The coordinate plane in two-dimensional space
 
  
As a coordinate plane  is referred to in the analytical geometry  one of two unit vectors  spanned original plane  . In two dimensions, the coordinate plane  corresponds to the Euclidean plane  and thus the base of a Cartesian coordinate system  . There are three coordinate planes in three-dimensional space: the xy plane  , the xz plane  and the yz plane  .
 
Analytical geometry  
Designations  
   
The three coordinate planes in three-dimensional space
 
  
In the following, the three coordinate axes  of three-dimensional space are denoted by , and . The three coordinate planes are often identified with the letter , which is provided with two indices that indicate the two unit vectors  that define the plane:
  
    
      
        
          
            R. 
           
          
            3 
           
         
       
     
    {\ displaystyle \ mathbb {R} ^ {3}} 
   
 
  
    
      
        
          x 
          
            1 
           
         
       
     
    {\ displaystyle x_ {1}} 
   
 
  
    
      
        
          x 
          
            2 
           
         
       
     
    {\ displaystyle x_ {2}} 
   
 
  
    
      
        
          x 
          
            3 
           
         
       
     
    {\ displaystyle x_ {3}} 
   
 
  
    
      
        E. 
       
     
    {\ displaystyle E} 
   
  
the plane is of the vectors and spanned
  
    
      
        
          x 
          
            1 
           
         
        
          x 
          
            2 
           
         
       
     
    {\ displaystyle x_ {1} x_ {2}} 
   
 
  
    
      
        
          E. 
          
            12 
           
         
       
     
    {\ displaystyle E_ {12}} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            1 
           
         
       
     
    {\ displaystyle {\ vec {e}} _ {1}} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            2 
           
         
       
     
    {\ displaystyle {\ vec {e}} _ {2}} 
   
  
the plane is of the vectors and spanned
  
    
      
        
          x 
          
            1 
           
         
        
          x 
          
            3 
           
         
       
     
    {\ displaystyle x_ {1} x_ {3}} 
   
 
  
    
      
        
          E. 
          
            13 
           
         
       
     
    {\ displaystyle E_ {13}} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            1 
           
         
       
     
    {\ displaystyle {\ vec {e}} _ {1}} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            3 
           
         
       
     
    {\ displaystyle {\ vec {e}} _ {3}} 
   
  
the plane is of the vectors and spanned
  
    
      
        
          x 
          
            2 
           
         
        
          x 
          
            3 
           
         
       
     
    {\ displaystyle x_ {2} x_ {3}} 
   
 
  
    
      
        
          E. 
          
            23 
           
         
       
     
    {\ displaystyle E_ {23}} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            2 
           
         
       
     
    {\ displaystyle {\ vec {e}} _ {2}} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            3 
           
         
       
     
    {\ displaystyle {\ vec {e}} _ {3}} 
   
  
 
Here are the three unit vectors , and . The three-dimensional space is divided into eight octants  by the three coordinate planes . The  intersection of  two coordinate planes results in a coordinate axis, the intersection of all three coordinate planes the  coordinate origin  .
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            1 
           
         
        = 
        ( 
        1 
        , 
        0 
        , 
        0 
        ) 
       
     
    {\ displaystyle {\ vec {e}} _ {1} = (1,0,0)} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            2 
           
         
        = 
        ( 
        0 
        , 
        1 
        , 
        0 
        ) 
       
     
    {\ displaystyle {\ vec {e}} _ {2} = (0,1,0)} 
   
 
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            3 
           
         
        = 
        ( 
        0 
        , 
        0 
        , 
        1 
        ) 
       
     
    {\ displaystyle {\ vec {e}} _ {3} = (0,0,1)} 
   
  
Plane equations  
The three coordinate planes are characterized by the following plane equations  :
Coordinate plane
 
Coordinate shape 
 
Normal form 
 
Parametric shape 
 
Intercept shape 
 
 
  
    
      
        
          E. 
          
            12 
           
         
       
     
    {\ displaystyle E_ {12}} 
   
  
  
    
      
        
          x 
          
            3 
           
         
        = 
        0 
       
     
    {\ displaystyle x_ {3} = 0} 
   
  
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            3 
           
         
        ⋅ 
        
          
            
              x 
              → 
             
           
         
        = 
        0 
       
     
    {\ displaystyle {\ vec {e}} _ {3} \ cdot {\ vec {x}} = 0} 
   
  
  
    
      
        
          
            
              x 
              → 
             
           
         
        = 
        s 
         
        
          
            
              
                e 
                → 
               
             
           
          
            1 
           
         
        + 
        t 
         
        
          
            
              
                e 
                → 
               
             
           
          
            2 
           
         
       
     
    {\ displaystyle {\ vec {x}} = s \, {\ vec {e}} _ {1} + t \, {\ vec {e}} _ {2}} 
   
  
not defined
 
 
  
    
      
        
          E. 
          
