Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page 1
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1 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page Questions Example (3.6.) Find a particular solution of the differential equation y 5y + 6y = 2e t. Check your answer using Example (3.6.4) Find a particular solution of the differential equation 4y 4y + y = 6e t/2. Check your answer using Example (3.6.3) Verify that y (t) = t 2 and y 2 (t) = t are solutions of the corresponding homogeneous differential equation for t 2 y 2y = 3t 2 for t > 0. Then find a particular solution of the nonhomogeneous differential equation. Solutions Example (3.6.) Find a particular solution of the differential equation y 5y + 6y = 2e t. Check your answer using This is a nonhomogeneous constant coefficient equation. We first solve the associated homogeneous differential equation: y 5y + 6y = 0 Since this is a constant coefficient differential equation, we assume the solution looks like y = e rt. Then: y = e rt, y = re rt, y = r 2 e rt. y 5y + 6y = 0 (r 2 5r + 6)e rt = 0 r 2 5r + 6 = 0 characteristic equation (r 3)(r 2) = 0 The roots of the characteristic equation are r = 3 and r 2 = 2. A fundamental set of solutions to the associated homogeneous equation is y (t) = e 3t and y 2 (t) = e 2t. The complementary solution is therefore y c (t) = c i y i (t) = c e 3t + c 2 e 2t. To find a particular solution, we assume a solution looks similar to the complementary solution, only with functions which we need to determine instead of constants (hence the name, variation of parameters): Y (t) = µ i (t)y i (t) = µ (t)e 3t + µ 2 (t)e 2t. Now differentiate: Y (t) = µ (t)e 3t + 3µ (t)e 3t + µ 2(t)e 2t + 2µ 2 (t)e 2t = 3µ (t)e 3t + 2µ 2 (t)e 2t. where we have introduced the condition: µ (t)e 3t + µ 2(t)e 2t = 0. () Differentiate again: Y (t) = 3µ (t)e 3t + 2µ 2(t)e 2t + 9µ (t)e 3t + 4µ 2 (t)e 2t.
2 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page 2 y 5y + 6y = 2e t 3µ (t)e 3t + 2µ 2(t)e 2t + 9µ (t)e 3t + 4µ 2 (t)e 2t 5(3µ (t)e 3t + 2µ 2 (t)e 2t ) + 6(µ (t)e 3t + µ 2 (t)e 2t ) = 2e t 3µ (t)e 3t + 2µ 2(t)e 2t = 2e t (2) All the terms without derivatives of the µ i (t) should drop out at this stage; if they don t check your work! We have the two equations (Eq. (??) and (??)) in two unknowns: µ (t)e 3t + µ 2(t)e 2t = 0 3µ (t)e 3t + 2µ 2(t)e 2t = 2e t Solve using Cramer s rule: 0 e 2t µ 2e t 2e 2t (t) = e 3t e 2t 3e 3t 2e 2t = 2e3t e 5t = +2e 2t, so we can solve this differential equation for µ (t): µ (t) = 2e 2t dµ (t) = 2 e 2t dt µ (t) = e 2t + k = e 2t set the constant to zero since we are interested in any particular solution Similarly, for µ 2 (t) we find: e 3t 0 µ 3e 3t 2e t 2(t) = e 3t e 2t 3e 3t 2e 2t = 2e4t e 5t = 2e t, so we can solve this differential equation for µ 2(t): µ 2(t) = 2e t dµ 2 (t) = 2 e t dt µ 2 (t) = 2e t + k 2 = 2e t set the constant to zero since we are interested in any particular solution A particular solution is therefore: y p (t) = µ (t)e 3t + µ 2 (t)e 2t = e 2t e 3t + 2e t e 2t = e t. We can use the method of undetermined coefficients to check, since the form of g(t) = 2e t is one of our special forms. Initially, assume a solution of the original differential equation is Y (t) = Ae t, since g(t) is an exponential. There is no overlap with y c (t), so this will be a solution of the nonhomogeneous equation. All we need to do is substitute it in and determine the value of the constants A and B. Y (t) = Ae t Y (t) = Ae t Y (t) = Ae t
3 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page 3 Substitute into the differential equation y 5y + 6y = 2e t Ae t 5Ae t + 6Ae t = 2e t 2A = 2 A = A particular solution is therefore y p (t) = Y (t) = Ae t = e t, which verifies what we found using variation of parameters. Example (3.6.4) Find a particular solution of the differential equation 4y 4y + y = 6e t/2. Check your answer using This is a nonhomogeneous constant coefficient equation. We first solve the associated homogeneous differential equation: 4y 4y + y = 0. Since this is a constant coefficient differential equation, we assume the solution looks like y = e rt. Then: y = e rt, y = re rt, y = r 2 e rt. 4y 4y + y = 0 (4r 2 4r + )e rt = 0 4r 2 4r + = 0 characteristic equation (2r )(2r ) = 0 The root of the characteristic equation is r = /2 of multiplicity two. A fundamental set of solutions to the associated homogeneous equation is y (t) = e t/2 and y 2 (t) = te t/2. The complementary solution is therefore y c (t) = c i y i (t) = c e t/2 + c 2 te t/2. To find a particular solution, we assume a solution looks similar to the complementary solution, only with functions which we need to determine instead of constants: Y (t) = µ i (t)y i (t) = µ (t)e t/2 + µ 2 (t)te t/2. Now differentiate: Y (t) = µ (t)e t/2 + µ 2(t)te t/2 + 2 µ (t)e t/2 + µ 2 (t) where we have introduced the condition: ( ) 2 tet/2 + e t/2 = ( ) 2 µ (t)e t/2 + µ 2 (t) 2 tet/2 + e t/2 µ (t)e t/2 + µ 2(t)te t/2 = 0. (3) Differentiate again: Y (t) = 2 µ (t)e t/2 + µ 2(t) ( ) 2 tet/2 + e t/2 + ( ) 4 µ (t)e t/2 + µ 2 (t) 4 tet/2 + e t/2.
