Linear equation

The name of the pictureThe name of the pictureThe name of the pictureClash Royale CLAN TAG#URR8PPP



Two Graphs of linear equations in two variables


In mathematics, a linear equation is an equation that may be put in the form


a1x1+⋯+anxn+b=0,displaystyle a_1x_1+cdots +a_nx_n+b=0,displaystyle a_1x_1+cdots +a_nx_n+b=0,

where x1,…,xndisplaystyle x_1,ldots ,x_nx_1,ldots ,x_n are the variables (or unknowns or indeterminates), and b,a1,…,andisplaystyle b,a_1,ldots ,a_ndisplaystyle b,a_1,ldots ,a_n are the coefficients, which are often real numbers. The coefficients may be considered as parameters of the equation, and may be stated as arbitrary expressions, restricted to not contain any of the variables. To yield a meaningful equation for non-zero values of b,displaystyle b,b, the coefficients are required not to be all zeros.


In the words of algebra, a linear equation is obtained by equating to zero a linear polynomial over some field, where the coefficients are taken from, and that does not contain the symbols for the indeterminates.


The solutions of such an equation are the values that, when substituted to the unknowns, make the equality true.


The case of just one variable is of particular importance, and it is frequent that the term linear equation refers implicitly to this particular case, in which the name unknown for the variable is sensibly used.


All the pairs of numbers that are solutions of a linear equation in two variables form a line in the Euclidean plane, and every line may be defined as the solutions of a linear equation. This is the origin of the term linear for qualifying this type of equations. More generally, the solutions of a linear equation in n variables form a hyperplane (of dimension n – 1) in the Euclidean space of dimension n.


Linear equations occur frequently in all mathematics and their applications in physics and engineering, partly because non-linear systems are often well approximated by linear equations.


This article considers the case of a single equation with coefficients from the field of real numbers, for which one studies the real solutions. All its content applies for complex solutions and, more generally, for linear equations with coefficient and solutions in any field. For the case of several simultaneous linear equations, see System of linear equations.




Contents





  • 1 One variable


  • 2 Two variables

    • 2.1 In Cartesian coordinates


    • 2.2 Slope–intercept form


    • 2.3 Point–slope form


    • 2.4 Intercept form


    • 2.5 Two-point form

      • 2.5.1 Expanded form


      • 2.5.2 Symmetric form


      • 2.5.3 Determinant form


      • 2.5.4 Mnemonic determinant


      • 2.5.5 Vectorial treatment



    • 2.6 Matrix form


    • 2.7 Parametric form


    • 2.8 Connection with linear functions


    • 2.9 Example



  • 3 More than two variables


  • 4 See also


  • 5 Notes


  • 6 References


  • 7 External links




One variable


Frequently the term linear equation refers implicitly to the case of just one variable. This case, in which the name unknown for the variable is sensibly used, is of particular importance, since it offers a unique value as solution to the equation. According to the above definition such an equation has the form


ax+b=0,displaystyle ax+b=0,displaystyle ax+b=0,

and, for a ≠ 0, a unique value as solution


x=−ba.displaystyle x=-frac ba.displaystyle x=-frac ba.

The above equation may always be rewritten to


ax=−b=b′,displaystyle ax=-b=b',displaystyle ax=-b=b',

and the solution is of course the same in both cases:


x=b′a=−ba.displaystyle x=frac b'a=-frac ba.displaystyle x=frac b'a=-frac ba.

In the case of a=0displaystyle a=0a=0, two possibilities emerge:



  1. b=0:displaystyle b=0:displaystyle b=0: Every value for xdisplaystyle xx is a solution to the equation 0⋅x+0=0,displaystyle 0cdot x+0=0,displaystyle 0cdot x+0=0, and


  2. b≠0:displaystyle bneq 0:displaystyle bneq 0: There is no solution for the equation 0⋅x+b=0,displaystyle 0cdot x+b=0,displaystyle 0cdot x+b=0, the equation is said to be inconsistent.


Two variables


In the case of just two variables the indexed variable names x1displaystyle x_1x_1 and x2displaystyle x_2x_2 and the respective coefficients a1displaystyle a_1a_1 and a2displaystyle a_2a_2 are often replaced, for the convenience of not having to deal with indices, by xdisplaystyle xx, ydisplaystyle yy, adisplaystyle aa and bdisplaystyle bb, respectively. As a consequence, the so called constant term, named coefficient bdisplaystyle bb in the above notation, must also be renamed; cdisplaystyle cc suggests itself. A linear equation in two variables is then denoted as


ax+by+c=0.displaystyle ax+by+c=0.displaystyle ax+by+c=0.

Any change to such an equation that does not alter the set of solutions, i.e., the set of pairs (x,y)displaystyle (x,y)(x,y), that satisfy this equation (i.e., make it an identity), generates an equivalent equation. It is immediate that changing the involved names (e.g. capitalizing names or using other letters) and also reordering the equation (e.g. by moving terms to the other side), does not change this set of solutions, and thus results in an equivalent equation, like, e.g.



