Therefore, the roots are, r₁ = 1, r2 = -1. Substitute r 1 in the system. www 1 -1 () ()-() = 3 -3 Then, from the reduced form, the equation obtained is, 1 - 2 = 0 Therefore, the corresponding eigen vector is obtained as, (²) = (1)
Therefore, the roots are, r₁ = 1, r2 = -1. Substitute r 1 in the system. www 1 -1 () ()-() = 3 -3 Then, from the reduced form, the equation obtained is, 1 - 2 = 0 Therefore, the corresponding eigen vector is obtained as, (²) = (1)
Therefore, the roots are, r₁ = 1, r2 = -1. Substitute r 1 in the system. www 1 -1 () ()-() = 3 -3 Then, from the reduced form, the equation obtained is, 1 - 2 = 0 Therefore, the corresponding eigen vector is obtained as, (²) = (1)
How do you get to the reduced form and then get the eigen vector in this problem?
Quantities that have magnitude and direction but not position. Some examples of vectors are velocity, displacement, acceleration, and force. They are sometimes called Euclidean or spatial vectors.
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