A function
is defined on the region
. Let
be the increment of
and
. Then
is called an increment of
and denoted by
.
If
is partially differentiable, then
, then we say a function
is totally diferentiable at
NOTE Note that we can express
as
is an increment of
as
moved to
. Then we can write
is an increment of
as
moved to
. Then we can write
The differential of
is denoted by
. Then for
is totally differentiable at
, Let
. Then
, where
can be expressed as
. Thus we write
is called taltal differential of
.
2.
3.

SOLUTION
1.
2.
3.
Since
, we approximate using these values. Increment of
can be approxiamted with the total differential of
that is
.
SOLUTION
Consider the function
. Let
. Then
. Now let
. Then
. Note that
. Thus
Thus for
, we have
. From this,
| Total Differentiability |
|---|
Use the contrapositive of Theorem4.2, if is not continuous at , then is not totally differentiable at .
|
NOTE Suppose that
is totally differentiable at
, then
.
Now we show that
is continuous at
. In other words, we show
. Then
is equivalent to
. Thus,
is continuous at
.
is partially differentiable with respect to
at
and
are continuous at
. Then
is totally differentiable at
.
| Check |
|---|
and
|
SOLUTION
Then
| Check | ||||||||
|---|---|---|---|---|---|---|---|---|
By Example4.8,
Then
is totally differentiable at only if
. Then
Then this limit depends on the value of . Thus it is not totally differentiable
|
| Check |
|---|
is totally differentiable at
is continuous at
. Now take the contrapositive to this statement. Then is not continuous at
is not totally differentiable at
.
|
Alernative Solution By Example4.8,
is partially differentiable at
. But by Example4.4,
is not continuous at
. Thus by Theorem4.2,
is not totally diffrentiable at
.
SOLUTION
and
. Then
is continuous at
. Thus by Theorem4.3,
is totally differentiable at
.
Altenative Solution
and
,
. Then
Thus,
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. Then
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|
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. Then
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is totally differentiable at
A vector orthogonal(perpendiculr) to the plane is called normal vector.
Thus the vector such as
is a normal vector.