How can i solve the eigenvector equation for a $2 times 2$ matrix with eigenvalues $lambda = -1$ and...
where
$$A=begin{bmatrix}1&1\4&1end{bmatrix}$$
(For clarification, the materials i am using are telling me to use the following formula and to input the appropriate values for a, b, c and d but i am getting terribly confused.)
(a-λ)x+by=0
cx+(d-λ)y=0
linear-algebra eigenvalues-eigenvectors
add a comment |
where
$$A=begin{bmatrix}1&1\4&1end{bmatrix}$$
(For clarification, the materials i am using are telling me to use the following formula and to input the appropriate values for a, b, c and d but i am getting terribly confused.)
(a-λ)x+by=0
cx+(d-λ)y=0
linear-algebra eigenvalues-eigenvectors
add a comment |
where
$$A=begin{bmatrix}1&1\4&1end{bmatrix}$$
(For clarification, the materials i am using are telling me to use the following formula and to input the appropriate values for a, b, c and d but i am getting terribly confused.)
(a-λ)x+by=0
cx+(d-λ)y=0
linear-algebra eigenvalues-eigenvectors
where
$$A=begin{bmatrix}1&1\4&1end{bmatrix}$$
(For clarification, the materials i am using are telling me to use the following formula and to input the appropriate values for a, b, c and d but i am getting terribly confused.)
(a-λ)x+by=0
cx+(d-λ)y=0
linear-algebra eigenvalues-eigenvectors
linear-algebra eigenvalues-eigenvectors
edited Jan 2 at 20:51
RocketKangaroo
asked Jan 2 at 19:19
RocketKangarooRocketKangaroo
334
334
add a comment |
add a comment |
3 Answers
3
active
oldest
votes
It's pretty straightforward; I'll work out the case $lambda = 3$; suppose
$vec v = begin{pmatrix} a \ b end{pmatrix} tag 1$
is the eigenvector corresponding to $lambda = 3$; then
$A vec v = 3vec v; tag 2$
we write this equation out using the given entries of $A$, $vec v$:
$begin{bmatrix} 1 & 1 \ 4 & 1 end{bmatrix} begin{pmatrix} a \ b end{pmatrix} = 3 begin{pmatrix} a \ b end{pmatrix} = begin{pmatrix} 3a \ 3b end{pmatrix}, tag 3$
or
$a + b = 3a, tag 4$
$4a + b = 3b; tag 5$
from (4),
$b = 2a; tag 6$
it is expeditious at this point to observe we cannot have an eigenvector with $a = 0$, lest by (6) $b = 0$ as well, and thus
$vec v = 0; tag 7$
but eigenvectors are non-vanishing by definition. Thus
$a ne 0, tag 8$
and since eigenvectors are scalable, that is, the quality of "eigenvector-ness" is invariant under scalar multiplication, we may assume
$a = 1; tag 9$
then
$b = 2a = 2, tag{10}$
$vec v = begin{pmatrix} 1 \ 2 end{pmatrix}; tag{11}$
it is easy to see that
$4a + b = 4(1) + 2 = 6 = 3(2), tag{12}$
so $vec v$ also satisfies (5).
That's about it for the case $lambda = 3$; I leave the case $lambda = -1$ to the reader.
1
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
add a comment |
To find an eigenvector of $lambda=3$ you need to solve :
$$AX = lambda X $$
$$begin{bmatrix}1&1\4&1end{bmatrix}begin{bmatrix}x_1\x_2end{bmatrix}=3begin{bmatrix}x_1\x_2end{bmatrix}$$
$$x_1+x_2 = 3x_1 text{ and }4x_1+x_2=3x_2 $$
Thus $X=begin{bmatrix}1\2end{bmatrix}$ is an eigenvector for $lambda=3$.
You can do the same reasonning for $lambda=-1$.
1
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
1
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
add a comment |
The characteristic polynomial of $A$ is
$$
(lambda-1)^2-4=(lambda-1-2)(lambda-1+2)=(lambda-3)(lambda+1)
$$
Therefore $(A-3I)(A+I)=(A+I)(A-3I)=0$.
So the columns of $(A-3I)$ are solutions of $(A+I)X=0$. And the columns of $(A+I)$ are solutions of $(A-3I)X=0$.
