The Next Step (Plane Geometry) After Defining the Family of Distance Measuring Rays in the Cartesian Plane?












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We start with $(M,0,+) left( ; = (mathbb R^{ge 0},0,+) ; right)$, a system of magnitudes with an additive identity.



Consider linear isometric mappings $rho: M to mathbb R^2$, where the image of the mapping is a ray and the distance between any points $m.n in M$ is equal to the length of the line segment
joining $rho(m)$ and $rho(n)$.



Intuitively (to me anyway), the collection (and relations between rays and points) of all these isometric-rays describe the plane geometry. So the hunch is that we can abstract this and replace $mathbb R^2$ with a set of points $mathbb E^2 = text{Euclid's 2-Dim Plane}$ and a family of 'isometric-rays' satisfying a list of properties/axioms. In this system, the unit of measure on the plane is not defined but can be fixed when convenient. This makes sense - similar triangle can be defined using proportions, and a selected unit of measure is not required.




Has such a program been carried out?




I found this



Old and New Results in the
Foundations of
Elementary Plane Euclidean and
Non-Euclidean Geometries

by Marvin Jay Greenberg



but it was a recondite article and I didn't to see (on a quick review) any immediate connections.



For more along the same ideas, see the accepted answer from stack question



The status of high school geometry










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    We start with $(M,0,+) left( ; = (mathbb R^{ge 0},0,+) ; right)$, a system of magnitudes with an additive identity.



    Consider linear isometric mappings $rho: M to mathbb R^2$, where the image of the mapping is a ray and the distance between any points $m.n in M$ is equal to the length of the line segment
    joining $rho(m)$ and $rho(n)$.



    Intuitively (to me anyway), the collection (and relations between rays and points) of all these isometric-rays describe the plane geometry. So the hunch is that we can abstract this and replace $mathbb R^2$ with a set of points $mathbb E^2 = text{Euclid's 2-Dim Plane}$ and a family of 'isometric-rays' satisfying a list of properties/axioms. In this system, the unit of measure on the plane is not defined but can be fixed when convenient. This makes sense - similar triangle can be defined using proportions, and a selected unit of measure is not required.




    Has such a program been carried out?




    I found this



    Old and New Results in the
    Foundations of
    Elementary Plane Euclidean and
    Non-Euclidean Geometries

    by Marvin Jay Greenberg



    but it was a recondite article and I didn't to see (on a quick review) any immediate connections.



    For more along the same ideas, see the accepted answer from stack question



    The status of high school geometry










    share|cite|improve this question

























      0












      0








      0







      We start with $(M,0,+) left( ; = (mathbb R^{ge 0},0,+) ; right)$, a system of magnitudes with an additive identity.



      Consider linear isometric mappings $rho: M to mathbb R^2$, where the image of the mapping is a ray and the distance between any points $m.n in M$ is equal to the length of the line segment
      joining $rho(m)$ and $rho(n)$.



      Intuitively (to me anyway), the collection (and relations between rays and points) of all these isometric-rays describe the plane geometry. So the hunch is that we can abstract this and replace $mathbb R^2$ with a set of points $mathbb E^2 = text{Euclid's 2-Dim Plane}$ and a family of 'isometric-rays' satisfying a list of properties/axioms. In this system, the unit of measure on the plane is not defined but can be fixed when convenient. This makes sense - similar triangle can be defined using proportions, and a selected unit of measure is not required.




      Has such a program been carried out?




      I found this



      Old and New Results in the
      Foundations of
      Elementary Plane Euclidean and
      Non-Euclidean Geometries

      by Marvin Jay Greenberg



      but it was a recondite article and I didn't to see (on a quick review) any immediate connections.



      For more along the same ideas, see the accepted answer from stack question



      The status of high school geometry










      share|cite|improve this question













      We start with $(M,0,+) left( ; = (mathbb R^{ge 0},0,+) ; right)$, a system of magnitudes with an additive identity.



      Consider linear isometric mappings $rho: M to mathbb R^2$, where the image of the mapping is a ray and the distance between any points $m.n in M$ is equal to the length of the line segment
      joining $rho(m)$ and $rho(n)$.



      Intuitively (to me anyway), the collection (and relations between rays and points) of all these isometric-rays describe the plane geometry. So the hunch is that we can abstract this and replace $mathbb R^2$ with a set of points $mathbb E^2 = text{Euclid's 2-Dim Plane}$ and a family of 'isometric-rays' satisfying a list of properties/axioms. In this system, the unit of measure on the plane is not defined but can be fixed when convenient. This makes sense - similar triangle can be defined using proportions, and a selected unit of measure is not required.




      Has such a program been carried out?




      I found this



      Old and New Results in the
      Foundations of
      Elementary Plane Euclidean and
      Non-Euclidean Geometries

      by Marvin Jay Greenberg



      but it was a recondite article and I didn't to see (on a quick review) any immediate connections.



      For more along the same ideas, see the accepted answer from stack question



      The status of high school geometry







      soft-question axioms plane-geometry






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      share|cite|improve this question











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