MHB What Value of 'a' Yields One, None, or Infinite Solutions?

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The discussion centers on determining the value of 'a' in the system of equations to yield one, none, or infinite solutions. Specifically, it is established that if a = -1, there are no solutions due to a contradiction in the last equation. Conversely, if a ≠ -1, the system has infinitely many solutions as each value of 'w' leads to a unique 'z', 'y', and 'x' when a ≠ 2. If a = 2, 'x' can take any value, resulting in infinite solutions as well.

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(a-2)x+2y+3z=-1
y+z-w=0
2(1+a)z+(1+a)w=3

what a will give us:
1. One Solution
2. No solution at all.
3. Infinite Solutions

Thank you!
 
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Hello and welcome to MHB! :D

Can you post what you have tried so far so our helpers can see where you are having difficulty and offer the best help?
 
MarkFL said:
Hello and welcome to MHB! :D

Can you post what you have tried so far so our helpers can see where you are having difficulty and offer the best help?

I understand that if a=-1 than there is no solution. I tried to row the matrix but I couldn't finish it.
 
The augmented matrix of this system:
\[
\left(\begin{array}{@{}{cccc}|c@{}}
a-2 & 2 & 3 & 0 & -1\\
0 & 1 & 1 & -1 & 0\\
0 & 0 & 2(1+a) & 1+a & 3
\end{array}\right)
\]
is already in row echelon form. You are correct that if $a=-1$, then the last equation becomes $0z+0w=3$, and it has no solutions. If $a\ne-1$, then we can solve that equation for $z$:
\[
z=\frac{3-(1+a)w}{2(1+a)}
\]
so every value of $w$ gives a unique value of $z$ that satisfies the last equation. From the second equation, given $w$ and $z$, we can find a unique $y$ that satisfies the second equation. Finally, if $a\ne2$, then given $w$, $z$ and $y$ we can find a unique $x$ that satisfies the first equation. All this happens for every value of $w$, so in this case there are infinitely many solutions.

What happens when $a=2$? Consider the system without $x$ (whose augmented matrix lacks the first column) and determine how many solutions it has. But the coefficient of $x$ is 0 in all equations, so $x$ can be arbitrary.
 
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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