Concretely,
$$
A-3I = left[begin{array}{cc}-2 & 1 \ 4 & -2end{array}right]
$$
So
$$
(A+I)left[begin{array}{c} 1 \ -2 end{array}right]=0
$$
And
$$
A+I = left[begin{array}{cc} 2 & 1 \ 4 & 2end{array}right]
$$
So
$$
(A-3I)left[begin{array}{c}1 \ 2end{array}right] = 0.
$$
add a comment |
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3 Answers
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active
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3 Answers
3
active
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It's pretty straightforward; I'll work out the case $lambda = 3$; suppose
$vec v = begin{pmatrix} a \ b end{pmatrix} tag 1$
is the eigenvector corresponding to $lambda = 3$; then
$A vec v = 3vec v; tag 2$
we write this equation out using the given entries of $A$, $vec v$:
$begin{bmatrix} 1 & 1 \ 4 & 1 end{bmatrix} begin{pmatrix} a \ b end{pmatrix} = 3 begin{pmatrix} a \ b end{pmatrix} = begin{pmatrix} 3a \ 3b end{pmatrix}, tag 3$
or
$a + b = 3a, tag 4$
$4a + b = 3b; tag 5$
from (4),
$b = 2a; tag 6$
it is expeditious at this point to observe we cannot have an eigenvector with $a = 0$, lest by (6) $b = 0$ as well, and thus
$vec v = 0; tag 7$
but eigenvectors are non-vanishing by definition. Thus
$a ne 0, tag 8$
and since eigenvectors are scalable, that is, the quality of "eigenvector-ness" is invariant under scalar multiplication, we may assume
$a = 1; tag 9$
then
$b = 2a = 2, tag{10}$
$vec v = begin{pmatrix} 1 \ 2 end{pmatrix}; tag{11}$
it is easy to see that
$4a + b = 4(1) + 2 = 6 = 3(2), tag{12}$
so $vec v$ also satisfies (5).
That's about it for the case $lambda = 3$; I leave the case $lambda = -1$ to the reader.
1
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
add a comment |
It's pretty straightforward; I'll work out the case $lambda = 3$; suppose
$vec v = begin{pmatrix} a \ b end{pmatrix} tag 1$
is the eigenvector corresponding to $lambda = 3$; then
$A vec v = 3vec v; tag 2$
we write this equation out using the given entries of $A$, $vec v$:
$begin{bmatrix} 1 & 1 \ 4 & 1 end{bmatrix} begin{pmatrix} a \ b end{pmatrix} = 3 begin{pmatrix} a \ b end{pmatrix} = begin{pmatrix} 3a \ 3b end{pmatrix}, tag 3$
or
$a + b = 3a, tag 4$
$4a + b = 3b; tag 5$
from (4),
$b = 2a; tag 6$
it is expeditious at this point to observe we cannot have an eigenvector with $a = 0$, lest by (6) $b = 0$ as well, and thus
$vec v = 0; tag 7$
but eigenvectors are non-vanishing by definition. Thus
$a ne 0, tag 8$
and since eigenvectors are scalable, that is, the quality of "eigenvector-ness" is invariant under scalar multiplication, we may assume
$a = 1; tag 9$
then
$b = 2a = 2, tag{10}$
$vec v = begin{pmatrix} 1 \ 2 end{pmatrix}; tag{11}$
it is easy to see that
$4a + b = 4(1) + 2 = 6 = 3(2), tag{12}$
so $vec v$ also satisfies (5).
That's about it for the case $lambda = 3$; I leave the case $lambda = -1$ to the reader.
1
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
add a comment |
It's pretty straightforward; I'll work out the case $lambda = 3$; suppose
$vec v = begin{pmatrix} a \ b end{pmatrix} tag 1$
is the eigenvector corresponding to $lambda = 3$; then
$A vec v = 3vec v; tag 2$
we write this equation out using the given entries of $A$, $vec v$:
$begin{bmatrix} 1 & 1 \ 4 & 1 end{bmatrix} begin{pmatrix} a \ b end{pmatrix} = 3 begin{pmatrix} a \ b end{pmatrix} = begin{pmatrix} 3a \ 3b end{pmatrix}, tag 3$
or
$a + b = 3a, tag 4$
$4a + b = 3b; tag 5$
from (4),
$b = 2a; tag 6$
it is expeditious at this point to observe we cannot have an eigenvector with $a = 0$, lest by (6) $b = 0$ as well, and thus
$vec v = 0; tag 7$
but eigenvectors are non-vanishing by definition. Thus
$a ne 0, tag 8$
and since eigenvectors are scalable, that is, the quality of "eigenvector-ness" is invariant under scalar multiplication, we may assume
$a = 1; tag 9$
then
$b = 2a = 2, tag{10}$
$vec v = begin{pmatrix} 1 \ 2 end{pmatrix}; tag{11}$
it is easy to see that
$4a + b = 4(1) + 2 = 6 = 3(2), tag{12}$
so $vec v$ also satisfies (5).
That's about it for the case $lambda = 3$; I leave the case $lambda = -1$ to the reader.
