a tiny rectangular box, while in cylindrical or spherical coordinates it becomes a small wedge-shaped or shell-shaped element. By using the volume differential, integrals can accurately represent continuous physical quantities distributed throughout a region in space.

Volume Differential (Cylindrical Coordinates) Formula |
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| \( dV \;=\; r \cdot dz \cdot dr \cdot d\theta \) | ||
| Symbol | English | Metric |
| \( dV \) = Volume Differential | \( in^3 \) | \( mm^2 \) |
| \( r \) = Radius | \( in \) | \( mm \) |
| \( dz \) = Imperceptible Change in z-plane | \( in \) | \( mm \) |
| \( dr \) = Imperceptible Change in Radius | \(in\) | \(mm\) |
| \( d\theta \) = Imperceptible Change in Degree | \(deg\) | \(rad\) |
Volume Differential (Spherical Coordinates) Formula |
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| \( dV \;=\; r^2 \cdot sin(\phi) \cdot dr \cdot d\phi \cdot d\theta \) | ||
| Symbol | English | Metric |
| \( dV \) = Volume Differential | \( in^3 \) | \( mm^2 \) |
| \( r \) = Radial Distance | \( in \) | \( mm \) |
| \( sin(\phi) \) = sin Polar Angle | \(deg\) | \(rad\) |
| \( dr \) = Imperceptible Change in Radius Distance | \(in\) | \(mm\) |
| \( d\phi \) = Imperceptible Change in Polar Angle | \(deg\) | \(rad\) |
| \( d\theta \) = Imperceptible Change in Azimuthal Angle | \(deg\) | \(rad\) |
