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Chapter 7: Linear Equations with Constant Coefficients
Introduction
* Several methods for solving differential equations with constant coefficients are presented in this book. A classical technique is treated in this and the next chapter. Chapters 14 and 15 contain a development of the Laplace transform and its use in solving linear differential equations. Each method has its advantages and disadvantages. Each is theoretically sufficient: all are necessary for maximum efficiency.
I. The Auxiliary Equation: Distinct Roots
1. Solve the equation
d3ydx3-4d2ydx2+dydx+6y=0
First write the auxiliary equation
m3-4m2+m+6=0
Whose roots m = 1, 2, 3 may be obtained by synthetic division. Then the general solution is seen to be
y= c1c1e-x+c2e2x+c3e3x
2. Solve the equation
3D3+5D2-2D)y=0
The auxiliary equation is
3m3+5m2-2m=0
And its roots are m = 0, -2, 1/3. By using the fact that e0x=1, the desired solution may be written
Y=c1+c2e-2x+c3exp13x
3. Solve the equation
d2xdt2-4=0
With the conditions that when t=0, x=0 and dx/dt=3.
The auxiliary equation is
m2 4 D 0;
With roots m D 2; 2. Hence the general solution of the differential equation is
x D c1 e2tC c2e2t:
It remains to enforce the conditions at t D 0. Now
dxdtD 2c1e2t 2c2e2t:
Thus the condition that x D 0 when t D 0 requires that
0 D c1 C c2;
And the condition that dx=dt D 3 when t D 0 requires that
3 D 2c1 2c2;
From the simultaneous equations for c1 and c2 we conclude that c1 D 34 and c2 D 34 Therefore,
X D 34.e2t e2t/;
Which can also be put in the form
x D 32sinh .2t ;/
Practice Set
1. .D2C 2D 3/y D 0: 11. d3xdt3Cd2xdt2 2dxdt D 0:
2. .D2C2DyD0: 12. . d3xdt319dxdt C 30x D 0:
3. .D2C D 6/y D 0: 13. .9D3 7D C 2/y D 0:
4. .D2 5DC6yD 0: 14. .4D3 21D 10/y D 0:
5. . D3C 3D2 4DyD 0: 15. .D3 14D C 8/y D 0:
6. . D3 3D2 10DyD 0: 16. .D3 D2 4D 2/y D 0:
7. . D3C6D2 C 11 D C 6/y D 0: 17. .4D4 8D3 7D2 C 11D C 6/y D 0:
8. .D3 C 3D2 4D 12/y D 0:...