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1. Coordinate base representation of vector
Suppose there is a vector a ⃗ \vec{a} in the spacea, in different coordinate systems (or coordinate bases), vector a ⃗ \vec{a}aRepresented by different coordinate values.
When the coordinate base is uniquely determined, the corresponding coordinate values are also uniquely determined. At the same time, vectors can also be represented by a linear combination of coordinate values and coordinate lines.
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When the vector is a two-dimensional plane vector, it can be expressed as
a ⃗ = axe ⃗ 1 + aye ⃗ 2 = [ e ⃗ 1 e ⃗ 2 ] [ axay ] \vec{a} = a_x \vec{e}_1 + a_y \vec{e}_2 = \left[\begin{matrix}\vec{e}_1 & \vec{e}_2 \end{matrix}\right] \left[\begin{matrix}a_x \\ a_y \end {matrix}\right]a=axe1+aye2=[e1e2][axay] -
When the vector is a vector in a three-dimensional space, it can be expressed as
a ⃗ = ax ⃗ 1 + aye ⃗ 2 + aze ⃗ 3 = [ e ⃗ 1 e ⃗ 2 e ⃗ 3 ] [ axayaz ] \vec{a} = a_x \vec {e}_1 + a_y \vec{e}_2 + a_z \vec{e}_3 = \left[\begin{matrix}\vec{e}_1 & \vec{e}_2 & \vec{e}_3 \ end{matrix}\right] \left[\begin{matrix}a_x \\ a_y \\ a_z \end{matrix}\right]a=axe1+aye2+aze3=[e1e2e3] axayaz
2. Example of two-dimensional plane vector
The following is an example based on a vector in a two-dimensional plane, but the case in three-dimensional space has the same properties and conclusions.
Suppose there is a two-dimensional plane vector a ⃗ \vec{a} as mentioned abovea, in the standard coordinate base e ⃗ 1 = [ 1 0 ] , e ⃗ 2 = [ 0 1 ] \vec{e}_1=\left[\begin{matrix} 1 \\ 0 \\ \end{matrix}\right ], \vec{e}_2=\left[\begin{matrix} 0 \\ 1 \\ \end{matrix}\right]e1=[10],e2=[01] The coordinate value under is[ axay ] = [ 3 4 ] \left[\begin{matrix}a_x \\ a_y \end{matrix}\right] = \left[\begin{matrix}3 \\ 4 \end{ matrix}\right][axay]=[34] . Then this vector can be expressed as
a ⃗ = a x e ⃗ 1 + a y e ⃗ 2 = [ e ⃗ 1 e ⃗ 2 ] [ a x a y ] = 3 [ 1 0 ] + 4 [ 0 1 ] = [ 1 0 0 1 ] [ 3 4 ] = [ 3 4 ] \begin{aligned} \vec{a} &= a_x \vec{e}_1 + a_y \vec{e}_2 = \left[\begin{matrix}\vec{e}_1 & \vec{e}_2 \end{matrix}\right] \left[\begin{matrix}a_x \\ a_y \end{matrix}\right] \\ &= 3 \left[\begin{matrix}1 \\ 0 \end{matrix}\right] + 4 \left[\begin{matrix}0 \\ 1 \end{matrix}\right] = \left[\begin{matrix} 1 & 0 \\ 0 & 1 \end{matrix}\right] \left[\begin{matrix}3 \\ 4 \end{matrix}\right] = \left[\begin{matrix}3 \\ 4 \end{matrix}\right] \end{aligned} a=axe1+aye2=[e1e2][axay]=3[10]+4[01]=[1001][34]=[34]
Now, we change the coordinate base to e ⃗ 1 ′ = [ 1 2 1 2 ] , e ⃗ 2 ′ = [ − 1 2 1 2 ] \vec{e}_{1^\prime}=\left[\begin{ matrix} \frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \\ \end{matrix}\right], \vec{e}_{2^\prime }=\left[\begin{matrix} -\frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \\ \end{matrix}\right]e1′=[2121],e2′=[−2121] , the coordinate value under this new basis is[ ax ′ ay ′ ] = [ 7 2 1 2 ] \left[\begin{matrix}a_{x^\prime} \\ a_{y^\prime} \end{ matrix}\right] = \left[\begin{matrix} \frac{7}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \end{matrix}\right][ax′ay′]=[2721] . Then this vector can be expressed as
