Euler’s Method — Question 5

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Question 5

A normalized population satisfies p′=2p(1−p),0≤p(0)≤1.p'=2p(1-p),\qquad 0\le p(0)\le 1. The exact solution preserves the physical interval [0,1][0,1]. For explicit Euler with step h>0h>0, write Pn+1=Fh(Pn)P_{n+1}=F_h(P_n). For the local discrete comparison, a small perturbation near P=1P=1 is multiplied to first order by Fh′(1)F_h'(1); call the linearized update contracting when |Fh′(1)|<1|F_h'(1)|<1.

Tasks

  1. Derive FhF_h and find exactly which positive steps map all of [0,1][0,1] back into [0,1][0,1].

  2. Prove the condition is necessary, not merely sufficient, by producing an overshooting initial value whenever it fails.

  3. Compute the first two Euler updates for h=1h=1, P0=3/4P_0=3/4, and explain why they misrepresent the exact solution’s qualitative behavior.

  4. Find the step range for linearized contraction at 11. Compare it with interval preservation, and sketch the update maps for h=1/4h=1/4 and h=1h=1.

Original worksheet page 1: question and worked solution for 2-9-005
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Question 5 – Solution

Strategy. Check the whole physical interval, not only the behavior of tiny perturbations near its upper endpoint.

Step 1: Factor the interval constraint. Euler gives Fh(p)=p+2hp(1−p)F_h(p)=p+2hp(1-p). On [0,1][0,1] it is nonnegative. Also 1−Fh(p)=(1−p)(1−2hp).1-F_h(p)=(1-p)(1-2hp). If 0<h≤1/20<h\le 1/2, both factors are nonnegative for every p∈[0,1]p\in[0,1], so Fh(p)≤1F_h(p)\le 1. Therefore 0<h≤1/2\boxed{0<h\le 1/2} preserves the interval at every step by induction.

Step 2: Prove necessity. If h>1/2h>1/2, choose pp strictly between 1/(2h)1/(2h) and 11. Then 1−p>01-p>0 but 1−2hp<01-2hp<0, so Fh(p)>1F_h(p)>1. Such a value exists for every h>1/2h>1/2, proving the stated condition is exact.

Step 3: Exhibit overshoot. For h=1h=1, F1(p)=3p−2p2F_1(p)=3p-2p^2, giving P1=9/8=1.125,P2=27/32=0.84375.\boxed{P_1=9/8=1.125,\qquad P_2=27/32=0.84375}. The numerical solution crosses above the capacity and then drops. The exact solution starting at 3/43/4 increases toward 11 from below and cannot cross that equilibrium, by uniqueness.

See the diagram in the original worksheet below.

Step 4: Distinguish two step restrictions. Since Fh′(p)=1+2h−4hpF_h'(p)=1+2h-4hp, Fh′(1)=1−2hF_h'(1)=1-2h. Linearized contraction therefore holds for 0<h<1\boxed{0<h<1}, a larger range than interval preservation. At h=1h=1 the linearized magnitude equals one, so the strict contraction test makes no decision about nonlinear asymptotic behavior.

A locally contracting update can still move some valid states above the physical bound. The map criterion protects the entire interval; the derivative criterion only describes first-order behavior near one fixed point.

Original worksheet page 2: question and worked solution for 2-9-005

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