Chapter 8: Q16E (page 426)
In the study of the vacuum tube, the following equation is encountered:
Find the Taylor polynomial of degree 4 approximating the solution with the initial values,.
Short Answer
The required polynomial is, .
Chapter 8: Q16E (page 426)
In the study of the vacuum tube, the following equation is encountered:
Find the Taylor polynomial of degree 4 approximating the solution with the initial values,.
The required polynomial is, .
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Get started for freeIn Problems 15-17, solve the given initial value problem t2x"-12x=0. x(1)=3 and x'(1)=5.
Use the change of variables \(s = \frac{2}{\alpha }\sqrt {\frac{k}{m}} {e^{ - \alpha t/2}}\)to show that the differential equation of the aging spring \(mx'' + k{e^{ - \alpha t}}x = 0\),\(\alpha > 0\)becomes\({s^2}\frac{{{d^2}x}}{{d{s^2}}} + s\frac{{dx}}{{ds}} + {s^2}x = 0\).
For Duffing's equation given in Problem 13, the behaviour of the solutions changes as rchanges sign. When, the restoring forcebecomes stronger than for the linear spring. Such a spring is called hard. When, the restoring force becomes weaker than the linear spring and the spring is called soft. Pendulums act like soft springs.
(a) Redo Problem 13 with. Notice that for the initial conditions, the soft and hard springs appear to respond in the same way forsmall.
(b) Keepingand, change the initial conditions toand. Now redo Problem 13 with.
(c) Based on the results of part (b), is there a difference between the behavior of soft and hard springs forsmall? Describe.
Use Table 6.4.1 to find the first three positive eigen values and corresponding eigen functions of the boundary-value problem\(xy'' + y' + \lambda xy = 0,y(x),y'(x)\)bounded as \(x \to {0^ + },y(2) = 0\). (Hint: By identifying \(\lambda = {\alpha ^2}\), the DE is the parametric Bessel equation of order zero.)
In Problems 13 and 14, use variation of parameters to find a general solution to the given equation for x>0.
x2y"(x)-2xy'(x)+2y(x)=x-1/2
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