Ax+By=C,displaystyle Ax+By=C,quad displaystyle Ax+By=C,quad with A=a,B=bdisplaystyle quad A=a,;B=bquad displaystyle quad A=a,;B=bquad and C=−c.displaystyle quad C=-c.displaystyle quad C=-c.

These equivalent variants are sometimes given generic names, like general form or standard form,[1] but contribute no new concepts.


The set of solutions also does not change when both sides of the equation are multiplied by the same non-zero number. According to the above definition, adisplaystyle aa and bdisplaystyle bb (identically Adisplaystyle AA and Bdisplaystyle BB) are not both zero, so multiplying the equation by the reciprocal of one of these non-zero coefficients, results in an equivalent equation with +1displaystyle +1+1 as the coefficient of one variable. This variable can be isolated on the left hand side, leaving an expression, possibly containing the other variable on the right hand side. This leads to either



b≠0:y=mx+y0,displaystyle bneq 0:quad y=mx+y_0,quad ;displaystyle bneq 0:quad y=mx+y_0,quad ; with m=−abdisplaystyle quad m=-frac abquad ;displaystyle quad m=-frac abquad ; and y0=−cb,displaystyle quad y_0=-frac cb,quad displaystyle quad y_0=-frac cb,quad or


a≠0:x=m′y+x0,displaystyle aneq 0:quad x=m'y+x_0,quad displaystyle aneq 0:quad x=m'y+x_0,quad with m′=−badisplaystyle quad m'=-frac baquad displaystyle quad m'=-frac baquad and x0=−ca.displaystyle quad x_0=-frac ca.displaystyle quad x_0=-frac ca.

When both coefficients adisplaystyle aa and bdisplaystyle bb are not zero, then both forms exist, and, assuming real numbers as coefficients and for the domain of the variables, the set of solutions for both equations can then be denoted as



S=∀x∈R,displaystyle S=(x,mx+y_0),quad displaystyle S=(x,mx+y_0),quad which is equal to the set S=∀y∈R.displaystyle quad S=(m'y+x_0,y).displaystyle quad S=(m'y+x_0,y).

In this case both components of the pairs in the set Sdisplaystyle SS vary over all real numbers, thereby depending in a so called linear affine manner on the respective other.


When exactly one coefficient, either adisplaystyle aa or bdisplaystyle b b, is not zero, then one equation remains, which is either



y=y0,displaystyle y=y_0,quad displaystyle y=y_0,quad for a=0,b≠0,displaystyle quad a=0,;bneq 0,quad displaystyle quad a=0,;bneq 0,quad with the set of solutions Sx=(x,y0),displaystyle quad S_x=;forall xin mathbb R ,quad displaystyle quad S_x=;forall xin mathbb R ,quad or


x=x0,displaystyle x=x_0,quad displaystyle x=x_0,quad for b=0,a≠0,displaystyle quad b=0,;aneq 0,quad displaystyle quad b=0,;aneq 0,quad with the set of solutions Sy=∀y∈R.displaystyle quad S^y=;forall yin mathbb R .displaystyle quad S^y=;forall yin mathbb R .

For both alternatives this is a set of pairs of numbers, where either the second component is a constant, and the first varies over all the reals (Sxdisplaystyle S_xS_x), or the first is a constant, and the second varies over all the reals (Sydisplaystyle S^ydisplaystyle S^y).



In Cartesian coordinates


Every single solution of a linear equation in two variables can be interpreted as two coordinate values, fixing a point in the Euclidean plane with a Cartesian coordinate system. The sets of solutions of such an equation make up a two-dimensional graph, which can be depicted in this plane. Conventionally, the first component of a solution (x,y)displaystyle (x,y)(x,y), the xdisplaystyle xx-value, is assigned to a horizontally drawn xdisplaystyle xx-axis, and the second component, the ydisplaystyle yy-value, to a vertical ydisplaystyle yy-axis.




Vertical Line x=x0displaystyle x=x_0 x = x_0
(in the picture:x0↦a)displaystyle (textin the picture:;x_0mapsto a)displaystyle (textin the picture:;x_0mapsto a)


In the case of a≠0,b=0displaystyle aneq 0,;b=0displaystyle aneq 0,;b=0 the equation is x=x0,displaystyle x=x_0,displaystyle x=x_0, and the set of its solutions Sy=∀y∈Rdisplaystyle S^y=;forall yin mathbb R displaystyle S^y=;forall yin mathbb R has a vertical line as its graph, as shown in the figure to the right. The value x0=−ca,displaystyle x_0=-tfrac ca,displaystyle x_0=-tfrac ca, where the line intersects the xdisplaystyle xx-axis in the point (x0,0)displaystyle (x_0,0)(x_0,0), is called an xdisplaystyle xx-intercept. Except for x0=0,displaystyle x_0=0,displaystyle x_0=0, when the graph coincides with the ydisplaystyle yy-axis, graphs of this kind do not intersect the ydisplaystyle yy-axis, they have no ydisplaystyle yy-intercept.