4 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page 4 [ 4 2 µ (t)e t/2 + µ 2(t) 4 ( ) 2 tet/2 + e t/2 [ 2 µ (t)e t/2 + µ 2 (t) + ( 4 µ (t)e t/2 + µ 2 (t) )] ( 2 tet/2 + e t/2 4y 4y + y )] = 6e t/2 4 tet/2 + e t/2 [ + µ (t)e t/2 + µ 2 (t)te t/2] = 6e t/2 2e t/2 µ + 4(e t/2 + t 2 et/2 )µ 2 = 6e t/2 (4) All the terms without derivatives of the µ i (t) should drop out at this stage; and they did! This is a good indication that our calculations are correct so far. We have the two equations (Eq. (??) and (??)) in two unknowns: µ (t) + tµ 2(t) = 0 2µ (t) + (4 + 2t)µ 2(t) = 6 Solve using Cramer s rule: 0 t µ t (t) = t t = 6t 4 = 4t, so we can solve this differential equation for µ (t): µ (t) = 4t dµ (t) = 4 t dt µ (t) = 2t 2 + k = 2t 2 set the constant to zero since we are interested in any particular solution Similarly, for µ 2 (t) we find: 0 µ 2 6 2(t) = t = 6 4 = 4, t so we can solve this differential equation for µ 2(t): µ 2(t) = 4 dµ 2 (t) = 4 dt µ 2 (t) = 4t + k 2 = 4t set the constant to zero since we are interested in any particular solution A particular solution is therefore: y p (t) = µ (t)e t/2 + µ 2 (t)te t/2 = 2t 2 e t/2 + 4tte t/2 = 2t 2 e t/2. We can use the method of undetermined coefficients to check, since the form of g(t) = 6e t2 /2 is one of our special forms. I leave this to you. Example (3.6.3) Verify that y (t) = t 2 and y 2 (t) = t are solutions of the corresponding homogeneous differential equation for t 2 y 2y = 3t 2 for t > 0. Then find a particular solution of the nonhomogeneous differential equation. This is a nonhomogeneous variable coefficient equation. We will learn how to solve variable coefficient differential equations using series solutions in Chapter 5. All we need to do is verify that the given functions are solutions.
5 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page 5 Substitute y into the differential equation: y = t 2 y = 2t y = 2 t 2 y 2y = t 2 (2) 2(t 2 ) = 0 (5) Therefore, y solves the associated homogeneous differential equation. Substitute y 2 into the differential equation: y 2 = t y 2 = t 2 y 2 = 2t 3 t 2 y 2y = t 2 (2t 3 ) 2(t ) = 0 (6) Therefore, y 2 solves the associated homogeneous differential equation. The complementary solution is therefore y c (t) = c i y i (t) = c t 2 + c 2 t. To find a particular solution, we assume a solution looks similar to the complementary solution, only with functions which we need to determine instead of constants: Y (t) = µ i (t)y i (t) = µ (t)t 2 + µ 2 (t)t. Now differentiate: Y (t) = µ (t)t 2 + µ 2(t)t + 2µ (t)t µ 2 (t)t 2 = 2µ (t)t µ 2 (t)t 2 where we have introduced the condition: µ (t)t 2 + µ 2(t)t = 0. (7) Differentiate again: Y (t) = 2µ (t)t µ 2(t)t 2 + 2µ (t) + 2µ 2 (t)t 3 t 2 y 2y = 3t 2 t 2 [ 2µ (t)t µ 2(t)t 2 + 2µ (t) + 2µ 2 (t)t 3] 2 [ µ (t)t 2 + µ 2 (t)t ] = 3t 2 2t 3 µ µ 2 = 3t 2 (8) We have the two equations (Eq. (??) and (??)) in two unknowns: 2t 3 µ µ 2 = 3t 2 µ (t)t 2 + µ 2(t)t = 0
6 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Variation of Parameters Page 6 Solve using Cramer s rule: 3t2 µ 0 t (t) = 2t3 t 2 t = 3t t 2t 2 + t 2 = t 3 t 3, so we can solve this differential equation for µ (t): µ (t) = t 3 t 3 dµ (t) = (t 3 ) t 3 dt µ (t) = ln t + t k = ln t + t 2 6 Where we set the constant k to zero since we are interested in any particular solution and there is no absolute value in logarithm since x > 0. Similarly, for µ 2 (t) we find: 2t3 3t 2 µ t 2 0 2(t) = 2t3 t 2 t = 3t4 + t 2 2t 2 + t 2 = t 2 + 3, so we can solve this differential equation for µ 2(t): µ 2(t) = t 2 + ( 3 dµ 2 (t) = t 2 + ) dt 3 µ 2 (t) = t3 3 + t 3 + k 2 = t3 3 + t 3 A particular solution is therefore: ) ( y p (t) = µ (t)t 2 + µ 2 (t)t = (ln t + t 2 t 2 + t t ) t = t 2 ln t t2 3. Note that t 2 /3 = cy (t) is actually a solution of the homogeneous equation. A simpler particular solution is therefore y p (t) = t 2 ln t + 2. We could use the method of undetermined coefficients to check, since the form of g(t) = 3t 2 is one of our special forms.
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