G.MATH
VECTOR INTEGRAL CALCULUS
The Gradient Vector Field

Okay guys and gals, now that you have some definitions of vector fields, it's time that we meet the famous del operator . In doing so, we will explore the vector-equivalent derivative in 3-dimenstional space.

Time we move from the number line to 3D space.
VIDEO LECTURE part 2


MAIN CONCEPTS
Meet the "del operator":
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CONCEPT
Let  be a real-value function of three variables. In the context of vectors, this function is called a scalar field. The gradient of , denoted by grad  or , is a vector field extracted from  according to the operation,

where each of these partial derivatives are defined. The notation  is read as “del phi” and  is called the del operator. While the geometric meaning of this operator will be elaborated later, just think of it as turning a scalar field to a vector field.

It also works on functions of two variable where  is a function of x and y, in which case

Ensure that you are taking partial derivatives which basically means holding the other variable fixed and differentiating accordingly to the w.r.t term, i.e.,  means holding y fixed and differentiating w.r.t to x.

 means the gradient of  evaluated at .

Let us look at a simple example. Suppose

then

I will now define a new term which you guys may be initially confused at. Don’t worry, you will be more familiar with it as we proceed in our learning.

The gradient of  is related to the directional derivative of . What is this directional derivative? Suppose we are given a point  in the direction of  specifying a direction from . The directional derivative of  at  in the direction of  is the rate of change of  with respect to  as  varies in the direction of  from . We denote this directional derivative as . The reason for the underlining is because the definition needs to have all three terms, ,  and . In order to under this a bit better, I will compare it with the derivative as we know in 1 variable calculus.

In single variable calculus, the derivative of  measures the rate of change of  was we vary . And in the number line,  can be varied in 2 ways, approaching it from the positive side or from the negative side as illustrated.

 

Now, let’s us move into 3-dimensional space and think of the vector analogy. In vectors, a point  in space is specificed by  and the function we apply is . We are to measure the rate of change of  but this time, in 3-dimensional space, we approach and pass through  using a vector, a vector which can originate from a variety of ways in the space and NOT limited to a number line like before. We designate this vector, unit vector , as illustrated

 

And this is exactly what the directional derivative means: rate of change of  with respect to  as  varies in the direction of  from .

Just think of it in this way. When I fly my F-22 through a point in space, I will experience a rate of change of turbulence depending on which direction I choose to travel through that point. So, if I pull up and travel through that point vertically up, the rate of change of turbulence will be different than if I just fly horizontally through it. It all depends on the vector I choose, or the unit vector .

While I understand that this lesson is about the gradient vector field, we shall soon see how this links with directional derivative. Right now, just get the meaning of the directional derivative.

All information presentated, less questions and exercises, is original content of Donny, with slight references to various books.
Video courtesy of YouTube.com service.
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