Imagine you’re exploring the invisible forces of nature—how does electricity move through a circuit, how do planets follow their curved paths, or how do fluids flow effortlessly through pipes?
The answer lies in vector calculus, the language of physics that reveals the hidden patterns in the universe.
Vector Calculus equips you with tools like the gradient to find steepest climbs, the divergence to measure spreading flows, and the curl to detect swirling motions. Whether you're decoding Maxwell's equations in electromagnetism or analyzing fluid dynamics, vector calculus is your key to unlocking the mysteries of the physical world!
Suppose that we have a function of three variables-say, V (x, y, z) in a
This tells us how V changes when we alter all three variables by the infinitesimal amounts dx, dy, dz. Notice that we do not require an infinite number of derivatives-three will suffice the partial derivatives along each of the three coordinate directions.
Thuswhere
is the gradient of V.
is a vector quantity with three components.
Like any vector, the gradient has magnitude and direction. To determine its geometrical meaning, let’s rewrite:
where
is the angle between
and
Now, if we fix the magnitude and search around in various directions (that is, vary
), the maximum change in V evidently occurs when
= 0 (for then cos
= 1). That is, for a fixed distance
, dT is greatest when one move in the same direction as
.
Thus, the gradient points in the direction of maximum increase of the function V.
Moreover, the magnitude gives the slope (rate of increase) along this maximal direction.
Gradient in Spherical polar coordinates
Gradient in cylindrical coordinates
Example 1:Find the gradient of a scalar function of position V where Calculate the magnitude of gradient at point
Example 2: Find the unit vector normal to the curve y = x2 at the point (2, 4, 1).
Solution:The equation of curve in the form of surface is given by
A constant scalar function V on the surface is given by V (x, y, z) = x2 - y
Taking the gradient
The value of the gradient at point (2, 4, 1),
The unit vector, as required
Example 3: In electrostatic field problems, the electric field is given by where V is the scalar field potential. If
in spherical coordinates, then find
.
The Operator
The gradient has the formal appearance of a vector “multiplying” a scalar V:
The term in parentheses is called “del”:
We should say that
is a vector operator that acts upon V, not a vector that multiplies V.
There are three ways the operator can act:
If
is a vector point function then
is called Divergence of
.
where
are the functions of x, y, z
Note:
1. Divergence of a vector is scalar.
2. Physically Divergence measures (outflow - inflow)
3. A vector whose divergence is zero then it is said to be divergence free vector (or) solenoid vector i.e. outflow = inflow = constant
is a measure of how much the vector
spreads out (diverges) from the point in question. For example, the vector function in figure (a) has a large (positive) divergence (if the arrows pointed in, it would be a large negative divergence), the function in figure (b) has zero divergence, and the function in figure (c) again has a positive divergence.
From the definition of we construct the curl
is a measure of how much the vector
“curls around” the point in question. Figure shown below have a substantial curl, pointing in the z-direction, as the natural right-hand rule would suggest.
Let ϕ1(x,y,z) = C, ϕ2(x,y,z) = C be given equations of two level surfaces and angle between these two surfaces are given as θ then cos θ
Note:
The angle between two surfaces is nothing but the angle between their normal.
then they are said to be orthogonal surfaces.
Example 4:The angle between the two surfaces x2 + y2+ z2 = 9 and z = x2 + y2 − 3 at the point (2, −1, 2) is
Solution:
Example 5: Find the curl of the vector
The directional derivative of a scalar function ϕ (x, y, z) in the direction of a vector
given as
ve then it is in the opposite direction.
Example 6: The Directional derivative of f(x, y, z) = x2yz + 4xz2 at (1, −2, −1) along (2i – j − 2k) is
Solution:
Directional Derivative =
At (1, −2, −1) we have
Example 7: The values of a, b, c so that the vector,
is irrotational.
Solution:
Given, that vector V is irrotational
⇒ c = −1, a = 4, b = 2
∴ a = 4, b = 2, c = −1
The gradient, the divergence, and the curl are the only first derivatives we can make with by applying
twice we can construct five species of second derivatives. The gradient
is a vector, so we can take the divergence and curl of it:
Divergence of gradient:
This object, which we write for short, is called the Laplacian of V. Notice that the Laplacian of a scalar V is a scalar.
Occasionally, we shall speak of the Laplacian of a vector, . By this we mean a vector quantity whose x-component is the Laplacian of Ax, and so on:
The divergence is a scalar-all we can do is taking its gradient.
The curl of a gradient is always zero:
The curl is a vector, so we can take its divergence and curl.
Notice that is not the same as the Laplacian of a vector:
The divergence of a curl, like the curl of a gradient, is always zero:
As you can check from the definition of
So curl-of-curl gives nothing new; the first term is just number (3) and the second is the Laplacian (of a vector).
1. What is the gradient of a vector field, and how is it calculated? | ![]() |
2. What is the divergence of a vector field and what does it signify? | ![]() |
3. How do you compute the curl of a vector field? | ![]() |
4. How do you find the angle between two surfaces using their gradients? | ![]() |
5. What are directional derivatives, and how are they calculated for a scalar function? | ![]() |