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The power of the Laplace transform is derived from the fact that there is a one-to-one correspondence between f (t) and L { f (t )}. This means that if L { f (t )} is known, then f (t) is uniquely determined. If F (s) = L { f (t )}, then f (t ) = L 1 { F (s)}. L 1 is called the inverse Laplace transform.

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fx 3x2 3 0 when x 1; fy 3y2 12 0 when y 2. Then critical points are P 1; 2 , Q 1; 2 ; R 1; 2 ; S 1; 2 . 2 fxx 6x; fyy 6y; fxy 0. Then fxx fyy fxy 36xy. At P 1; 2 ; > 0 and fxx (or fyy > 0; hence P is a relative minimum point. At Q 1; 2 ; < 0 and Q is neither a relative maximum or minimum point. At R 1; 2 ; < 0 and R is neither a relative maximum or minimum point. At S 1; 2 ; > 0 and fxx (or fyy < 0 so S is a relative maximum point. Thus, the relative minimum value of f x; y occurring at P is 2, while the relative maximum value occurring at S is 38. Points Q and R are saddle points.

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InverseLaplaceTransform[F[var1], var1, var2] computes the inverse Laplace transform of the function F, with independent variable var1, and expresses it as a function of var2.

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InverseLaplaceTransform 1 , s, t s 3 3t InverseLaplaceTransform 31 , s, t s 8 1 t 3 t Cos[ 3 t] 3 Sin [ 3 t] 12

Traditionally, one would factor the denominator, expand into partial fractions, and find the inverse transformation separately for each term. Mathematica does it all automatically.

8.23. A rectangular box, open at the top, is to have a volume of 32 cubic feet. dimensions so that the total surface is a minimum

The next example illustrates how the Laplace transform can be used to solve a simple differential equation.

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d2y dy 3 + 2 y = t 2 , y '(0) = 1, y(0) = 2 . First we compute the dt dt 2 Laplace transform of both sides of the equation. This can be done in one step.

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equation = y''[t] 3 y'[t]+ 2 y[t] t2; temp = LaplaceTransform[equation, t, s] 2 LaplaceTransform[y[t], t, s]+ s2 LaplaceTransform[y[t], t, s] 3(s LaplaceTransform[y[t], t, s] y[0]) s y[0] y'[0] 2 s3 Then we solve for the Laplace transform satisfying the given initial conditions. temp2 = Solve[temp, LaplaceTransform[y[t], t, s]] /. {y'[0] 1, y[0] 2}

If x, y and z are the edges (see Fig. 8-7), then 1 2 Volume of box V xyz 32 Surface area of box S xy 2yz 2xz

3 4 LaplaceTransform[y[t], t, s] 2 5 s + 2 s 2 s3 (2 3 s + s )

Next we extract the transform as a function of s. temp3 = temp2[[1, 1, 2]] 2 5 s3 + 2 s4 s3 (2 3 s + s2) Finally, we compute the inverse Laplace transform to get the solution of the equation. InverseLaplaceTransform[temp3, s, t] 1 (7 + 4 t 3 2t + 6 t + 2 t2 ) 4

or, since z 32=xy from (1), S xy 64 64 x y Fig. 8-7

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