It's pretty straightforward; I'll work out the case $lambda = 3$; suppose
$vec v = begin{pmatrix} a \ b end{pmatrix} tag 1$
is the eigenvector corresponding to $lambda = 3$; then
$A vec v = 3vec v; tag 2$
we write this equation out using the given entries of $A$, $vec v$:
$begin{bmatrix} 1 & 1 \ 4 & 1 end{bmatrix} begin{pmatrix} a \ b end{pmatrix} = 3 begin{pmatrix} a \ b end{pmatrix} = begin{pmatrix} 3a \ 3b end{pmatrix}, tag 3$
or
$a + b = 3a, tag 4$
$4a + b = 3b; tag 5$
from (4),
$b = 2a; tag 6$
it is expeditious at this point to observe we cannot have an eigenvector with $a = 0$, lest by (6) $b = 0$ as well, and thus
$vec v = 0; tag 7$
but eigenvectors are non-vanishing by definition. Thus
$a ne 0, tag 8$
and since eigenvectors are scalable, that is, the quality of "eigenvector-ness" is invariant under scalar multiplication, we may assume
$a = 1; tag 9$
then
$b = 2a = 2, tag{10}$
$vec v = begin{pmatrix} 1 \ 2 end{pmatrix}; tag{11}$
it is easy to see that
$4a + b = 4(1) + 2 = 6 = 3(2), tag{12}$
so $vec v$ also satisfies (5).
That's about it for the case $lambda = 3$; I leave the case $lambda = -1$ to the reader.
answered Jan 2 at 19:50
Robert LewisRobert Lewis
43.9k22963
43.9k22963
1
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
add a comment |
1
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
1
1
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
Hi, could you expand on how you went from (3) to (6) please? I'm getting confused because the materials i am working from are telling me to use the following formula for a 2x2 matrix; (a-λ)x+by=0 and cx+(d-λ)y=0.
– RocketKangaroo
Jan 2 at 20:49
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
@RocketKangaroo: look at (4), which is just the first row of (3) written out. (4) says $a + b = 3a$; now subtract $a$ from both sides; you get (6), OK? The formula $(a - lambda)x + by = 0$ is also the first row of $Avec w = lambda vec w$ written out, with $A = begin{bmatrix} a & b \ c & d end{bmatrix}$ and $vec w = (x, y)^T$; from $A vec w = lambda vec w$ we get $ax + by = lambda a$ or $(a - lambda)x + by = 0$. It's just the general case of what I did. Does this help?
– Robert Lewis
Jan 2 at 20:57
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
Yes indeed, i'm still a little confused on how you figured out a = 1 however, is this because 0 cannot exist as an eigenvector?
– RocketKangaroo
Jan 2 at 21:25
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: see (6)-(7) and the words between; they explain why $a ne 0$; then we just multiply $vec v$ by $a^{-1}$, whatever $a ne 0$ may be.
– Robert Lewis
Jan 2 at 21:31
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
@RocketKangaroo: yes, because $0$ cannot be an eigenvector.
– Robert Lewis
Jan 2 at 21:32
add a comment |
To find an eigenvector of $lambda=3$ you need to solve :
$$AX = lambda X $$
$$begin{bmatrix}1&1\4&1end{bmatrix}begin{bmatrix}x_1\x_2end{bmatrix}=3begin{bmatrix}x_1\x_2end{bmatrix}$$
$$x_1+x_2 = 3x_1 text{ and }4x_1+x_2=3x_2 $$
Thus $X=begin{bmatrix}1\2end{bmatrix}$ is an eigenvector for $lambda=3$.
You can do the same reasonning for $lambda=-1$.
1
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
1
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
add a comment |
To find an eigenvector of $lambda=3$ you need to solve :
$$AX = lambda X $$
$$begin{bmatrix}1&1\4&1end{bmatrix}begin{bmatrix}x_1\x_2end{bmatrix}=3begin{bmatrix}x_1\x_2end{bmatrix}$$
$$x_1+x_2 = 3x_1 text{ and }4x_1+x_2=3x_2 $$
Thus $X=begin{bmatrix}1\2end{bmatrix}$ is an eigenvector for $lambda=3$.
You can do the same reasonning for $lambda=-1$.
1
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
1
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
add a comment |
To find an eigenvector of $lambda=3$ you need to solve :
$$AX = lambda X $$
$$begin{bmatrix}1&1\4&1end{bmatrix}begin{bmatrix}x_1\x_2end{bmatrix}=3begin{bmatrix}x_1\x_2end{bmatrix}$$
$$x_1+x_2 = 3x_1 text{ and }4x_1+x_2=3x_2 $$
Thus $X=begin{bmatrix}1\2end{bmatrix}$ is an eigenvector for $lambda=3$.
