The target of this answer is to provide a certain understanding of the "configuration space" of triangles with side lengths $(a,b,c)$ (with $a,b,c >0$) :
For any such triple $(a,b,c)$, there exists an alternative representation $(u,v,w)$, (with $u,v,w>0$) such that :
$$\begin{cases}a&=&&&v&+&w\\
b&=&u&&&+&w\\
c&=&u&+&v&&\\\end{cases}\tag{1}$$
with a geometrical interpretation of $u,v,w$) that can be seen on Fig. 1

Fig.1 $u,v,w$ can be interpreted as the radii of mutually tangent circles centered in $A,B,C$ resp, all of them orthogonal to the incircle.
(1) can be written under the form :
$$\pmatrix{a\\b\\c}=\pmatrix{0&1&1\\1&0&1\\1&1&0} \pmatrix{u\\v\\w} \ \iff \ \pmatrix{u\\v\\w}=\tfrac12 \pmatrix{-1&1&1\\1&-1&1\\1&1&-1}\pmatrix{a\\b\\c} \tag{2}$$
As a consequence of (2), $u,v,w$ are positive due to triangle inequalities that can be written under the following form :
$$\begin{cases}(b+c)-a=2u > 0\\(c+a)-b=2v > 0\\(a+b)-c=2w > 0\end{cases}\tag{3}$$
Besides, (1) can be written in the following way :
$$\pmatrix{a\\b\\c}=u \pmatrix{0\\1\\1}+v \pmatrix{1\\0\\1}+w \pmatrix{1\\1\\0},\tag{4}$$
which means that the set of triangles can be represented wrt coordinates $a,b,c$ as
$$\text{the convex hull of half-lines} \ \ \mathbb{R}^+ \pmatrix{0\\1\\1}, \ \ \ \ \mathbb{R}^+ \pmatrix{1\\0\\1}, \ \ \ \ \mathbb{R}^+ \pmatrix{1\\1\\0}\tag{5}$$
Let us retrieve this result in a different manner.
Let us consider the Cayley-Menger determinant :
$$16\Delta ^{2}=\begin{vmatrix}0&1&1&1\\1&0&c^{2}&b^{2}\\1&c^{2}&0&a^{2}\\1&b^{2}&a^{2}&0\\\end{vmatrix} > 0 \tag{6}$$
where $\Delta$ is the area of the triangle.
In the present low-dimensional case, (6) is nothing else than Heron's formula
$$16 \Delta^2=(a+b+c)(b+c-a)(c+a-b)(a+b-c)\tag{7}$$
or, in terms of variables $u,v,w$, under the more compact form :
$$\Delta^2=(u+v+w)uvw\tag{8}$$
Expressing the positivity of product (7) is equivalent to say that the valid points are those already found in the first part : generic point $(a,b,c)$ must be on a certain side of three different planes, which amounts to say that it must belong to the non-bounded wedge-form volume whose truncation appears as a tetrahedron on Fig. 2.

Fig. 2.
Remark : the interest of Cayley-Menger expression is that it can be extended to any dimensions.