Eigenvalue of 0 and its physical meaning

Click For Summary
SUMMARY

The discussion centers on the conditions under which an eigenvalue can be zero and its implications in linear transformations. An eigenvalue of zero indicates that the matrix transformation is not invertible, collapsing all associated eigenvectors to the zero vector. This results in a kernel that contains all linear combinations of those eigenvectors. The mathematical definition states that an eigenvalue c is a solution to the equation det(A - cI) = 0, and if c equals zero, then det(A) must also equal zero, confirming the non-invertibility of the matrix.

PREREQUISITES
  • Understanding of linear algebra concepts, particularly eigenvalues and eigenvectors.
  • Familiarity with matrix operations and determinants.
  • Knowledge of linear transformations and their properties.
  • Basic comprehension of mathematical notation and definitions related to eigenvalues.
NEXT STEPS
  • Study the implications of eigenvalues in different physical systems, such as the moment of inertia tensor.
  • Learn about the process of diagonalization of matrices and its applications in simplifying linear transformations.
  • Explore the relationship between eigenvalues and stability in dynamical systems.
  • Investigate the geometric interpretation of eigenvalues and eigenvectors in multi-dimensional spaces.
USEFUL FOR

Students of mathematics, particularly those studying linear algebra, as well as physicists and engineers applying these concepts to real-world problems involving transformations and system dynamics.

EvLer
Messages
454
Reaction score
0
I need a bit of explanation on the conditions under which there is an eigenvalue that is equal to zero and what it's "physical" meaning.
Thanks in advance.
 
Physics news on Phys.org
We get an eigenvalue equal to zero only when the matrix transformation is not invertible.

So, the meaning it seems to me is that it maps all it's eigenvectors with respect to the eigenvalue 0 to 0. Therefore, all linear combinations of those eigenvectors are in the kernel of the transformation.
 
Mathematics concepts do NOT have "physical" meanings. Of course, when you apply mathematics to a specific physics problem, THEN they can have physical meanings relative to that problem. What physics problem are you applying eigenvalues to?
 
um, actually no physics, just math class, I was trying to get a better understanding of eigenvalues and how those two say something about each other, matrices and eigenvalues/vectors that is...
 
EvLer said:
um, actually no physics, just math class, I was trying to get a better understanding of eigenvalues and how those two say something about each other, matrices and eigenvalues/vectors that is...

It takes the eigenvectors and maps in it to the 0 vector. So, I guess you can say the "collaspe" to the 0 vector. That's probably all the "physical" meaning you can get.
 
By definition, an eigenvalue c will be a solution to det(A-cI)=0. If c=0, then det(A)=0.
 
ZioX said:
By definition, an eigenvalue c will be a solution to det(A-cI)=0. If c=0, then det(A)=0.

Really?

Let A = cI, then det(A-cI)=0, but det(A) is not equal to 0. How did you deduce that conclusion?
 
EvLer said:
um, actually no physics, just math class, I was trying to get a better understanding of eigenvalues and how those two say something about each other, matrices and eigenvalues/vectors that is...

ok, what I am going to say is not much of a "physical explanation" (it will really depend on the situation and application), but it may help you visualise what is going on.

you start with a set of axes (say the usual x, y), now you can represent an arbitrary vector, v, in this space (defined by your set of axes) using just a set of coordinates (with respect to those set of axes)... eg. v = (a,b)... etc...
now suppose you have an "operator" in this space, represented in a form of a 2x2 matrix. ok, this "operator" can be a representation of anything really (eg. evolution of prey-predator, interactions of system of particles...), it doesn't matter for our discussion here. But what is important is that this "operator" when acted on the vector, v, it changes the entries (a,b) to something else (via matrix multiplication). So Mv = w gives you a new vector w in this space.

Ok, now, if you look at your eigenvalues equation:
Mu = ku
where u is the eigenvector, k is the eigenvalue, you can see that u is a very special vector in the sense that the "operator" M does nothing but stretch or shrink the length of the eigenvector u by a factor of k (the e-vals)! The moral of this is that if you now express your original vector, v, with respect to the set of axes defined by e-vec u's (instead of the original set with x,y), your entries (a1, b1) where a1, b1 are different from a, b, would be transformed to (k1 a1, k2 b1) by the "operator", where k1 and k2 are the e-vals.

in most instances, such "change of basis" would make the physical interpretation of a system more transparent and simplier to anaylse.

for example, if your M is the moment of inertia matrix/tensor, then diagonalising it give you the principle axes of rotation (the direction of the e-vec's), while the e-vals are the "moment" about those axes.
 
JasonRox said:
Really?

Let A = cI, then det(A-cI)=0, but det(A) is not equal to 0. How did you deduce that conclusion?

What does that have to do with anything? You might want to reread what I said. In particular, what was the constraint on c?
 
Last edited:
  • #10
ZioX said:
By definition, an eigenvalue c will be a solution to det(A-cI)=0. If c=0, then det(A)=0.

JasonRox said:
Really?

Let A = cI, then det(A-cI)=0, but det(A) is not equal to 0. How did you deduce that conclusion?

?? If det(A) is not equal to 0, then c= 0 cannot be an eigenvalue! Ziox did say "If c= 0".
 

Similar threads

Replies
5
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
Replies
2
Views
1K
Replies
11
Views
2K
  • · Replies 24 ·
Replies
24
Views
4K
Replies
9
Views
2K
  • · Replies 2 ·
Replies
2
Views
980
  • · Replies 17 ·
Replies
17
Views
1K
  • · Replies 2 ·
Replies
2
Views
1K
Replies
5
Views
2K