You can do the same reasonning for $lambda=-1$.
To find an eigenvector of $lambda=3$ you need to solve :
$$AX = lambda X $$
$$begin{bmatrix}1&1\4&1end{bmatrix}begin{bmatrix}x_1\x_2end{bmatrix}=3begin{bmatrix}x_1\x_2end{bmatrix}$$
$$x_1+x_2 = 3x_1 text{ and }4x_1+x_2=3x_2 $$
Thus $X=begin{bmatrix}1\2end{bmatrix}$ is an eigenvector for $lambda=3$.
You can do the same reasonning for $lambda=-1$.
answered Jan 2 at 19:38
JenniferJennifer
8,41721737
8,41721737
1
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
1
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
add a comment |
1
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
1
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
1
1
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
Gee, your answer is almost the same as mine! How could that possible be? ;) +1
– Robert Lewis
Jan 2 at 19:51
1
1
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
Yours is way more detailed :)
– Jennifer
Jan 2 at 19:53
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
True enough. Maybe I talk too much! ;)
– Robert Lewis
Jan 2 at 19:55
add a comment |
The characteristic polynomial of $A$ is
$$
(lambda-1)^2-4=(lambda-1-2)(lambda-1+2)=(lambda-3)(lambda+1)
$$
Therefore $(A-3I)(A+I)=(A+I)(A-3I)=0$.
So the columns of $(A-3I)$ are solutions of $(A+I)X=0$. And the columns of $(A+I)$ are solutions of $(A-3I)X=0$.
Concretely,
$$
A-3I = left[begin{array}{cc}-2 & 1 \ 4 & -2end{array}right]
$$
So
$$
(A+I)left[begin{array}{c} 1 \ -2 end{array}right]=0
$$
And
$$
A+I = left[begin{array}{cc} 2 & 1 \ 4 & 2end{array}right]
$$
So
$$
(A-3I)left[begin{array}{c}1 \ 2end{array}right] = 0.
$$
add a comment |
The characteristic polynomial of $A$ is
$$
(lambda-1)^2-4=(lambda-1-2)(lambda-1+2)=(lambda-3)(lambda+1)
$$
Therefore $(A-3I)(A+I)=(A+I)(A-3I)=0$.
So the columns of $(A-3I)$ are solutions of $(A+I)X=0$. And the columns of $(A+I)$ are solutions of $(A-3I)X=0$.
Concretely,
$$
A-3I = left[begin{array}{cc}-2 & 1 \ 4 & -2end{array}right]
$$
So
$$
(A+I)left[begin{array}{c} 1 \ -2 end{array}right]=0
$$
And
$$
A+I = left[begin{array}{cc} 2 & 1 \ 4 & 2end{array}right]
$$
So
$$
(A-3I)left[begin{array}{c}1 \ 2end{array}right] = 0.
$$
add a comment |
The characteristic polynomial of $A$ is
$$
(lambda-1)^2-4=(lambda-1-2)(lambda-1+2)=(lambda-3)(lambda+1)
$$
Therefore $(A-3I)(A+I)=(A+I)(A-3I)=0$.
So the columns of $(A-3I)$ are solutions of $(A+I)X=0$. And the columns of $(A+I)$ are solutions of $(A-3I)X=0$.
Concretely,
$$
A-3I = left[begin{array}{cc}-2 & 1 \ 4 & -2end{array}right]
$$
So
$$
(A+I)left[begin{array}{c} 1 \ -2 end{array}right]=0
$$
And
$$
A+I = left[begin{array}{cc} 2 & 1 \ 4 & 2end{array}right]
$$
So
$$
(A-3I)left[begin{array}{c}1 \ 2end{array}right] = 0.
$$
The characteristic polynomial of $A$ is
$$
(lambda-1)^2-4=(lambda-1-2)(lambda-1+2)=(lambda-3)(lambda+1)
$$
Therefore $(A-3I)(A+I)=(A+I)(A-3I)=0$.
So the columns of $(A-3I)$ are solutions of $(A+I)X=0$. And the columns of $(A+I)$ are solutions of $(A-3I)X=0$.
Concretely,
$$
A-3I = left[begin{array}{cc}-2 & 1 \ 4 & -2end{array}right]
$$
So
$$
(A+I)left[begin{array}{c} 1 \ -2 end{array}right]=0
$$
And
$$
A+I = left[begin{array}{cc} 2 & 1 \ 4 & 2end{array}right]
$$
So
$$
(A-3I)left[begin{array}{c}1 \ 2end{array}right] = 0.
$$
answered Jan 4 at 5:13
DisintegratingByPartsDisintegratingByParts
58.7k42579
58.7k42579
add a comment |
add a comment |
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