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Lecture 5.2: Properties and applications of the Laplace transform Matthew Macauley Department of Mathematical Sciences Clemson University http://www.math.clemson.edu/~macaule/ Math 2080, Differential Equations M. Macauley (Clemson) Lecture


  1. Lecture 5.2: Properties and applications of the Laplace transform Matthew Macauley Department of Mathematical Sciences Clemson University http://www.math.clemson.edu/~macaule/ Math 2080, Differential Equations M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 1 / 7

  2. Laplace transform fundamentals Two key properties L is linear. L turns derivatives into multiplication. M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 2 / 7

  3. Useful shortcuts More properties Suppose we know F ( s ) = L{ f ( t ) } . Then: (i) L{ e at f ( t ) } = F ( s − a ); (ii) L{ tf ( t ) } = − F ′ ( s ); (iii) L{ t n f ( t ) } = ( − 1) n · d n ds n F ( s ). Examples (i) Compute the Laplace transform of f ( t ) = e 2 t cos 3 t . (ii) Compute the Laplace transform of f ( t ) = t 2 e 3 t . M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 3 / 7

  4. Using the Laplace transform to solve ODEs Example Sove the initial value problem y ′′ − y = e 2 t , y (0) = 0, y ′ (0) = 1. M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 4 / 7

  5. Inverse Laplace transforms Example Compute L − 1 � � 1 . s 2 +4 s +13 M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 5 / 7

  6. Comparison of old vs. new methods M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 6 / 7

  7. Structure of the solution to an ODE A generic example Consider an initial value problem ay ′′ + by ′ + cy = f ( t ), y (0) = x 0 , y ′ (0) = v 0 . M. Macauley (Clemson) Lecture 5.2: Properties & applications of L Differential Equations 7 / 7

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