a ⃗ = 7 2 [ 1 2 1 2 ] + 1 2 [ − 1 2 1 2 ] = [ 1 2 − 1 2 1 2 1 2 ] [ 7 2 1 2 ] = [ 3 4 ] \begin{aligned} \vec{a} &= \frac{7}{\sqrt{2}} \left[\begin{matrix}\frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \end{matrix}\right] + \frac{1}{\sqrt{2}} \left[\begin{matrix}-\frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \end{matrix}\right] = \left[\begin{matrix} \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \end{matrix}\right] \left[\begin{matrix} \frac{7}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \end{matrix}\right] = \left[\begin{matrix}3 \\ 4 \end{matrix}\right] \end{aligned} a=27[2121]+21[−2121]=[2121−2121][2721]=[34]
From the above example, we can see that no matter which coordinate base is used, there will always be the following equation
a ⃗ = a x e ⃗ 1 + a y e ⃗ 2 = [ e ⃗ 1 e ⃗ 2 ] [ a x a y ] = a x ′ e ⃗ 1 ′ + a y ′ e ⃗ 2 ′ = [ e ⃗ 1 ′ e ⃗ 2 ′ ] [ a x ′ a y ′ ] \begin{aligned} \vec{a} &= a_x \vec{e}_1 + a_y \vec{e}_2 = \left[\begin{matrix}\vec{e}_1 & \vec{e}_2 \end{matrix}\right] \left[\begin{matrix}a_x \\ a_y \end{matrix}\right] \\ &= a_{x^\prime} \vec{e}_{1^\prime} + a_{y^\prime} \vec{e}_{2^\prime} = \left[\begin{matrix}\vec{e}_{1^\prime} & \vec{e}_{2^\prime} \end{matrix}\right] \left[\begin{matrix}a_{x^\prime} \\ a_{y^\prime} \end{matrix}\right] \end{aligned} a=axe1+aye2=[e1e2][axay]=ax′e1′+ay′e2′=[e1′e2′][ax′ay′]
Similar conclusions can be drawn for vectors in three-dimensional space.
As for how to obtain the coordinate values under the new basis, we can achieve it through the following steps
[ e ⃗ 1 e ⃗ 2 ] [ a x a y ] = [ e ⃗ 1 ′ e ⃗ 2 ′ ] [ a x ′ a y ′ ] [ e ⃗ 1 ′ e ⃗ 2 ′ ] − 1 [ e ⃗ 1 e ⃗ 2 ] [ a x a y ] = [ a x ′ a y ′ ] [ 1 2 − 1 2 1 2 1 2 ] − 1 [ 1 0 0 1 ] [ 3 4 ] = [ 7 2 1 2 ] \begin{aligned} \left[\begin{matrix}\vec{e}_1 & \vec{e}_2 \end{matrix}\right] \left[\begin{matrix}a_x \\ a_y \end{matrix}\right] &= \left[\begin{matrix}\vec{e}_{1^\prime} & \vec{e}_{2^\prime} \end{matrix}\right] \left[\begin{matrix}a_{x^\prime} \\ a_{y^\prime} \end{matrix}\right] \\ \left[\begin{matrix}\vec{e}_{1^\prime} & \vec{e}_{2^\prime} \end{matrix}\right]^{-1} \left[\begin{matrix}\vec{e}_1 & \vec{e}_2 \end{matrix}\right] \left[\begin{matrix}a_x \\ a_y \end{matrix}\right] &= \left[\begin{matrix}a_{x^\prime} \\ a_{y^\prime} \end{matrix}\right] \\ \left[\begin{matrix} \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \end{matrix}\right]^{-1} \left[\begin{matrix} 1 & 0 \\ 0 & 1 \end{matrix}\right] \left[\begin{matrix} 3 \\ 4 \end{matrix}\right] &= \left[\begin{matrix} \frac{7}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \end{matrix}\right] \\ \end{aligned} [e1e2][axay][e1′e2′]−1[e1e2][axay][2121−2121]−1[1001][34]=[e1′e2′][ax′ay′]=[ax′ay′]=[2721]
3. Matlab code verification
a_x = 3;
a_y = 4;
e_1 = [ 1
0];
e_2 = [ 0
1];
a_x_prime = 7/sqrt(2);
a_y_prime = 1/sqrt(2);
e_1_prime = [ sqrt(2)/2
sqrt(2)/2];
e_2_prime = [-sqrt(2)/2
sqrt(2)/2];
>> pinv([e_1_prime e_2_prime]) * [e_1 e_2] * [a_x; a_y]
ans =
4.9497
0.7071
>> a_x_prime
ans =
4.9497
>> a_y_prime
ans =
0.7071