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Blow-up of Solutions of Semilinear Parabolic Equations

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where ∫ 1<br />

√<br />

dy<br />

0<br />

then it follows that<br />

is a constant dependent on p. Define C<br />

1−y p+1 p := ∫ 1<br />

0<br />

ϕ(M) = C p M − p−1<br />

2 .<br />

√<br />

Since ϕ is monotone decreasing and the range <strong>of</strong> ϕ is (0, ∞), ϕ(M) =<br />

has a unique positive solution for every L > 0.<br />

Theorem 6. Consider the problem<br />

⎧<br />

⎨ u t = u xx + u p , |x| < 1, p > 1,<br />

(P) u = 0, |x| = 1,<br />

⎩<br />

u(x, 0) = u 0 (x), |x| < 1.<br />

dy<br />

√1−y p+1 ,<br />

2<br />

L p+1<br />

q.e.d.<br />

If u 0 (x) ≥ v(x), u 0 ≢ v(x), v is the solution <strong>of</strong> (S), then u blows <strong>up</strong> in finite<br />

time.<br />

Pro<strong>of</strong>. By the maximum principle, if τ > 0, then u(x, τ) > v(x) for |x| < 1.<br />

Moreover u x (1, τ) < v x (1) and u x (−1, τ) > v x (−1). Hence there is k > 1<br />

such that u(x, τ) > kv(x).<br />

Thus, it is suffcient to consider the case where u 0 (x) = kv(x), k > 1. In<br />

this case, we have<br />

(u t ) t = (u t ) xx + pu p−2 u t , |x| < 1,<br />

u t = 0, |x| = 1,<br />

u t (x, 0) = kv xx + k p v p > k(v xx + v p ) = 0.<br />

By the maximum principle, we obtain u t ≥ 0 as long as u exists.<br />

S<strong>up</strong>pose u is global. If u is bounded, there exists a solution w(x) <strong>of</strong> (S)<br />

such that<br />

u(x, t) → w(x) as t → ∞, w(x) > v(x), |x| < 1,<br />

this is a contradiction with Theorem 5.<br />

If u is unbounded, then<br />

u(x, t) ≡ u(−x, t), u x (x, t) < 0 for x ∈ [0, 1),<br />

and either<br />

or<br />

(i) lim<br />

t→∞<br />

u(x, t) < ∞, x ∈ (a, 1], a ∈ (0, 1],<br />

(ii) lim<br />

t→∞<br />

u(x, t) = ∞, |x| < 1,<br />

8

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