 6.4.1: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.2: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.3: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.4: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.5: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.6: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.7: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.8: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.9: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.10: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.11: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.12: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.13: In each of 1 through 13: (a) Find the solution of the given initial...
 6.4.14: Find an expression involving uc(t) for a function f that ramps up f...
 6.4.15: Find an expression involving uc(t) for a function g that ramps up f...
 6.4.16: A certain springmass system satisfies the initial value problem u +...
 6.4.17: Modify the problem in Example 2 of this section by replacing the gi...
 6.4.18: Consider the initial value problem y + 1 3 y + 4y = fk(t), y(0) = 0...
 6.4.19: Resonance and Beats. In Section 3.8 we observed that an undamped ha...
 6.4.20: Resonance and Beats. In Section 3.8 we observed that an undamped ha...
 6.4.21: Resonance and Beats. In Section 3.8 we observed that an undamped ha...
 6.4.22: Resonance and Beats. In Section 3.8 we observed that an undamped ha...
 6.4.23: Resonance and Beats. In Section 3.8 we observed that an undamped ha...
Solutions for Chapter 6.4: Differential Equations with Discontinuous Forcing Functions
Full solutions for Elementary Differential Equations and Boundary Value Problems  9th Edition
ISBN: 9780470383346
Solutions for Chapter 6.4: Differential Equations with Discontinuous Forcing Functions
Get Full SolutionsSince 23 problems in chapter 6.4: Differential Equations with Discontinuous Forcing Functions have been answered, more than 13073 students have viewed full stepbystep solutions from this chapter. This expansive textbook survival guide covers the following chapters and their solutions. Elementary Differential Equations and Boundary Value Problems was written by and is associated to the ISBN: 9780470383346. This textbook survival guide was created for the textbook: Elementary Differential Equations and Boundary Value Problems, edition: 9. Chapter 6.4: Differential Equations with Discontinuous Forcing Functions includes 23 full stepbystep solutions.

Affine transformation
Tv = Av + Vo = linear transformation plus shift.

Column space C (A) =
space of all combinations of the columns of A.

Cross product u xv in R3:
Vector perpendicular to u and v, length Ilullllvlll sin el = area of parallelogram, u x v = "determinant" of [i j k; UI U2 U3; VI V2 V3].

Cyclic shift
S. Permutation with S21 = 1, S32 = 1, ... , finally SIn = 1. Its eigenvalues are the nth roots e2lrik/n of 1; eigenvectors are columns of the Fourier matrix F.

Free columns of A.
Columns without pivots; these are combinations of earlier columns.

Hypercube matrix pl.
Row n + 1 counts corners, edges, faces, ... of a cube in Rn.

Indefinite matrix.
A symmetric matrix with eigenvalues of both signs (+ and  ).

Kirchhoff's Laws.
Current Law: net current (in minus out) is zero at each node. Voltage Law: Potential differences (voltage drops) add to zero around any closed loop.

lAII = l/lAI and IATI = IAI.
The big formula for det(A) has a sum of n! terms, the cofactor formula uses determinants of size n  1, volume of box = I det( A) I.

Left inverse A+.
If A has full column rank n, then A+ = (AT A)I AT has A+ A = In.

Norm
IIA II. The ".e 2 norm" of A is the maximum ratio II Ax II/l1x II = O"max· Then II Ax II < IIAllllxll and IIABII < IIAIIIIBII and IIA + BII < IIAII + IIBII. Frobenius norm IIAII} = L La~. The.e 1 and.e oo norms are largest column and row sums of laij I.

Nullspace matrix N.
The columns of N are the n  r special solutions to As = O.

Reduced row echelon form R = rref(A).
Pivots = 1; zeros above and below pivots; the r nonzero rows of R give a basis for the row space of A.

Right inverse A+.
If A has full row rank m, then A+ = AT(AAT)l has AA+ = 1m.

Row picture of Ax = b.
Each equation gives a plane in Rn; the planes intersect at x.

Schur complement S, D  C A } B.
Appears in block elimination on [~ g ].

Singular matrix A.
A square matrix that has no inverse: det(A) = o.

Spanning set.
Combinations of VI, ... ,Vm fill the space. The columns of A span C (A)!

Trace of A
= sum of diagonal entries = sum of eigenvalues of A. Tr AB = Tr BA.

Tridiagonal matrix T: tij = 0 if Ii  j I > 1.
T 1 has rank 1 above and below diagonal.