The set of solutions defines a function f(t)displaystyle f(t)f(t) and, simultaneously, the graph of this function, by interpreting the pairs (x,y)displaystyle (x,y)(x,y) as (t,f(t)),displaystyle (t,f(t)),displaystyle (t,f(t)), provided that any two such solutions that differ in their second value (y=f(t)displaystyle y=f(t)displaystyle y=f(t)), also differ in their respective first values (x=tdisplaystyle x=tdisplaystyle x=t). The set Sy=∀y∈Rdisplaystyle S^y=;forall yin mathbb R displaystyle S^y=;forall yin mathbb R violates this condition: all real values ydisplaystyle yy in the second component have the same first component x0.displaystyle x_0.x_0. Nevertheless, a graph for this set may be drawn, but it is not a graph of a function under the conventional assignment of axes, it obviously fails the vertical line test. This is the only type of straight line which is not the graph of any function f(t)displaystyle f(t)f(t).




Horizontal Line y=y0displaystyle y=y_0displaystyle y=y_0
(in the picture:y0↦b)displaystyle (textin the picture:;y_0mapsto b)displaystyle (textin the picture:;y_0mapsto b)


The sets Sxdisplaystyle S_xS_x and Sdisplaystyle SS satisfy the above condition, and the graph of Sx=(x,y0)displaystyle S_x=;forall xin mathbb R displaystyle S_x=;forall xin mathbb R is shown to the right. In this case of a=0,b≠0displaystyle a=0,;bneq 0displaystyle a=0,;bneq 0 the graph of the constant function f(x)=y=y0displaystyle f(x)=y=y_0displaystyle f(x)=y=y_0 is a horizontal line. The value y0=−cb,displaystyle y_0=-tfrac cb,displaystyle y_0=-tfrac cb, where the line intersects the ydisplaystyle yy-axis, is called ydisplaystyle yy-intercept. Except for y0=0,displaystyle y_0=0,displaystyle y_0=0, where the graph coincides with the xdisplaystyle xx-axis, graphs of this kind have no xdisplaystyle xx-intercept.


In the case of a≠0≠bdisplaystyle aneq 0neq bdisplaystyle aneq 0neq b with the equation y=mx+y0displaystyle y=mx+y_0displaystyle y=mx+y_0 the set of solutions is S=∀x∈R.displaystyle S=(x,mx+y_0).displaystyle S=(x,mx+y_0). It consists of pairs of numbers, with the first component varying over all the reals, and the other being calculated by a simple expression, representing a linear map (x↦mxdisplaystyle xmapsto mxdisplaystyle xmapsto mx) and adding a constant (y0displaystyle y_0y_0). This is sometimes called a linear affine function, or simply also linear function, slightly abusing the strict term linear. Also in this case the graph of a linear equation in two variables is a straight line (see figure at the top) that intersects the xdisplaystyle xx-axis at xdisplaystyle xx-intercept x0=−cadisplaystyle x_0=-tfrac cadisplaystyle x_0=-tfrac ca (i.e., (x0,0)displaystyle (x_0,0)(x_0,0) is a solution) and the ydisplaystyle yy-axis at the ydisplaystyle yy-intercept y0=−cbdisplaystyle y_0=-tfrac cbdisplaystyle y_0=-tfrac cb (i.e., (0,y0)displaystyle (0,y_0)displaystyle (0,y_0) is a solution).


Besides the intercepts being obvious from graphing the solutions of a linear equation in two variables, also their ratio (if it exists) can be graphically interpreted as determining the incline of the considered line (and all lines parallel to it). The slope of a straight line, usually introduced as rise over run, is the negative ratio of the rise, the ydisplaystyle yy-intercept, to the run, the xdisplaystyle xx-intercept. The negative sign accommodates for a positive slope, when the line rises for increasing xdisplaystyle xx-values. Immediately


−y0x0=−−cb−ca=−ab=m,displaystyle -frac y_0x_0=-frac -tfrac cb-tfrac ca=-frac ab=m,displaystyle -frac y_0x_0=-frac -tfrac cb-tfrac ca=-frac ab=m,

which holds if both intercepts exist. If the xdisplaystyle xx-intercept does not exist (a=0displaystyle a=0a=0), the slope mdisplaystyle mm equals 0,displaystyle 0,displaystyle 0, belonging to a horizontal line.


Since rise and run of a straight line can be determined not only between the intercept points and the origin (x0−0displaystyle x_0-0displaystyle x_0-0 and y0−0displaystyle y_0-0displaystyle y_0-0), but also between arbitrary points (x1,y1)displaystyle (x_1,y_1)(x_1,y_1) and (x2,y2)displaystyle (x_2,y_2)(x_2,y_2) on the line, the slope may also be determined by


m=y2−y1x2−x1=y1−y2x1−x2.displaystyle m=frac y_2-y_1x_2-x_1=frac y_1-y_2x_1-x_2.displaystyle m=frac y_2-y_1x_2-x_1=frac y_1-y_2x_1-x_2.

