Two linearly independent solutions of the differential equation y"...
Particular integral of y" - 2y' + y - e
x sin x is
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Two linearly independent solutions of the differential equation y"...
To find two linearly independent solutions of the differential equation y'' + 4y' + 4y = 0, we can assume a solution of the form y = e^(rx), where r is a constant.
Plugging this into the differential equation, we get:
r^2e^(rx) + 4re^(rx) + 4e^(rx) = 0
Dividing through by e^(rx), we have:
r^2 + 4r + 4 = 0
This is a quadratic equation in r. Solving for r, we get:
(r + 2)^2 = 0
r + 2 = 0
r = -2
Therefore, one solution of the differential equation is y1 = e^(-2x).
To find a second linearly independent solution, we can use the method of reduction of order. Let's assume a second solution of the form y2 = v(x)e^(-2x), where v(x) is another function to be determined.
Taking the first derivative of y2, we have:
y2' = v'(x)e^(-2x) - 2v(x)e^(-2x)
Taking the second derivative of y2, we have:
y2'' = v''(x)e^(-2x) - 4v'(x)e^(-2x) + 4v(x)e^(-2x)
Plugging y2 and its derivatives into the differential equation, we get:
(v''(x)e^(-2x) - 4v'(x)e^(-2x) + 4v(x)e^(-2x)) + 4(v'(x)e^(-2x) - 2v(x)e^(-2x)) + 4(v(x)e^(-2x)) = 0
Simplifying, we have:
v''(x)e^(-2x) = 0
v''(x) = 0
Integrating twice, we have:
v'(x) = c1
v(x) = c1x + c2
Therefore, the second solution of the differential equation is y2 = (c1x + c2)e^(-2x).
The two linearly independent solutions of the differential equation are y1 = e^(-2x) and y2 = (c1x + c2)e^(-2x), where c1 and c2 are arbitrary constants.