1 First-order Odes 2 Second-order Linear Odes 3 Higher Order Linear Odes 4 Systems Of Odes. Phase Plane. Qualitative Methods 5 Series Solutions Of Odes. Special Functions 6 Laplace Transforms 7 Linear Algebra: Matrices, Vectors, Determinants. Linear Systems 8 Linear Algebra: Matrix Eigenvalue Problems 9 Vector Differential Calculus. Grad, Div, Curl 10 Vector Integral Calculus. Integral Theorems 11 Fourier Analysis. Partial Differential Equations (pdes) 12 Partial Differential Equations (pdes) 13 Complex Numbers And Functions 14 Complex Integration 15 Power Series, Taylor Series 16 Laurent Series. Residue Integration 17 Conformal Mapping 18 Complex Analysis And Potential Theory 19 Numerics In General 20 Numeric Linear Algebra 21 Numerics For Odes And Pdes 22 Unconstrauined Optimization. Linear Programming 23 Graphs. Combinatorial Optimization 24 Data Analysis. Probability Theory 25 Mathematical Statistics Chapter2: Second-order Linear Odes
2.1 Homogeneous Linear Odes Of Second Order 2.2 Homogeneous Linear Odes With Constant Coefficients 2.3 Differential Operators 2.4 Modeling Of Free Oscillators Of A Mass-spring System 2.5 Euler-cauchy Equations 2.6 Existence And Uniqueness Of Solutions. Wronskian 2.7 Nonhomogeneous Odes 2.8 Modeling: Forced Oscillations. Resonance 2.9 Modeling: Electric Circuits 2.10 Solution By Variation Of Parameters Chapter Questions Section: Chapter Questions
Problem 1RQ Problem 2RQ Problem 3RQ: By what methods can you get a general solution of a nonhomogeneous ODE from a general solution of a... Problem 4RQ Problem 5RQ Problem 6RQ Problem 7RQ: Find a general solution. Show the details of your calculation.
4y″ + 32y′ + 63y = 0
Problem 8RQ: Find a general solution. Show the details of your calculation.
y″ + y′ − 12y = 0
Problem 9RQ: Find a general solution. Show the details of your calculation.
y″ + 6y′ + 34y = 0
Problem 10RQ: Find a general solution. Show the details of your calculation.
y″ + 0.20y′ + 0.17y = 0
Problem 11RQ: Find a general solution. Show the details of your calculation.
(100D2 − 160D + 64I)y = 0
Problem 12RQ: Find a general solution. Show the details of your calculation.
(D2 + 4πD + 4π2I)y = 0
Problem 13RQ: Find a general solution. Show the details of your calculation.
(x2D2 + 2xD − 12I)y = 0
Problem 14RQ: Find a general solution. Show the details of your calculation.
(x2D2 + xD − 9I)y = 0
Problem 15RQ Problem 16RQ Problem 17RQ Problem 18RQ: Find a general solution. Show the details of your calculation.
yy″ = 2y′2
Problem 19RQ: Solve the problem, showing the details of your work. Sketch or graph the solution.
y″ + 16y =... Problem 20RQ: Solve the problem, showing the details of your work. Sketch or graph the solution.
y″ − 3y′ + 2y =... Problem 21RQ: Solve the problem, showing the details of your work. Sketch or graph the solution.
(x2D2 + xD − I)y... Problem 22RQ: Solve the problem, showing the details of your work. Sketch or graph the solution.
(x2D2 + 15xD +... Problem 23RQ: Find the steady-state current in the RLC-circuit in Fig. 71 when R = 2Ω (2000 Ω), L = 1 H, C = 4 ·... Problem 24RQ: Find a general solution of the homogeneous linear ODE corresponding to the ODE in Prob. 23.
25. Find... Problem 25RQ: Find the steady-state current in the RLC-circuit in Fig. 71 when R = 50 Ω, L = 30 H, C = 0.025 F, E... Problem 26RQ: Find the current in the RLC-circuit in Fig. 71 when R = 40 Ω, L = 0.4 H, C = 10−4 F, E = 220 sin... Problem 27RQ Problem 28RQ Problem 29RQ Problem 30RQ Problem 1RQ
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Question 3: Summarize how to find the limits of integration when integrating in order dr dθ. We will typically integrate in this order.