Denoting the angle enclosed by the xdisplaystyle xx-axis and the line as φ,displaystyle varphi ,varphi , then


tan⁡φ=m=−ab.displaystyle tan varphi =m=-frac ab.displaystyle tan varphi =m=-frac ab.

For b=0displaystyle b=0displaystyle b=0 the slope is undefined (φ=π/2displaystyle varphi =pi /2displaystyle varphi =pi /2).


This shows that only two of x0,y0displaystyle x_0,;y_0displaystyle x_0,;y_0 and mdisplaystyle mm can be selected independently.


With the premise that at least one axis is intersected, and since both intercept values may range over the whole real number line, all parallels to both axes as well as all oblique straight lines, i.e., in fact all straight lines in the Euclidean plane, can be expressed by linear equations in two variables, and all such equations denote either oblique or axis-parallel straight lines. Therefore all equations, equivalent to one of the above forms are often referred to as "equations of a line". They are adjusted to fit best to specific tasks, and are given therefore specific names, described below. In what follows, x,y,t,θdisplaystyle x,;y,;t,;theta displaystyle x,;y,;t,;theta are the names of variables, and other letters denote constants (fixed numbers) as coefficients.



Slope–intercept form


This form relies on the habit of writing y=f(x)displaystyle y=f(x)y=f(x) and the conventional way of assigning the variables of the linear equation to the axes of a Cartesian coordinate system, drawn in the conventional manner as described above. This form exists only for b≠0,displaystyle bneq 0,displaystyle bneq 0, allowing to isolate ydisplaystyle yy on the left hand side


y=mx+y0.displaystyle y=mx+y_0.displaystyle y=mx+y_0.

This way the slope m=−abdisplaystyle m=-tfrac abdisplaystyle m=-tfrac ab describes the inclination of the straight line which is the graph of this equation. The slope is positive for a line ascending to the right and negative, if the line ascends to the left. A zero-slope m=0displaystyle m=0m=0 belongs to a horizontal line.


The ydisplaystyle yy-intercept y0=−cbdisplaystyle y_0=-tfrac cbdisplaystyle y_0=-tfrac cb fixes the point (0,y0),displaystyle (0,y_0),displaystyle (0,y_0), where the line crosses the ydisplaystyle yy-axis, and y0=0displaystyle y_0=0y_0=0 characterizes lines that cross the origin (0,0).displaystyle (0,0).displaystyle (0,0).


Recalling the xdisplaystyle xx-intercept as x0=−ca,displaystyle x_0=-tfrac ca,displaystyle x_0=-tfrac ca, the above slope-intercept form, employing the slope mdisplaystyle mm and the ydisplaystyle yy-intercept, can be transformed to


y=−abx−cb=−ab(x+ba⋅cb)=m(x−x0),displaystyle y=-frac abx-frac cb=-frac ab(x+frac bacdot frac cb)=m(x-x_0),displaystyle y=-frac abx-frac cb=-frac ab(x+frac bacdot frac cb)=m(x-x_0),

involving the slope mdisplaystyle mm and the xdisplaystyle xx-intercept x0displaystyle x_0x_0.


In the case of b=0,displaystyle b=0,displaystyle b=0, there is no slope-intercept form in the above way, because a slope does not exist for φ=π/2displaystyle varphi =pi /2displaystyle varphi =pi /2.


For a≠0≠bdisplaystyle aneq 0neq bdisplaystyle aneq 0neq b it is possible to express the inverse functions f−1displaystyle f^-1f^-1 in the slope-intercept form as



x=m′y+x0,displaystyle x=m'y+x_0,quad displaystyle x=m'y+x_0,quad with m′=ba.displaystyle m'=tfrac ba.displaystyle m'=tfrac ba.

The graph of this equation, having the same set of solutions, is necessarily identical to the above graph, but depicting it under exchanged assignment of the variables to the coordinate-axes ((x,y)↦(y-axis,x-axis)displaystyle (x,y)mapsto (ytext-axis,;xtext-axis)displaystyle (x,y)mapsto (ytext-axis,;xtext-axis)), yields the usual f−1displaystyle f^-1f^-1-graph for inverse functions, the fdisplaystyle ff-graph mirrored along y=x.displaystyle y=x.displaystyle y=x. This holds for both (a=0,b≠0)displaystyle (a=0,;bneq 0)displaystyle (a=0,;bneq 0) and (b=0,a≠0).displaystyle (b=0,;aneq 0).displaystyle (b=0,;aneq 0).


The graph of a vertical line (b=0displaystyle b=0b=0) with no existing slope and the equation x=ddisplaystyle x=ddisplaystyle x=d changes under this inverted assignment to the graph of the function y=ddisplaystyle y=ddisplaystyle y=d with zero-slope (ddisplaystyle dd an arbitrary constant), and vice versa.