            13 
           
         
       
     
    {\ displaystyle E_ {13}} 
   
  
  
    
      
        
          x 
          
            2 
           
         
        = 
        0 
       
     
    {\ displaystyle x_ {2} = 0} 
   
  
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            2 
           
         
        ⋅ 
        
          
            
              x 
              → 
             
           
         
        = 
        0 
       
     
    {\ displaystyle {\ vec {e}} _ {2} \ cdot {\ vec {x}} = 0} 
   
  
  
    
      
        
          
            
              x 
              → 
             
           
         
        = 
        s 
         
        
          
            
              
                e 
                → 
               
             
           
          
            1 
           
         
        + 
        t 
         
        
          
            
              
                e 
                → 
               
             
           
          
            3 
           
         
       
     
    {\ displaystyle {\ vec {x}} = s \, {\ vec {e}} _ {1} + t \, {\ vec {e}} _ {3}} 
   
  
not defined
 
 
  
    
      
        
          E. 
          
            23 
           
         
       
     
    {\ displaystyle E_ {23}} 
   
  
  
    
      
        
          x 
          
            1 
           
         
        = 
        0 
       
     
    {\ displaystyle x_ {1} = 0} 
   
  
  
    
      
        
          
            
              
                e 
                → 
               
             
           
          
            1 
           
         
        ⋅ 
        
          
            
              x 
              → 
             
           
         
        = 
        0 
       
     
    {\ displaystyle {\ vec {e}} _ {1} \ cdot {\ vec {x}} = 0} 
   
  
  
    
      
        
          
            
              x 
              → 
             
           
         
        = 
        s 
         
        
          
            
              
                e 
                → 
               
             
           
          
            2 
           
         
        + 
        t 
         
        
          
            
              
                e 
                → 
               
             
           
          
            3 
           
         
       
     
    {\ displaystyle {\ vec {x}} = s \, {\ vec {e}} _ {2} + t \, {\ vec {e}} _ {3}} 
   
  
not defined
 
 
 
Here, a point of the respective level, the scalar product of  the vectors and as well as and are real numbers.
  
    
      
        
          
            
              x 
              → 
             
           
         
        = 
        ( 
        
          x 
          
            1 
           
         
        , 
        
          x 
          
            2 
           
         
        , 
        
          x 
          
            3 
           
         
        ) 
        ∈ 
        
          
            R. 
           
          
            3 
           
         
       
     
    {\ displaystyle {\ vec {x}} = (x_ {1}, x_ {2}, x_ {3}) \ in \ mathbb {R} ^ {3}} 
   
 
  
    
      
        
          
            
              x 
              → 
             
           
         
        ⋅ 
        
          
            
              y 
              → 
             
           
         
       
     
    {\ displaystyle {\ vec {x}} \ cdot {\ vec {y}}} 
   
 
  
    
      
        
          
            
              x 
              → 
             
           
         
       
     
    {\ displaystyle {\ vec {x}}} 
   
 
  
    
      
        
          
            
              y 
              → 
             
           
         
       
     
    {\ displaystyle {\ vec {y}}} 
   
 
  
    
      
        s 
       
     
    {\ displaystyle s} 
   
 
  
    
      
        t 
       
     
    {\ displaystyle t} 
   
  
Descriptive geometry  
In the representing geometry  , the three coordinate planes often correspond to the floor plan, the elevation plane and the cross elevation plane.
Synthetic geometry  
In the synthetic geometry  is an affine  or projective plane  , the (a coordinate range as a set with a specific algebraic structure planar ternary ring  , quasifield  , Alternatively body  , skew  , etc.) can be assigned, as a coordinate plane  on this generalized body  designated. 
literature  
Wolf-Dieter Klix, Karla Nestler: Constructive geometry  . Hanser, 2001, ISBN 3-446-21566-2  .  
 
Max Koecher, Aloys Krieg: level geometry  . 3. Edition. Springer, 2007, ISBN 3-540-49328-X  .  
 
 
Web links  
 
<img src="https://de.wikipedia.org//de.wikipedia.org/wiki/Special:CentralAutoLogin/start?type=1x1" alt="" title="" width="1" height="1" style="border: none; position: absolute;">