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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Laplace Transforms of Step Functions

    Bernd Schroder

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t)

    Original

    DE & IVP

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t)

    Original

    DE & IVP EL

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    T f d N F l A M d l Th I iti l V l P bl D bl Ch k

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t)

    Original

    DE & IVP

    Algebraic equation for

    the Laplace transformEL

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    T f d N F l A M d l Th I iti l V l P bl D bl Ch k

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t) Transform domain (s)

    Original

    DE & IVP

    Algebraic equation for

    the Laplace transformEL

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t) Transform domain (s)

    Original

    DE & IVP

    Algebraic equation for

    the Laplace transformEL

    Algebraic solution,

    partial fractions

    c

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t) Transform domain (s)

    Original

    DE & IVP

    Algebraic equation for

    the Laplace transform

    Laplace transform

    of the solution

    EL

    Algebraic solution,

    partial fractions

    c

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t) Transform domain (s)

    Original

    DE & IVP

    Algebraic equation for

    the Laplace transform

    Laplace transform

    of the solution

    E

    '

    L

    L1

    Algebraic solution,

    partial fractions

    c

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Everything Remains As It Was

    No matter what functions arise, the idea for solving differentialequations with Laplace transforms stays the same.

    Time Domain (t) Transform domain (s)

    Original

    DE & IVP

    Algebraic equation for

    the Laplace transform

    Laplace transform

    of the solutionSolution

    E

    '

    L

    L1

    Algebraic solution,

    partial fractions

    c

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    3. The function U(t

    a)

    U(t

    b) is equal to 1 on [a,b)

    and equal to zero outside [a,b).

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    3. The function U(t

    a)

    U(t

    b) is equal to 1 on [a,b)

    and equal to zero outside [a,b).

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    3. The function U(t

    a)

    U(t

    b) is equal to 1 on [a,b)

    and equal to zero outside [a,b).

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    3. The function U(t

    a)

    U(t

    b) is equal to 1 on [a,b)

    and equal to zero outside [a,b).4. The function f(t)U(ta)f(t)U(tb) is equal to f on

    [a,b) and equal to zero outside [a,b).

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    3. The function U(t

    a)

    U(t

    b) is equal to 1 on [a,b)

    and equal to zero outside [a,b).4. The function f(t)U(ta)f(t)U(tb) is equal to f on

    [a,b) and equal to zero outside [a,b).5. Lf(ta)U(ta)(s) = e

    asF(s).

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    The Unit Step Function

    1. U(t) =1; for t 0,0; for t< 0,

    2. The unit step function can be shifted and then used to

    model the switching on and off of another function.

    3. The function U(t

    a)

    U(t

    b) is equal to 1 on [a,b)

    and equal to zero outside [a,b).4. The function f(t)U(ta)f(t)U(tb) is equal to f on

    [a,b) and equal to zero outside [a,b).5. Lf(ta)U(ta)(s) = e

    asF(s).

    6. Keep the exponential separate when working in thetransform domain.

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    An Application Problem

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    An Application Problem(Dimensions fictitious.)

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    An Application Problem(Dimensions fictitious.)

    In an RC circuit with resistance R = 1 and capacitance

    C=1

    3F initially, the charge of the capacitor is 2C. At time

    t= 2 seconds, a sine shaped external voltage is activated. Attime t= 5 seconds, the external voltage is turned off.

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    An Application Problem(Dimensions fictitious.)

    In an RC circuit with resistance R = 1 and capacitance

    C=1

    3F initially, the charge of the capacitor is 2C. At time

    t= 2 seconds, a sine shaped external voltage is activated. Attime t= 5 seconds, the external voltage is turned off. Find thecharge of the capacitor as a function of time.

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    d

    d

    ERI

    '

    E(t) = Rq +1

    Cq

    q

    C

    f

    ff

    f

    ff

    f

    ff

    f

    ff

    E(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations Ry

    +

    1

    Cy = E(t),

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations Ry

    +

    1

    Cy = E(t), y

    + 3y = E(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations Ry +

    1

    Cy = E(t), y

    + 3y = E(t)

    y(0) = 2

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations Ry +

    1

    Cy = E(t), y

    + 3y = E(t)

    y(0) = 2 E(t) is sin(t), activated at t= 2 and deactivated at t= 5.

