Chapter 6 – Differentiation on  and Other Normed Linear Spaces
 and Other Normed Linear Spaces
1. Directional and Partial Derivatives
In Chapter 5 we considered functions f : E1 → E of one real variable.
Now we take up functions f : E′ → E where both E′ and E are normed spaces.
The scalar field of both is always assumed the same: E1 or C (the complex field). The case E = E∗ is excluded here; thus all is assumed finite.
We mostly use arrowed letters  for vectors in the domain space E′, and nonarrowed letters for those in E and for scalars.
 for vectors in the domain space E′, and nonarrowed letters for those in E and for scalars.
As before, we adopt the convention that f is defined on all of E′, with f(~x) = 0 if not defined otherwise.
Note that, if ~p ∈ E′, one can express any point  as
 as

with t ∈ E1 and ~u a unit vector. For if  set
 set

and if  set t = 0, and any ~u will do. We often use the notation
 set t = 0, and any ~u will do. We often use the notation

First of all, we generalize Definition 1 in Chapter 5,
Definition 1
Given  , we define the directional derivative of f along ~u (or ~u-directed derivative of f) at ~p by
, we define the directional derivative of f along ~u (or ~u-directed derivative of f) at ~p by

if this limit exists in E (finite). We also define the ~u-directed derived function,

as follows. For any 
 if this limit exists, otherwise.
  if this limit exists, otherwise.
Thus  is always defined, but the name derivative is used only if the limit (1) exists (finite). If it exists for each
 is always defined, but the name derivative is used only if the limit (1) exists (finite). If it exists for each  in a set B ⊆ E′, we call
 in a set B ⊆ E′, we call  (in classical notation ∂f/∂~u) the ~u-directed derivative of f on B.
 (in classical notation ∂f/∂~u) the ~u-directed derivative of f on B.
Note that, as t → 0,  tends to ~p over the line
 tends to ~p over the line  Thus
 Thus  can be treated as a relative limit over that line. Observe that it depends on both the direction and the length of
 can be treated as a relative limit over that line. Observe that it depends on both the direction and the length of  . Indeed, we have the following result.
. Indeed, we have the following result.
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