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Del Operator

Del Operator

The symbol Nabla symbol (∇), an inverted triangle used to represent the del or gradient vector operator in calculus., which stands for the "vector" 2D del operator as a vector of partial derivatives: (∂/∂x, ∂/∂y) or Row vector of partial derivative operators: (∂/∂x, ∂/∂y, ∂/∂z).

 

 

See also

Multivariable calculus, partial derivative, curly d

Key Formula

=xi^+yj^+zk^\nabla = \frac{\partial}{\partial x}\,\hat{\mathbf{i}} + \frac{\partial}{\partial y}\,\hat{\mathbf{j}} + \frac{\partial}{\partial z}\,\hat{\mathbf{k}}
Where:
  • \nabla = The del (or nabla) operator
  • x\frac{\partial}{\partial x} = Partial derivative with respect to x
  • y\frac{\partial}{\partial y} = Partial derivative with respect to y
  • z\frac{\partial}{\partial z} = Partial derivative with respect to z
  • i^,j^,k^\hat{\mathbf{i}},\,\hat{\mathbf{j}},\,\hat{\mathbf{k}} = Unit vectors along the x, y, and z axes

Worked Example

Problem: Given the scalar function f(x, y, z) = 3x² + 2yz, compute the gradient ∇f.
Step 1: Apply del to f by taking the partial derivative with respect to each variable.
f=fxi^+fyj^+fzk^\nabla f = \frac{\partial f}{\partial x}\,\hat{\mathbf{i}} + \frac{\partial f}{\partial y}\,\hat{\mathbf{j}} + \frac{\partial f}{\partial z}\,\hat{\mathbf{k}}
Step 2: Compute the partial derivative with respect to x, treating y and z as constants.
fx=6x\frac{\partial f}{\partial x} = 6x
Step 3: Compute the partial derivative with respect to y, treating x and z as constants.
fy=2z\frac{\partial f}{\partial y} = 2z
Step 4: Compute the partial derivative with respect to z, treating x and y as constants.
fz=2y\frac{\partial f}{\partial z} = 2y
Step 5: Combine the results into a vector.
f=6xi^+2zj^+2yk^\nabla f = 6x\,\hat{\mathbf{i}} + 2z\,\hat{\mathbf{j}} + 2y\,\hat{\mathbf{k}}
Answer: The gradient is ∇f = (6x, 2z, 2y). At the point (1, 2, 3), for instance, ∇f = (6, 6, 4).

Another Example

Problem: Given the vector field F(x, y, z) = (x², y², z²), compute the divergence ∇ · F.
Step 1: The divergence is the dot product of del with the vector field.
F=Fxx+Fyy+Fzz\nabla \cdot \mathbf{F} = \frac{\partial F_x}{\partial x} + \frac{\partial F_y}{\partial y} + \frac{\partial F_z}{\partial z}
Step 2: Compute each partial derivative.
x(x2)=2x,y(y2)=2y,z(z2)=2z\frac{\partial}{\partial x}(x^2) = 2x, \quad \frac{\partial}{\partial y}(y^2) = 2y, \quad \frac{\partial}{\partial z}(z^2) = 2z
Step 3: Sum the results.
F=2x+2y+2z\nabla \cdot \mathbf{F} = 2x + 2y + 2z
Answer: The divergence is ∇ · F = 2x + 2y + 2z. At the point (1, 1, 1), the divergence equals 6.

Frequently Asked Questions

What is the difference between gradient, divergence, and curl using the del operator?
All three use del (∇) but in different ways. The gradient (∇f) applies del to a scalar function, producing a vector that points in the direction of steepest increase. The divergence (∇ · F) takes the dot product of del with a vector field, producing a scalar that measures how much the field "spreads out." The curl (∇ × F) takes the cross product of del with a vector field, producing a vector that measures the field's rotation.
Is the del operator itself a vector?
Not exactly. Del is a vector differential operator — it looks and behaves like a vector in that it has three components (one for each coordinate direction), but each component is a partial derivative rather than a number. It only produces a meaningful result when it acts on a function or field.

Del operator (∇) vs. Laplacian operator (∇²)

The del operator ∇ is a first-order vector differential operator. The Laplacian ∇² (also written Δ) equals ∇ · ∇, meaning you apply del twice — first as a gradient, then take the divergence. The Laplacian is a second-order scalar operator: ∇²f = ∂²f/∂x² + ∂²f/∂y² + ∂²f/∂z². Del produces vectors (when used as a gradient), while the Laplacian produces scalars.

Why It Matters

The del operator is the central notational tool of vector calculus. It appears throughout physics — in Maxwell's equations for electromagnetism, the Navier-Stokes equations for fluid flow, and Schrödinger's equation in quantum mechanics. Without ∇, these fundamental laws would require far more cumbersome expressions involving separate partial derivatives for each coordinate.

Common Mistakes

Mistake: Treating ∇ as an ordinary vector that can stand alone without acting on something.
Correction: Del is an operator, not a standalone vector. Writing ∇ by itself has no meaning — it must operate on a scalar field (∇f) or combine with a vector field (∇ · F or ∇ × F).
Mistake: Confusing ∇f (gradient, a vector) with ∇ · F (divergence, a scalar).
Correction: The gradient applies del to a scalar and returns a vector. The divergence dots del with a vector field and returns a scalar. Pay attention to whether you are working with a scalar function or a vector field, and whether the operation uses multiplication, a dot product, or a cross product.

Related Terms