Hint 1: Read the subsection “Finding Limits of Integration” (p. 916 – 917).
Transcribed Image Text: rsin - y=√/2
or
r=√√/2csc 0
2
2
√₂
Leaves at r = 2
L
R
R
Enters at r
(b)
Largest 0 is
L
√2 csc 0
Smallest is.
>X
FIGURE 15.24 Finding the limits of
integration in polar coordinates.
A version of Fubini's Theorem says that the limit approached by these sums can be evalu-
ated by repeated single integrations with respect to r and as
8-B pr-gy(0)
f(r, 0)r dr do.
[[
f(r, 9) dA =
Finding Limits of Integration
The procedure for finding limits of integration in rectangular coordinates also works for
polar coordinates. We illustrate this using the region R shown in Figure 15.24. To evaluate
f(r, 0) dA in polar coordinates, integrating first with respect to r and then with respect
to 0, take the following steps.
1. Sketch. Sketch the region and label the bounding curves (Figure 15.24a).
2. Find the r-limits of integration. Imagine a ray L. from the origin cutting through R in the
direction of increasing r. Mark the r-values where L enters and leaves R. These are the
r-limits of integration. They usually depend on the angle that L makes with the posi-
tive x-axis (Figure 15.24b).
3. Find the 0-limits of integration. Find the smallest and largest 9-values that bound R.
These are the 0-limits of integration (Figure 15.24c). The polar iterated integral is
8/2
[[ f(r. 0 ) dA =
A =
6/4 Jr=√₂ csc 9
f(r, 0) r dr d0.
EXAMPLE 1 Find the limits of integration for integrating f(r, 8) over the region R
that lies inside the cardioid r = 1 + cos 0 and outside the circle r = 1.
Solution
1. We first sketch the region and label the bounding curves (Figure 15.25).
2. Next we find the r-limits of integration. A typical ray from the origin enters R where
r = 1 and leaves where r = 1 + cos 0.
Transcribed Image Text: Enters
at
r=1
r=1+cos 0
2
Enters at
7 = 0
Leaves at
r = 1 + cos
FIGURE 15.25 Finding the limits of
integration in polar coordinates for the
region in Example 1.
Area Differential in Polar Coordinates
dA = r dr do
Leaves at
r=V/4 cos 26
X
²-4 cos 20
FIGURE 15.26 To integrate over
the shaded region, we run from 0 to
√4 cos 20 and 6 from 0 to 7/4
(Example 2).
3. Finally we find the 0-limits of integration. The rays from the origin that intersect & run
from 0 = -7/2 to 0 = 7/2. The integral is
•/2 pl+c88
f(r, 0) r dr do.
If f(r, 0) is the constant function whose value is 1, then the integral of f over R is the
area of R.
Area in Polar Coordinates
The area of a closed and bounded region R in the polar coordinate plane is
15.4 Double Integrals in Polar Form 917
A = 4
- If
= 4
A =
This formula for area is consistent with all earlier formulas.
EXAMPLE 2
Find the area enclosed by the lemniscate 2² = 4 cos 20.
Solution We graph the lemniscate to determine the limits of integration (Figure 15.26) and
see from the symmetry of the region that the total area is 4 times the first-quadrant portion.
#/4 V4 cos 26
#/4
r=V/4 con 28
" r dr do = 4
-4.****
do
r dr do.
/4
2 cos 20 d0 - 4 sin 20
1/4
Jo
= 4.
Changing Cartesian Integrals into Polar Integrals
The procedure for changing a Cartesian integral f(x, y) dx dy into a polar integral has
two steps. First substitute x = r cos 8 and y = r sin 8, and replace dx dy by r dr do in the
Cartesian integral. Then supply polar limits of integration for the boundary of R. The Car-
tesian integral then becomes
With differentiation, one of the major concepts of calculus. Integration involves the calculation of an integral, which is useful to find many quantities such as areas, volumes, and displacement.
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