HP 48gII User Manual

Page 497

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Page 16-19

The result is:

, i.e.,

h(t) = a/(k-1)

⋅e

-t

+((k-1)

⋅cC

o

-a)/(k-1)

⋅e

-kt

.

Thus, cC0 in the results from LDEC represents the initial condition h(0).
Note: When using the function LDEC to solve a linear ODE of order n in f(X),
the result will be given in terms of n constants cC0, cC1, cC2, …, cC(n-1),
representing the initial conditions f(0), f’(0), f”(0), …, f

(n-1)

(0).


Example 2 – Use Laplace transforms to solve the second-order linear equation,

d

2

y/dt

2

+2y = sin 3t.


Using Laplace transforms, we can write:

L{d

2

y/dt

2

+2y} = L{sin 3t},

L{d

2

y/dt

2

} + 2

⋅L{y(t)} = L{sin 3t}.


Note: ‘SIN(3*X)’ ` LAP µ produces ‘3/(X^2+9)’, i.e.,

L{sin 3t}=3/(s

2

+9).


With Y(s) = L{y(t)}, and L{d

2

y/dt

2

} = s

2

⋅Y(s) - s⋅y

o

– y

1

, where y

o

= h(0) and y

1

=

h’(0), the transformed equation is

s

2

⋅Y(s) – s⋅y

o

– y

1

+ 2

⋅Y(s) = 3/(s

2

+9).


Use the calculator to solve for Y(s), by writing:

‘X^2*Y-X*y0-y1+2*Y=3/(X^2+9)’

` ‘Y’ ISOL

The result is

‘Y=((X^2+9)*y1+(y0*X^3+9*y0*X+3))/(X^4+11*X^2+18)’.

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