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations Ry +

    1

    Cy = E(t), y

    + 3y = E(t)

    y(0) = 2 E(t) is sin(t), activated at t= 2 and deactivated at t= 5. E(t) = sin(t)U(t2)

    Bernd Schroder Louisiana Tech University, College of Engineering and ScienceLaplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Underlying Equations Ry +

    1

    Cy = E(t), y

    + 3y = E(t)

    y(0) = 2 E(t) is sin(t), activated at t= 2 and deactivated at t= 5. E(t) = sin(t)U(t2) sin(t)U(t5)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    sin(t)U(t

    2)

    sin(t)U(t

    5)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    sin(t)U(t

    2)

    sin(t)U(t

    5)

    = sin(t2+ 2)U(t2) sin(t5+ 5)U(t5)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    sin(t)U(t

    2)

    sin(t)U(t

    5)

    = sin

    (t2) + 2U(t2) sin(t5+ 5)U(t5)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    sin(t)U(t

    2)

    sin(t)U(t

    5)

    = sin

    (t2) + 2U(t2) sin(t5) + 5U(t5)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    sin(t)U(t

    2)

    sin(t)U(t

    5)

    = sin

    (t2) + 2U(t2) sin(t5) + 5U(t5)= sin(t2)U(t2)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

  • 7/29/2019 Laplace_transform_step_fun

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    logo1

    Solve the Initial Value Problem

    y + 3y = sin(t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.Adjusting the right side.

    sin(t)U(t

    2)

    sin(t)U(t

    5)

    = sin

    (t2) + 2U(t2) sin(t5) + 5U(t5)= sin(t2)U(t2) + sin(t5)U(t5)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y + 3

    y= sin(

    t)U

    (t2

    ) sin(t)U

    (t5

    ),y(0) = 2.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y +

    3y=

    sin(t)U

    (t

    2)

    sin(t)U

    (t

    5)

    ,

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y +

    3y=

    sin(t)U

    (t

    2)

    sin(t)U

    (t

    5)

    ,

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y +

    3y=

    sin(t)U

    (t

    2)

    sin(t)U

    (t

    5)

    ,

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2 + 3Y

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y+ 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2 + 3Y = e2s 1s2 + 1

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y+ 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2 + 3Y = e2s 1s2 + 1

    + e5s 1s2 + 1

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

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    logo1

    Solve the Initial Value Problem

    y+ 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2 + 3Y = e2s 1s2 + 1

    + e5s 1s2 + 1

    (s+ 3)Y2 = e2s 1s2 + 1

    + e5s1

    s2 + 1

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    S l h I i i l V l P bl

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    logo1

    Solve the Initial Value Problem

    y+ 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2 + 3Y = e2s 1s2 + 1

    + e5s 1s2 + 1

    (s+ 3)Y2 = e2s 1s2 + 1

    + e5s1

    s2 + 1

    (s+ 3)Y = e2

    s

    1

    s2 + 1 + e5

    s

    1

    s2 + 1 + 2

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    S l h I i i l V l P bl

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    logo1

    Solve the Initial Value Problem

    y+ 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.y + 3y = sin(t2)U(t2) + sin(t5)U(t5),

    y(0) = 2

    sY2 + 3Y = e2s 1s2 + 1

    + e5s 1s2 + 1

    (s+ 3)Y2 = e2s 1s2 + 1

    + e5s1

    s2 + 1

    (s+ 3)Y = e2

    s

    1

    s2 + 1 + e5

    s

    1

    s2 + 1 + 2

    Y = e2s1

    (s2+1) (s+3)+ e5s

    1

    (s2+1) (s+3)+

    2

    s+3

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    P ti l F ti D iti

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    Partial Fraction Decomposition.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    P ti l F ti D iti

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 :

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 :

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition.

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    s = 1 :

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition.

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    s = 1 : 1 = A+ 3104 + 1

    10 2

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition.

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    logo1

    Partial Fraction Decomposition.

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    s = 1 : 1 = A+ 3104 + 1

    10 2, A =

    1

    10

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition.

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    logo1

    p

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    s = 1 : 1 = A+ 3104 + 1

    10 2, A =

    1

    101

    (s2 + 1) (s+ 3)=

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition.

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    logo1

    p

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    s = 1 : 1 = A+ 3104 + 1

    10 2, A =

    1

    101

    (s2 + 1) (s+ 3)=

    1

    10

    s+ 3s2 + 1

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Partial Fraction Decomposition.

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    logo1

    p

    1(s2 + 1) (s+ 3)

    = As+Bs2 + 1

    + Cs+ 3

    1 = (As+B)(s+ 3) +Cs2 + 1

    s = 3 : 1 = 10C, C=1

    10

    s = 0 : 1 = 3B+1

    10, B =

    3

    10

    s = 1 : 1 = A+ 3104 + 1

    10 2, A =

    1

    101

    (s2 + 1) (s+ 3)=

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    g p

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    g p

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s ss2 + 1

    + 3 1s2 + 1

    + 1s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s ss2 + 1

    + 3 1s2 + 1

    + 1s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    y = 110

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s s

    s2 + 1+ 3 1

    s2 + 1+ 1

    s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    y = 110U(t2)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s s

    s2 + 1+ 3 1

    s2 + 1+ 1

    s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    y = 110U(t2)

    cos(t) + 3sin(t) + e3t

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s s

    s2 + 1+ 3 1

    s2 + 1+ 1

    s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    y = 110U(t2)

    cos(t) + 3sin(t) + e3t

    tt2

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s s

    s2 + 1+ 3 1

    s2 + 1+ 1

    s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    y = 110U(t2)

    cos(t) + 3sin(t) + e3t

    tt2

    +1

    10U(t5)

    cos(t) + 3sin(t) + e3t

    tt5

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Inverting the Laplace transform.

