$\def\b{\mathbb}\def\F{\b F}\def\R{\b R}\def\C{\b C}\def\n#1{\|#1\|}\def\abs#1{\left|#1\right|}$Setup: Let $X$ be a vector space over a field $\F$. (For simplicity, let $\F \in \{\R,\C\}$.) Let $\n\cdot$ be a norm on $X$, and let $f : X \to \F$ be a bounded linear functional.
Norm of Functionals: Recall that we can define the norm of $f$ by
$$\n f := \sup_{\substack{x \in X \\ x \ne 0}} \frac{\abs{f(x)}}{\n x} = \sup_{\substack{x \in X \\ \n x = 1}} \abs{f(x)}$$
Hyperplanes & $H_1$: Define now a hyperplane as follows. Let $Y$ be a subspace of $X$ with $\mathrm{codim} \; Y := \dim X/Y = 1$. The elements of the quotient space $X/Y$ are called hyperplanes parallel to $Y$.
In particular (cf. Kreyszig's Introduction to Functional Analysis, exercise $2.9.12$): if $f \ne 0$ is a functional on $X$, then the set $H_1$ defined by
$$H_1 := \Big\{ x \in X \; \Big| \; f(x) = 1 \Big\}$$
is a hyperplane parallel to the null space of $f$,
$$\mathcal N(f) := \Big\{ x \in X \; \Big| \; f(x) = 0 \Big\}$$
That is to say, since $\mathrm{codim}\, \mathcal N(f) = 1$ (as $f \ne 0$), then $H_1$ is parallel to $\mathcal N(f)$, and $H_1 \in X/\mathcal N(f)$.
The Property of Concern: Another exercise in Kreyszig ($2.9.14$) then gives the following property: within the previous circumstances, we may write
$$\n f = \frac{1}{\displaystyle \inf_{x \in H_1} \n x}$$
Alternatively, taking the convention of a distance between a point $x$ and a set $S$ in a metric space with metric $d$ to be
$$d(x,S) := \inf_{s \in S} d(x,s)$$
then we may equivalently write $\n f$ as being the reciprocal of the distance from the origin (or zero vector) and the hyperplane $H_1$, i.e.
$$\n f = \frac{1}{d(0,H_1)}$$
Of course in our context the distance (between points) is that induced by the norm, i.e.
$$d(x,y) := \n{x-y}$$
My Question: Normally it is very hard for me to imagine what the norm of a functional or operator might look like in the sense that norms generalize the Euclidean length/magnitude of vectors that we're used to. However, this seems to be very close to a very nice visual in my opinion, though I don't know what. The reciprocal in the statement of the property in particular seems problematic, yet possibly also hints at the notion of circles of inversion in some sense, but I wouldn't know nearly enough about that to flesh it out.
In any event, does anyone have a nice way to visualize the norm of a functional as given above? Examples in particular would be amazing; I would love to have some concrete visualizations of such an otherwise-abstract notion!
(To be clear, I do not need help proving these properties, I have already done so. Rather I seek a means of visualizing the norm of an operator as the reciprocal of the distance between it and the hyperplane $H_1$.)
Let us consider a linear functional $f:\Bbb R^2\to\Bbb R$ (with $f\neq0$). We imagine the functional as a plane in 3-dimensional space, as you described in the comments.
Now, imagine you are at the origin. Suppose you want to get to height $1$ as quickly as possible while walking on the plane given by $f$. To do this, you choose the direction of the steepest ascent.
While walking up the plane, you are at points of the form $(y_1,y_2,f(y))$, and you should also imagine the point $y$ below you at height $0$. Lets call this point the shadow.
If you have reached a point with height $1$, then your shadow is in the set $H_1$ (by definition of $H_1$). Since you have chosen the steepest ascent on the plane, this is actually the shortest path that you can take from $0$ to $H_1$, and your shadow has walked distance $d(0,H_1)$.
As you have shown, this is the inverse of the norm of $f$, so let us give some intuition for this inverse relationship. If you consider the functional $2f$, then you reach height $1$ twice as fast, and the length that you walk is therefore half as long. Similarly, if you consider a functional which is half as steep, then the distance $d(0,H_1)$ is twice as long.
what can we learn from this? We can observe that for the norm of a functional only the values of $f$ along the steepest ascent are relevant, it does not really matter what $f$ does in other direction, as long as $f$ is less steep in these other directions.
Remark on representation of functionals as a vector: In Hilbert spaces (such as the $n$-dimensional Euclidean spaces), functionals can be described using vectors of the space itself. Here, one should know that this representation is a multiple of the direction $x$ of the steepest ascent.