Point–slope form


It is observational evident that fixing an arbitrary point on a line and a slope uniquely defines this straight line. In the slope-intersect form this point on the line is either taken as the intersection (0,y0)displaystyle (0,y_0)displaystyle (0,y_0) with the ydisplaystyle yy-axis, or the intersection (x0,0)displaystyle (x_0,0)(x_0,0) with the xdisplaystyle xx-axis and is combined with the slope mdisplaystyle mm, provided its existence, to establish the equation for the according line. Generalizing this approach to an arbitrary point with coordinates (x1,y1)displaystyle (x_1,y_1)(x_1,y_1) yields:


y−y1=m(x−x1).displaystyle y-y_1=m(x-x_1).displaystyle y-y_1=m(x-x_1).

The point-slope form expresses the fact that the difference of the ydisplaystyle yy coordinates between two points on a line (i.e., y−y1displaystyle y-y_1displaystyle y-y_1) is proportional to the difference of the xdisplaystyle xx-coordinate (i.e., x−x1displaystyle x-x_1displaystyle x-x_1), with the proportionality constant m,displaystyle m,m, the slope of the line.



Intercept form


Straight lines that cross both coordinate axis outside the origin can be specified via the intercept form, that employs just these two values to specify an appropriate equation


xx0+yy0=1.displaystyle frac xx_0+frac yy_0=1.displaystyle frac xx_0+frac yy_0=1.

The intercept form results from moving cdisplaystyle cc in the equation ax+by+c=0displaystyle ax+by+c=0ax+by+c=0 to the right side, and then multiplying both sides of the equation with −1/c,displaystyle -1/c,displaystyle -1/c, yielding


(−ac)x+(−bc)y=1x0x+1y0y=1,displaystyle (-frac ac)x+(-frac bc)y=frac 1x_0x+frac 1y_0y=1,displaystyle (-frac ac)x+(-frac bc)y=frac 1x_0x+frac 1y_0y=1,

which is identical to the above form. The intercept form also works conveniently in higher dimensions for specifying (hyper)planes, when their intersections with all coordinate axes exist and are known.



Two-point form


Two points (x1,y1)displaystyle (x_1,y_1)(x_1,y_1) and (x2,y2)displaystyle (x_2,y_2)(x_2,y_2) with x1≠x2displaystyle x_1neq x_2displaystyle x_1neq x_2 (no vertical lines!) determine the slope of the line through these points. This slope, calculated as above, can be used with either point to employ the point-slope form, thereby establishing appropriate equations for this line, based on two points with different xdisplaystyle xx-values. This yields



y−yj=y2−y1x2−x1(x−xj),displaystyle y-y_j=frac y_2-y_1x_2-x_1(x-x_j),quad displaystyle y-y_j=frac y_2-y_1x_2-x_1(x-x_j),quad for j=1,2.displaystyle j=1,2.displaystyle j=1,2.

In the rest of this paragraph j=1displaystyle j=1j=1 is used.



Expanded form


Expanding, regrouping, and appropriately factoring the products leads to


(y1−y2)x+(x2−x1)y+(x1y2−x2y1)=0,displaystyle (y_1-y_2)x+(x_2-x_1)y+(x_1y_2-x_2y_1)=0,displaystyle (y_1-y_2)x+(x_2-x_1)y+(x_1y_2-x_2y_1)=0,

identifying: a=(y1−y2),b=(x2−x1),displaystyle quad a=(y_1-y_2),quad b=(x_2-x_1),quad displaystyle quad a=(y_1-y_2),quad b=(x_2-x_1),quad and c=(x1y2−x2y1).displaystyle quad c=(x_1y_2-x_2y_1).displaystyle quad c=(x_1y_2-x_2y_1).



Symmetric form


Multiplying both sides of the 2-point form by (x2−x1)displaystyle (x_2-x_1)(x_2-x_1) yields an equation in a symmetric form


(x2−x1)(y−y1)=(y2−y1)(x−x1).displaystyle (x_2-x_1)(y-y_1)=(y_2-y_1)(x-x_1).displaystyle (x_2-x_1)(y-y_1)=(y_2-y_1)(x-x_1).

This form also works in the case of a non-existing slope (x1=x2displaystyle x_1=x_2x_1=x_2), but requires y1≠y2displaystyle y_1neq y_2displaystyle y_1neq y_2 in this case: it correctly delivers x=x1.displaystyle quad x=x_1.displaystyle quad x=x_1.



Determinant form


The products in the above equation result also from the evaluation of a 2-rowed determinant, inducing this form of the linear equation:


|x−x1y−y1x2−x1y2−y1|=0.displaystyle beginvmatrixx-x_1&y-y_1\x_2-x_1&y_2-y_1endvmatrix=0.displaystyle beginvmatrixx-x_1&y-y_1\x_2-x_1&y_2-y_1endvmatrix=0.


