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MCS,PHD
Argosy University/ Phoniex University/
Nov-2005 - Oct-2011
Professor
Phoniex University
Oct-2001 - Nov-2016
2.39Â Given the following system of equations
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16s + 32u + 33p + 13w = 91 5s + 11u + 10p + 8w = 16
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9s + 7u + 6p + 12w = 5 34s + 14u + 15p + w = 43
Â
determine the values of s, u, p, and w, the value of the determinant, and the inverse of the coefficients of s, u, p, and w (Answer: s = - 0.1258, u = - 8.7133, p = 11.2875, and
w = - 0.0500. Determinant = 7,680).
Â
              Consider two long cylinders of two different materials where one cylinder just fits inside the other. The inner radius of the inner cylinder is a, and its outer radius is b. The inner radius of the outer cylinder is also b, and its outer radius is c. The Young’s modu-lus and Poisson ratio of the inner cylinder are E1 and n1, respectively, and those of the outer cylinder are E2 and n2, respectively. The radial stress srr, hoop stress suu, and radi-al displacement ur are given, respectively, by,
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srri(r) = |
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Ai |
+ Bi |
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r |
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suui(r) = |
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- Ai |
+ Bi |
i = 1, 2 |
(a) |
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r2 |
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uri(r) = |
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Ai + |
(1 - yi) |
rBi |
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rEi |
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Ei |
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where i = 1 refers to the inner cylinder and i = 2 to the outer cylinder.
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    Szabo, Linear Algebra, p. 265.
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     Ibid., p. 266.
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If the outer surface of the outer cylinder is subjected to a compressive radial dis-placement Uo and the inner surface of the inner cylinder has no radial stress, then the following four boundary conditions can be used to determine Ai and Bi, i = 1, 2:
srr1(a) = 0
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srr1(b) = srr2(b) (b) ur1(b) = ur2(b)
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ur2(c) = - Uo
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Substituting Eqs. (a) into (b), the following system of equations in matrix form is obtained:
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Â
         1
1
  (1 + n1) 0
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Â
Â
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a2 |
0 |
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0 |
T d |
A1 |
t |
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d |
0 |
t |
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b2 |
- 1 |
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- b2 |
B1 |
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0 |
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(1 - n1)b2 |
(1 + n2)E1/E2 |
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(1 - n2)b2E1/E2 |
A2 |
0 |
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- (1 + n2) |
(1 - n2)c2 |
B2 |
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- UoE2c |
Â
Determine the hoop stress in the inner and outer cylinders at r = b when n1 = n2 = 0.4, E1 = 2.1 * 109 N/m2, E2 = 0.21 * 109 N/m2, Uo = 0.25 mm, a = 5 mm, b = 6.4 mm, and c = 8 mm (Answer: suu1(b) = - 6.301 * 107 N/m2 and suu2(b) =
  1.179 * 107 N/m2)
Â
              For the electric circuit shown in Figure 2.10, the governing equations for the three loop currents are given by
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V1 - 6Ri1Â + 4R(i2 - i1) = 0
V2Â + 2R(i3 - i2) - 3Ri2 - 4R(i2 - i1) = 0
- V3 - Ri3 - 2R(i3 - i2) = 0
Use solve from Symbolic toolbox to show that the three currents are given by
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i1Â = |
1 |
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(12V2 - 8V3Â + 23V1) |
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182R |
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i2Â = |
1 |
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(6V1Â + 15V2Â - 10V3) |
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91R |
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i3Â = |
1 |
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(4V1Â + 10V2Â - 37V3) |
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91R |
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i2 |
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6R |
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i1 |
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4R |
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i3 |
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2R |
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3R |
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Figure 2.10Â Electric circuit. |
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Â
Â
              An ac electric circuit with resistors R and capacitances C is described by the following set of equations in the Laplace transformed domain:
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C |
2s + to |
- s |
0 |
S c |
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1(s) |
s = |
c |
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s |
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sU |
(s) |
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s + to |
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- s |
2s + to |
- s |
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V2(s) |
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0 |
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Â
where s is the Laplace transform parameter, to = 1/RC, Vj(s), j = 1, 2, 3, are the trans-formed nodal voltages, and Uj(s) is the transformed applied voltage. Use the Symbolic
toolbox to solve for Vj(s).
Â
Â
Â
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