Understanding of Higher-Order Derivatives

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In summary, the derivative of a function f : \mathbb{R}^n \to \mathbb{R} is a linear map at each point, and the second derivative is a map from \mathbb{R}^n to the space of linear maps between the space of linear maps from \mathbb{R}^n to \mathbb{R} and \mathbb{R}^n . This continues for higher derivatives, and the reason we specify two arguments for the derivative is because the derivative itself is not necessarily linear, but rather a best linear approximation to the function.
  • #1
shaggymoods
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Hey guys, so this may be a really silly question, but I'm trying to grasp a subtle point about higher-order derivatives of multivariable functions. In particular, suppose we have an infinitely differentiable function

[tex]f: \mathbb{R}^{n} \rightarrow \mathbb{R}[/tex]

I know that the first derivative of this function is a linear map [tex]\lambda: \mathbb{R}^{n}\rightarrow\mathbb{R}[/tex]. However, when we take the second-derivative of [tex]\lambda[/tex], some questions arise for me:

1.) If we are taking this derivative when considering [tex]\lambda[/tex] as a linear function, then we'd just get back [tex]\lambda[/tex], which isn't the case. So how are we interpreting the first derivative when taking a second?

2.) In general, why do we say that [tex]D^{k}f:\mathbb{R}^{n^{k}}\rightarrow\mathbb{R}[/tex] and not [tex]D^{k}f:\mathbb{R}^{n}\rightarrow\mathbb{R}[/tex] ??

Thanks in advance.
 
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  • #2
If [tex] f : \mathbb{R}^n \to \mathbb{R} [/tex], then the derivative of [tex] f [/tex] is a linear map [tex]\lambda : \mathbb{R}^n \to \mathbb{R} [/tex] at each point in [tex] \mathbb{R}^n [/tex]. That is to say, the derivative of [tex] f [/tex], properly considered, is a map [tex] Df : \mathbb{R}^n \to L(\mathbb{R}^n, \mathbb{R}) [/tex], where [tex] L(\mathbb{R}^n, \mathbb{R}) [/tex] denotes the space of all linear maps [tex] \lambda : \mathbb{R}^n \to \mathbb{R} [/tex], which is just the dual of [tex] \mathbb{R}^n [/tex] (and is thus isomorphic to [tex] \mathbb{R}^n [/tex]). The second derivative of [tex] f [/tex] is then a map [tex] D^2 f : \mathbb{R}^n \to L(\mathbb{R}^n, L(\mathbb{R}^n, \mathbb{R})) \cong L(\mathbb{R}^n, \mathbb{R}^n) [/tex], where [tex] L(\mathbb{R}^n, \mathbb{R}^n) [/tex] is the space of all [tex] n \times n [/tex] matrices, and is isomorphic to [tex] \mathbb{R}^{n^2} [/tex]. (The output of the second derivative is usually called the Hessian matrix of [tex] f [/tex].) Continuing in this vein, you can show that [tex] D^k f [/tex] is a map from [tex] \mathbb{R}^n [/tex] to [tex] \mathbb{R}^{n^k} [/tex], not a map from [tex] \mathbb{R}^{n^k} \to \mathbb{R} [/tex] as you suggest in #2.

Basically, what's going on here is that a derivative, properly defined, is a best linear approximation to a function. Thus, at some point [tex] \mathbf{p} \in \mathbb{R}^n [/tex], the derivative [tex] Df [/tex] takes the value of the linear map [tex]\lambda : \mathbb{R}^n \to \mathbb{R} [/tex] which most closely resembles [tex] f [/tex] near [tex] \mathbf{p} [/tex]. Thus, [tex] Df [/tex] is actually a map from [tex] \mathbb{R}^n [/tex] into the space of all possible such approximations, and [tex] D^k f [/tex] is a map from [tex] \mathbb{R}^n [/tex] into some higher tensor product of [tex] \mathbb{R}^n [/tex] and its dual space. Your answer to #1 is thus that, while elements of the range of [tex] Df [/tex] must be linear maps and have trivial derivatives, [tex] Df [/tex] itself is not necessarily linear. This is why it is necessary to specify two arguments when evaluating [tex] Df [/tex]: a location [tex] \mathbf{a} [/tex], and a direction [tex] \mathbf{h} [/tex]. The location specifies a linear map, i.e., there is some linear map [tex] \lambda [/tex] for which [tex] Df : \mathbf{a} \mapsto \lambda [/tex]. The direction then serves as the argument for [tex] \lambda [/tex], and, in a slight abuse of notation, we usually write [tex] \lambda(\mathbf{h}) \equiv Df(\mathbf{a})(\mathbf{h}) [/tex] or [tex] Df(\mathbf{a}, \mathbf{h}) [/tex].
 

1. What are higher-order derivatives?

Higher-order derivatives refer to the derivatives of a function with respect to its independent variable, taken multiple times. In other words, it is the rate of change of a rate of change. For example, a second-order derivative is the rate of change of the first-order derivative, and a third-order derivative is the rate of change of the second-order derivative.

2. Why are higher-order derivatives important?

Higher-order derivatives are important because they provide more information about the behavior of a function. They can help us understand the concavity, inflection points, and maximum/minimum values of a function. They are also used in optimization problems and in physics to describe the acceleration of an object.

3. How do you find higher-order derivatives?

To find higher-order derivatives, we use the process of differentiation. We take the derivative of a function with respect to its independent variable as many times as needed. For example, to find the third-order derivative, we take the derivative of the second-order derivative.

4. What is the notation for higher-order derivatives?

The notation for higher-order derivatives is similar to that of first-order derivatives. The second-order derivative is denoted as f''(x) or d2f(x)/dx2. The third-order derivative is denoted as f'''(x) or d3f(x)/dx3. The notation continues with the number of apostrophes corresponding to the order of the derivative.

5. Can you give an example of a higher-order derivative?

Yes, the fourth-order derivative of the function f(x) = x3 is f''''(x) = 6. This means that the rate of change of the rate of change of the rate of change of the rate of change of x3 is 6. In other words, the function is accelerating at a constant rate of 6.

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