Mnemonic determinant


The products on the left hand side of the expanded version can be reproduced by evaluating the 3-rowed determinant, designed for easy memorability:


|xy1x1y11x2y21|=0.displaystyle beginvmatrixx&y&1\x_1&y_1&1\x_2&y_2&1endvmatrix=0.displaystyle beginvmatrixx&y&1\x_1&y_1&1\x_2&y_2&1endvmatrix=0.


Vectorial treatment


Any pair of numbers (x,y)displaystyle (x,y)(x,y) may be treated as a vector, given by two components with respect to a Cartesian coordinate system. A (naive) vector starts at the origin (0,0)displaystyle (0,0)(0,0), and ends at the given coordinates. Any two non-collinear vectors (a1,a2)displaystyle (a_1,a_2)(a_1,a_2) and (b1,b2)displaystyle (b_1,b_2)displaystyle (b_1,b_2) span a parallelogram, with these three points. The area Adisplaystyle AA of this parallelogramm can be calculated as the magnitude of the exterior product (2dim-cross product, geometric product, ...) of these vectors. In components this can be done by evaluating the absolute value of a determinant with the components:


A=||a1a2b1b2||...

Two given points P1=(x1,y1),P2=(x2,y2)displaystyle P_1=(x_1,y_1),;P_2=(x_2,y_2)displaystyle P_1=(x_1,y_1),;P_2=(x_2,y_2) and an arbitrary third point P=(x,y)displaystyle P=(x,y)P=(x,y) are on one straight line (collinear), if, e.g., the vector from P1displaystyle P_1P_1 to P2displaystyle P_2P_2 and the vector from P1displaystyle P_1P_1 to Pdisplaystyle PP span no parallelogram, i.e., a parallelogram with area zero, i.e., also the vectors are collinear.


The vector from point P1displaystyle P_1P_1 to point P2displaystyle P_2P_2 can be expressed as


P12=P2−P1=(x2,y2)−(x1,y1)=(x2−x1,y2−y1)displaystyle P_12=P_2-P_1=(x_2,y_2)-(x_1,y_1)=(x_2-x_1,y_2-y_1)displaystyle P_12=P_2-P_1=(x_2,y_2)-(x_1,y_1)=(x_2-x_1,y_2-y_1)

and similarly the vector from point P1displaystyle P_1P_1 to an arbitrary point Pdisplaystyle PP is


P1.=P−P1=(x,y)−(x1,y1)=(x−x1,y−y1).displaystyle P_1.=P-P_1=(x,y)-(x_1,y_1)=(x-x_1,y-y_1).displaystyle P_1.=P-P_1=(x,y)-(x_1,y_1)=(x-x_1,y-y_1).

Equating the exterior product of these two vectors, as specified above, to zero, yields a linear equation


|x−x1y−y1x2−x1y2−y1|=0,displaystyle beginvmatrixx-x_1&y-y_1\x_2-x_1&y_2-y_1endvmatrix=0,displaystyle beginvmatrixx-x_1&y-y_1\x_2-x_1&y_2-y_1endvmatrix=0,

which is identical to the determinant form above.



Matrix form


Writing a linear equation in two unknowns in the form


Ax+By=C,displaystyle Ax+By=C,displaystyle Ax+By=C,

and considering the collection of coefficients (A,B)displaystyle (A,B)(A,B) as a (1,2)displaystyle (1,2)(1,2)-matrix, and the collection of variables (xy)displaystyle beginpmatrixx\yendpmatrixdisplaystyle beginpmatrixx\yendpmatrix as a (2,1)displaystyle (2,1)(2,1)-matrix, then their matrix product equals the (1,1)displaystyle (1,1)(1,1)-matrix (C):displaystyle beginpmatrixCendpmatrix:displaystyle beginpmatrixCendpmatrix:


(AB)(xy)=(C).displaystyle beginpmatrixA&Bendpmatrixbeginpmatrixx\yendpmatrix=beginpmatrixCendpmatrix.beginpmatrixA&Bendpmatrixbeginpmatrixx\yendpmatrix=beginpmatrixCendpmatrix.

This notation can easily expanded to more linear equations in more than two variables. For example, a system of two equations in two variables


A1x+B1y=C1,displaystyle A_1x+B_1y=C_1,,A_1x+B_1y=C_1,,

A2x+B2y=C2,displaystyle A_2x+B_2y=C_2,,A_2x+B_2y=C_2,,

can be denoted with a (2,2)displaystyle (2,2)(2,2)-matrix and a (2,1)displaystyle (2,1)(2,1)-matrix for the coefficients, by equaling the matrix product of the (2,2)displaystyle (2,2)(2,2)-coefficient matrix with the (2,1)displaystyle (2,1)(2,1)-variable matrix to the (2,1)displaystyle (2,1)(2,1)-matrix of the constant terms:


(A1B1A2B2)(xy)=(C1C2).displaystyle beginpmatrixA_1&B_1\A_2&B_2endpmatrixbeginpmatrixx\yendpmatrix=beginpmatrixC_1\C_2endpmatrix.beginpmatrixA_1&B_1\A_2&B_2endpmatrixbeginpmatrixx\yendpmatrix=beginpmatrixC_1\C_2endpmatrix.