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    logo1

    Y = e2s

    110s+ 3s2 + 1

    + 110

    1s+ 3

    +e5s

    1

    10

    s+ 3s2 + 1

    +1

    10

    1

    s+ 3

    +

    2

    s+ 3

    = 110

    e2s s

    s2 + 1+ 3 1

    s2 + 1+ 1

    s+ 3

    +

    1

    10e5s

    ss2 + 1

    + 31

    s2 + 1+

    1

    s+ 3

    + 2

    1

    s+ 3

    y = 110U(t2)cos(t) + 3sin(t) + e3t tt2

    +1

    10U(t5)

    cos(t) + 3sin(t) + e3t

    tt5

    + 2e3t

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Solve the Initial Value Problem

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    logo1

    y + 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.

    y =1

    10U(t2)cos(t) + 3sin(t) + e

    3t

    tt2+

    1

    10U(t5)

    cos(t) + 3sin(t) + e3t

    tt5

    + 2e3t

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Solve the Initial Value Problem

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    logo1

    y + 3y = sin(t)U(t

    2)

    sin(t)U(t

    5),

    y(0) = 2.

    y =1

    10U(t2)cos(t) + 3sin(t) + e

    3t

    tt2+

    1

    10U(t5)

    cos(t) + 3sin(t) + e3t

    tt5

    + 2e3t

    =1

    10U(t2)

    cos(t) + 3sin(t) + e3(t2)

    + 1

    10U(t5)

    cos(t)3sin(t) + e3(t5)

    + 2e3t

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    y =1

    10U(t2)

    cos(t) + 3sin(t) + e3(t2)

    1 3(t 5 ) 3t

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    logo1

    +1

    10U(t5)cos(t)3sin(t) + e

    3(t5)

    + 2e3t

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    y = 110U(t2)cos(t) + 3sin(t) + e3(t2)

    +1

    10U(t5)

    cos(t)3sin(t) + e3(t5)

    + 2e3t

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions

    Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    y = 110U(t2)cos(t) + 3sin(t) + e3(t2)

    +1

    10U(t5)

    cos(t)3sin(t) + e3(t5)

    + 2e3t

    Initial value: By inspection. The function y = e3t solves the differential equationy + 3y = 0.

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    y = 110U(t2)cos(t) + 3sin(t) + e3(t2)

    +1

    10U(t5)

    cos(t)3sin(t) + e3(t5)

    + 2e3t

    Initial value: By inspection. The function y = e3t solves the differential equationy + 3y = 0.

    So all exponential terms in the solution are o.k., provided

    that the rest, which is1

    10

    U(t2)U(t5)

    cos(t) + 3sin(t)

    produces a sine function that only exists on [2,5).

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    1

    10 cos(t) + 3sin(t) + 3 110 cos(t) + 3sin(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    1

    10 cos(t) + 3sin(t) + 3 110 cos(t) + 3sin(t)

    =1

    10

    sin(t) + 3cos(t)

    + 3

    1

    10

    cos(t) + 3sin(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    1

    10 cos(t) + 3sin(t) + 3 110 cos(t) + 3sin(t)

    =1

    10

    sin(t) + 3cos(t)

    + 3

    1

    10

    cos(t) + 3sin(t)

    =

    1

    10 (33) cos(t) +1

    10 (1 + 9) sin(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    1

    10 cos(t) + 3sin(t) + 3 110 cos(t) + 3sin(t)

    =1

    10

    sin(t) + 3cos(t)

    + 3

    1

    10

    cos(t) + 3sin(t)

    =

    1

    10 (33) cos(t) +1

    10 (1 + 9) sin(t)= sin(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions Transforms and New Formulas A Model The Initial Value Problem Double Check

    Checking the Solution.

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    logo1

    1

    10 cos(t) + 3sin(t) + 3 110 cos(t) + 3sin(t)

    =1

    10

    sin(t) + 3cos(t)

    + 3

    1

    10

    cos(t) + 3sin(t)

    =

    1

    10 (33) cos(t) +1

    10 (1 + 9) sin(t)= sin(t)

    Bernd Schroder Louisiana Tech University, College of Engineering and Science

    Laplace Transforms of Step Functions