Basic Concepts — Question 5

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Question 5

For a normalized linear equation y″+p(t)y′+q(t)y=g(t)y''+p(t)y'+q(t)y=g(t), continuity of p,q,gp,q,g on an open interval containing the initial time guarantees a unique solution throughout that interval for any two initial data.

Consider t(t−2)y″+(t+1)y′+ln⁡(t+3)y=1t−4.t(t-2)y''+(t+1)y'+\ln(t+3)y=\frac 1{t-4}. All functions and solutions are real.

Tasks

  1. Find the domain of the displayed coefficients before normalization. List the additional points excluded when solving for y″y''.

  2. Find the largest theorem-guaranteed interval for initial time t0=1t_0=1, and then for t0=3t_0=3, with arbitrary finite initial value and slope.

  3. Does a finite endpoint of such an interval prove that every solution blows up there? Explain precisely what the theorem does and does not say.

  4. Test that distinction on the separate equation ty″+y′=0ty''+y'=0 with data y(1)=ay(1)=a, y′(1)=by'(1)=b. Solve on (0,∞)(0,\infty) and determine exactly which resulting solutions extend as C2C^2 solutions of the undivided equation across zero.

Original worksheet page 1: question and worked solution for 3-1-005
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Question 5 – Solution

Strategy. Locate coefficient obstructions before applying the theorem, then compare its guaranteed interval with the behavior of actual solutions.

Step 1: Separate domain from degeneracy. The logarithm requires t>−3t>-3 and the forcing excludes t=4t=4. Thus the original coefficient domain is (−3,4)∪(4,∞)(-3,4)\cup(4,\infty). Normalization additionally excludes t=0,2t=0,2, where the leading coefficient vanishes. For other allowed tt, p=t+1t(t−2),q=ln⁡(t+3)t(t−2),g=1(t−4)t(t−2).p=\frac{t+1}{t(t-2)},\qquad q=\frac{\ln(t+3)}{t(t-2)},\qquad g=\frac 1{(t-4)t(t-2)}.

Step 2: Choose the connected interval containing the data. The regular intervals are (−3,0)(-3,0), (0,2)(0,2), (2,4)(2,4) and (4,∞)(4,\infty). Therefore the largest applicable intervals are t0=1:(0,2),t0=3:(2,4).\boxed{t_0=1:\ (0,2)},\qquad \boxed{t_0=3:\ (2,4)}. The initial values do not change these coefficient-based guarantees.

Step 3: State the limitation accurately. The theorem guarantees existence and uniqueness within the selected interval. It does not classify the behavior at a singular endpoint or prove that every solution becomes unbounded there. Whether a particular solution extends requires examination of that solution and the original equation. A coefficient-domain boundary is also distinct from a pole in the solution itself.

Step 4: Solve the comparison equation completely. Since (ty′)′=ty″+y′(ty')'=ty''+y', integration on t>0t>0 gives ty′=Cty'=C, then y=Cln⁡t+Dy=C\ln t+D. The data at 1 imply C=bC=b, D=aD=a, so y=a+bln⁡t(t>0).\boxed{y=a+b\ln t\quad(t>0)}. If b≠0b\ne 0, yy is unbounded as t↓0t\downarrow 0, so no continuous, hence no C2C^2, extension exists. If b=0b=0, the constant solution y=ay=a satisfies the undivided equation on all of ℝ\mathbb R.

Thus extension occurs exactly when b=0\boxed{b=0}. In fact it is unique among C2C^2 extensions: on the negative side every solution has form C−ln⁡|t|+D−C_-\ln|t|+D_-; continuity forces C−=0C_-=0, D−=aD_-=a. The normalized theorem alone did not provide that endpoint conclusion.

Original worksheet page 2: question and worked solution for 3-1-005

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