A system of three linear equations in four variables would employ a (3,4)displaystyle (3,4)(3,4)-matrix for the coefficients of the variables, which, multiplied with the (4,1)displaystyle (4,1)displaystyle (4,1)-(column)-matrix of the variables, is equaled to the (3,1)displaystyle (3,1)(3,1)-matrix of the constant terms. For this ready extendability to higher dimensions, the matrix notation is a common representation tool for a system of linear equations, in linear algebra, and in computer programming. There are named methods for solving systems of linear equations, like Gauss-Jordan which can be expressed in matrix elementary row operations.



Parametric form


The parametric form of a curve is useful to e.g. describe the movement of a point along this curve, and controlling this movement with a single parameter. This setting resembles the task in physics, where a particle starts at time t=0displaystyle t=0t=0 at some point in space, say (h,k)displaystyle (h,k)(h,k), and travels along the curve, where it reaches point (p,q)displaystyle (p,q)(p,q) at time t=1.displaystyle t=1.t=1. With linear equations the curves are restricted to straight lines.


This task can be solved by adding a motion from h→pdisplaystyle hto pdisplaystyle hto p in the direction of the xdisplaystyle xx-axis and a simultaneous motion from k→qdisplaystyle kto qdisplaystyle kto q in the direction of the ydisplaystyle yy-axis, both motions controlled by the parameter t.displaystyle t.t. The motion in xdisplaystyle xx-direction can be described as


x=(k−h)t+hdisplaystyle x=(k-h)t+hdisplaystyle x=(k-h)t+h

and similarly, the motion in xdisplaystyle xx-direction can be described as


y=(q−k)t+k.displaystyle y=(q-k)t+k.displaystyle y=(q-k)t+k.

These two linear equations, with variables (t,x)displaystyle (t,x)(t,x) and (t,y)displaystyle (t,y)displaystyle (t,y), make up a parametric form for a linear equation with variables (x,y)displaystyle (x,y)(x,y) that can be constructed from the two-point form with (h,k)displaystyle (h,k)(h,k) and (p,q)displaystyle (p,q)(p,q) as points.


For t=0:(x,y)|t=0=(h,k)displaystyle t=0:quad (x,y)displaystyle t=0:quad (x,y) and for t=1:(x,y))|t=1=(p,q).displaystyle t=1:quad (x,y))displaystyle t=1:quad (x,y)) For all tdisplaystyle tt in the interval [0,1]displaystyle [0,1][0,1] the point (x,y)|tdisplaystyle (x,y)displaystyle (x,y) is on the straight line segment connecting the points for t=0displaystyle t=0t=0 and t=1.displaystyle t=1.t=1. This is sometimes called interpolation. For values of tdisplaystyle tt outside this interval, points outside of the segment, but still on the line are addressed extrapolation.



Connection with linear functions



A linear equation, written in the form y = f(x) whose graph crosses the origin (x,y) = (0,0), that is, whose y-intercept is 0, has the following properties:



  • Additivity: f(x1+x2)=f(x1)+f(x2) displaystyle f(x_1+x_2)=f(x_1)+f(x_2) f(x_1+x_2)=f(x_1)+f(x_2)


  • Homogeneity of degree 1: f(ax)=af(x),displaystyle f(ax)=af(x),,f(ax)=af(x),,

where a is any scalar. A function which satisfies these properties is called a linear function (or linear operator, or more generally a linear map). However, linear equations that have non-zero y-intercepts, when written in this manner, produce functions which will have neither property above and hence are not linear functions in this sense. They are known as affine functions.



Example


An everyday example of the use of different forms of linear equations is computation of tax with tax brackets. This is commonly done with a progressive tax computation, using either point–slope form or slope–intercept form.



More than two variables


For the general case of a linear equation with n>2displaystyle n>2n>2 unknowns the equation may always be assumed to be be denoted as at the top


a1x1+a2x2+⋯+anxn+b=0.displaystyle a_1x_1+a_2x_2+cdots +a_nx_n+b=0.displaystyle a_1x_1+a_2x_2+cdots +a_nx_n+b=0.

Sometimes bdisplaystyle bb is called the absolute term, and the term coefficient is reserved for the ai.displaystyle a_i.a_i. A variant to denote b,displaystyle b,b, stemming from the use in polynomials, is to write a0displaystyle a_0a_0 instead, alluding to the zeroth power of any variable, that always reduces to 1.displaystyle 1.1.


When dealing with n=3displaystyle n=3n=3 variables, it is common to use x,ydisplaystyle x,;ydisplaystyle x,;y and zdisplaystyle zz instead of indexed variables.


