When we study analytical geometry at the undergraduate level we define free vectors as oriented line segments. This raises a problem when we try to formalize the multiplication of a free vector by a scalar. In order to elaborate on that, denote by $\mathbb V^3$ the set of free vectors. How can we show there exists a unique map
$$\cdot : \mathbb R\times \mathbb V^3\rightarrow \mathbb V^3, (\lambda, \overrightarrow{v})\mapsto \lambda \overrightarrow{v}$$
such that:
(1) $0\cdot \overrightarrow{v}=\overrightarrow{0}$
(2) $\lambda \overrightarrow{v}$ has the same direction as $\overrightarrow{v}$
(3) $\lambda \overrightarrow{v}$ has the same orientation as $\overrightarrow{v}$ if $\lambda>0$ and opposite orientation when $\lambda<0$
(4) $|\lambda \overrightarrow{v}|=|\lambda||\overrightarrow{v}|.$
Back in the past I found a book that proved this but I ended up forgetting which book was that. Do you know how to prove the existence of such a map or where I can find the proof?
Thanks.
You mention in a comment that you want to use the abstract Euclidean space $E$ rather than the coordinate space $\mathbb R^3$. The space $E$ has the nice property that every point in the space has equal status, unlike the space $\mathbb R^3$ in which one point, $(0,0,0),$ is singled out as the origin.
But this presents you with a special difficulty when you try to define your scalar product. The definition of the scalar product requires the existence of a unique vector $\vec 0$ such that for any vector $\vec v,$ no matter which you choose,
$$ 0 (\vec v) = \vec 0.$$
The question then is: which vector in $\mathbb V^3$ is $\vec 0$?
There can only be one zero vector, hence you must single out just one of your "free vectors" to be the zero vector. As soon as you do so, you have established a special point in your space $E,$ the same way that the origin is a special point in $R^3.$ In order to define a scalar product on your "free vectors," you are going to have to give up one of the most significant differences between your space and $R^3.$
Note that once you find $\vec 0$ such that $0 (\vec v) = \vec 0,$ the property $|\lambda \vec{v}|=|\lambda||\vec{v}|$ implies that $|\vec 0|=|0\vec v|=|0||\vec v| = 0.$ That is, both endpoints of $\vec 0$ must be the same point.
As long as you are willing to identify $\vec 0$ as a particular point in $E,$ you might as well call that point the origin of $E.$ You can then define $\lambda \vec v$ for any free vector $\vec v$ as follows:
For any point $p \in E,$ if $p = \vec 0$ then $\lambda p = \vec 0$; otherwise define $\lambda p$ as a point on the line through $\vec 0$ and $p$ such that the distance from $\vec 0$ to $\lambda p$ is $|\lambda|$ times the distance from $\vec 0$ to $p$ and such that $\vec 0$ is strictly between $p$ and $\lambda p$ if and only if $\lambda < 0.$
Then for any free vector $\vec v$, if $\vec v$ is the directed line segment from $p \in E$ to $q \in E,$ let $\lambda \vec v$ be the directed line segment from $\lambda p$ to $\lambda q.$
You can check that this satisfies all four of your properties.