Why Use Matrices for Linear Transformations?

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Using matrices for linear transformations simplifies the process of performing successive transformations, such as rotations, through matrix multiplication. Matrices allow for easier computation of eigenvalues and eigenvectors, providing insights like the axis of rotation without losing information. They convert conceptual operations into numerical ones, making calculations more straightforward, especially in physical applications with predefined coordinate systems. For example, computing derivatives using matrix representations clarifies operations across different bases. Overall, matrices enhance the efficiency and transparency of linear transformations in various contexts.
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Why would you want to use a matrix for a linear transformation?
Why not just use the given transformation instead of writing it as a matrix?
 
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If you have a number of rotations to be performed in succession, you can just multiply the matrices. Also you can determine information about a rotation, for example the axis of rotation, by calclulating the eigevectors of the matrix.
 
Using the transformation or using the matrix is equivalent. You won't lose information if you use the matrix.

If you want to keep on using the transformation, then you can do this. But in many cases, using the matrix is simply much easier. Finding eigenvalues for example is much easier with a matrix than with a transformation.
 
one reason is:

a matrix calculation reduces the computation of composition of linear transformations, as well as the computation of image elements under a linear transformation, to arithmatic operations in the underlying field. that is:

conceptual--->numerical.

sometimes, this is preferrable for getting "actual answers" in a physical application, where some preferred basis (coordinate system) might already be supplied.

for example, the differentiation operator is a linear transformation from Pn(F) to Pn(F).

actually "computing a derivative" IS just computing the matrix product [D]B[p]B = [p']B:

for n = 2, and F = R, we have for the basis B = {1,x,x2}, that [D]B=

[0 1 0]
[0 0 2]
[0 0 0],

or that if p(x) = a + bx + cx2,

p'(x) = b + 2cx.

of course, this would be just as easy using D(p) = p' using the calculus definition,

but it's not so clear what happens if you want to use THIS basis: {1+x,1-x,1-x2}, using the calculus definition, whereas the matrix form makes it transparent.
 
Is it by using a matrix representation of a derivative that CAS and programmable calculators evaluate derivatives?
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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