The set of solutions of such an equation is a set of ndisplaystyle nn-tuples, and each ndisplaystyle nn-tuple makes the equation an identity, when its components are inserted for the respective unknowns. The values of the variables with zero coefficients are taken arbitrarily from the field of coefficients.


For an equation to have meaningful solutions, at least one coefficient must be non-zero. This can be formulated as


a12+a22+⋯+an2=∑i=1nai2>0.displaystyle a_1^2+a_2^2+cdots +a_n^2=textstyle sum _i=1^na_i^2>0.displaystyle a_1^2+a_2^2+cdots +a_n^2=textstyle sum _i=1^na_i^2>0.

If all coefficients aidisplaystyle a_ia_i equal zero, then, as mentioned for one variable, the equation is either inconsistent (for b≠0displaystyle bneq 0displaystyle bneq 0) and there is no solution, or all
ndisplaystyle nn-tuples are solutions.


The set of solutions (ndisplaystyle nn-tuples) of a linear equation in ndisplaystyle nn variables is an (n−1)displaystyle (n-1)(n-1)-dimensional hyperplane in an ndisplaystyle nn-dimensional Euclidean space (or affine space if the coefficients are complex numbers or belong to any field). Within the usual setting of real numbers and a three-dimensional space with Cartesian coordinates, the set of the solutions of a linear equation with three variables describes a plane in the intuitive sense.


A given equation may be solved for all variables with a non-zero coefficient. Let jdisplaystyle jj be an index such that aj≠0,displaystyle a_jneq 0,displaystyle a_jneq 0, then


xj=−(baj+a1ajx1+⋯+0⋅xj+⋯+anajxn).displaystyle x_j=-(tfrac ba_j+tfrac a_1a_jx_1+cdots +0cdot x_j+cdots +tfrac a_na_jx_n).displaystyle x_j=-(tfrac ba_j+tfrac a_1a_jx_1+cdots +0cdot x_j+cdots +tfrac a_na_jx_n).

This way the linear equation can be seen as defining a function of (n−1)displaystyle (n-1)(n-1) variables, which maps, assuming the setting of reals, the set of (n−1)displaystyle (n-1)(n-1)-tuples[2] of reals to the real numbers, i.e.:


xj:Rn−1→Rdisplaystyle x_j:;mathbb R ^n-1to mathbb R displaystyle x_j:;mathbb R ^n-1to mathbb R


See also


  • Line (geometry)

  • Linear function

  • Linear equation over a ring

  • Algebraic equation

  • Linear belief function

  • Linear inequality


Notes




  1. ^ Barnett, Ziegler & Byleen 2008, pg. 15


  2. ^ The (n-1)-tuples are ordered to represent the removal of j from the sequence 1..n.




References



  • Barnett, R.A.; Ziegler, M.R.; Byleen, K.E. (2008), College Mathematics for Business, Economics, Life Sciences and the Social Sciences (11th ed.), Upper Saddle River, N.J.: Pearson, ISBN 0-13-157225-3.mw-parser-output cite.citationfont-style:inherit.mw-parser-output qquotes:"""""""'""'".mw-parser-output code.cs1-codecolor:inherit;background:inherit;border:inherit;padding:inherit.mw-parser-output .cs1-lock-free abackground:url("//upload.wikimedia.org/wikipedia/commons/thumb/6/65/Lock-green.svg/9px-Lock-green.svg.png")no-repeat;background-position:right .1em center.mw-parser-output .cs1-lock-limited a,.mw-parser-output .cs1-lock-registration abackground:url("//upload.wikimedia.org/wikipedia/commons/thumb/d/d6/Lock-gray-alt-2.svg/9px-Lock-gray-alt-2.svg.png")no-repeat;background-position:right .1em center.mw-parser-output .cs1-lock-subscription abackground:url("//upload.wikimedia.org/wikipedia/commons/thumb/a/aa/Lock-red-alt-2.svg/9px-Lock-red-alt-2.svg.png")no-repeat;background-position:right .1em center.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registrationcolor:#555.mw-parser-output .cs1-subscription span,.mw-parser-output .cs1-registration spanborder-bottom:1px dotted;cursor:help.mw-parser-output .cs1-hidden-errordisplay:none;font-size:100%.mw-parser-output .cs1-visible-errorfont-size:100%.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration,.mw-parser-output .cs1-formatfont-size:95%.mw-parser-output .cs1-kern-left,.mw-parser-output .cs1-kern-wl-leftpadding-left:0.2em.mw-parser-output .cs1-kern-right,.mw-parser-output .cs1-kern-wl-rightpadding-right:0.2em


External links



  • Linear Equations and Inequalities Open Elementary Algebra textbook chapter on linear equations and inequalities.


  • Hazewinkel, Michiel, ed. (2001) [1994], "Linear equation", Encyclopedia of Mathematics, Springer Science+Business Media B.V. / Kluwer Academic Publishers, ISBN 978-1-55608-010-4







Popular posts from this blog

California gubernatorial recall election

Telugu cinema

List of Pawn Stars episodes