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Mama L [17]
3 years ago
10

Use variation of parameters to find a general solution to the differential equation given that the functions y1 and y2 are linea

rly independent solutions to the corresponding homogeneous equation for t > 0. ty" + (2t - 1 )y' - 2y = 6t^2 e^-2t​; y1 = 22t −​1, y2 = e^-2t
Mathematics
1 answer:
Gennadij [26K]3 years ago
3 0

Answer:

y_g(t) = c_1*( 2t - 1 ) + c_2*e^(^-^2^t^) - e^(^-^2^t^)* [ t^3 + \frac{3}{4}t^2 + \frac{3}{4}t ]

Step-by-step explanation:

Solution:-

- Given is the 2nd order linear ODE as follows:

                      ty'' + ( 2t - 1 )*y' - 2y = 6t^2 . e^(^-^2^t^)

- The complementary two independent solution to the homogeneous 2nd order linear ODE are given as follows:

                     y_1(t) = 2t - 1\\\\y_2 (t ) = e^-^2^t

- The particular solution ( yp ) to the non-homogeneous 2nd order linear ODE is expressed as:

                    y_p(t) = u_1(t)*y_1(t) + u_2(t)*y_2(t)

Where,

              u_1(t) , u_2(t) are linearly independent functions of parameter ( t )

- To determine [  u_1(t) , u_2(t) ], we will employ the use of wronskian ( W ).

- The functions [u_1(t) , u_2(t) ] are defined as:

                       u_1(t) = - \int {\frac{F(t). y_2(t)}{W [ y_1(t) , y_2(t) ]} } \, dt \\\\u_2(t) =  \int {\frac{F(t). y_1(t)}{W [ y_1(t) , y_2(t) ]} } \, dt \\

Where,

      F(t): Non-homogeneous part of the ODE

      W [ y1(t) , y2(t) ]: the wronskian of independent complementary solutions

- To compute the wronskian W [ y1(t) , y2(t) ] we will follow the procedure to find the determinant of the matrix below:

                      W [ y_1 ( t ) , y_2(t) ] = | \left[\begin{array}{cc}y_1(t)&y_2(t)\\y'_1(t)&y'_2(t)\end{array}\right] |

                      W [ (2t-1) , (e^-^2^t) ] = | \left[\begin{array}{cc}2t - 1&e^-^2^t\\2&-2e^-^2^t\end{array}\right] |\\\\W [ (2t-1) , (e^-^2^t) ]= [ (2t - 1 ) * (-2e^-^2^t) - ( e^-^2^t ) * (2 ) ]\\\\W [ (2t-1) , (e^-^2^t) ] = [ -4t*e^-^2^t ]\\

- Now we will evaluate function. Using the relation given for u1(t) we have:

                     u_1 (t ) = - \int {\frac{6t^2*e^(^-^2^t^) . ( e^-^2^t)}{-4t*e^(^-^2^t^)} } \, dt\\\\u_1 (t ) =  \frac{3}{2} \int [ t*e^(^-^2^t^) ] \, dt\\\\u_1 (t ) =  \frac{3}{2}* [ ( -\frac{1}{2} t*e^(^-^2^t^) - \int {( -\frac{1}{2}*e^(^-^2^t^) )} \, dt]  \\\\u_1 (t ) =  -e^(^-^2^t^)* [ ( \frac{3}{4} t +  \frac{3}{8} )]  \\\\

- Similarly for the function u2(t):

                     u_2 (t ) =  \int {\frac{6t^2*e^(^-^2^t^) . ( 2t-1)}{-4t*e^(^-^2^t^)} } \, dt\\\\u_2 (t ) =  -\frac{3}{2} \int [2t^2 -t ] \, dt\\\\u_2 (t ) =  -\frac{3}{2}* [\frac{2}{3}t^3 - \frac{1}{2}t^2  ]  \\\\u_2 (t ) =  t^2 [\frac{3}{4} - t ]

- We can now express the particular solution ( yp ) in the form expressed initially:

                    y_p(t) =  -e^(^-^2^t^)* [\frac{3}{2}t^2 + \frac{3}{4}t - \frac{3}{8} ]    + e^(^-^2^t^)*[\frac{3}{4}t^2 - t^3 ]\\\\y_p(t) =  -e^(^-^2^t^)* [t^3 + \frac{3}{4}t^2 + \frac{3}{4}t - \frac{3}{8} ] \\

Where the term: 3/8 e^(-2t) is common to both complementary and particular solution; hence, dependent term is excluded from general solution.

- The general solution is the superposition of complementary and particular solution as follows:

                    y_g(t) = y_c(t) + y_p(t)\\\\y_g(t) = c_1*( 2t - 1 ) + c_2*e^(^-^2^t^) - e^(^-^2^t^)* [ t^3 + \frac{3}{4}t^2 + \frac{3}{4}t ]

                   

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