Abstract:The current paper is devoted to the study of spreading speeds and traveling wave solutions of the following parabolic-elliptic chemotaxis system,We then consider the extensions of the results in the case N = 1 to the case N ≥ 2.
“…Hence U (·, ·; u) ∈ E. By the similar arguments as those in [14,Lemma 4.3], we can prove that the mapping E ∋ u → U (·, ·; u) ∈ E is continuous and compact. Then there is u * ∈ E such that U (t, x; u * ) = u * (t, x).…”
The current series of research papers is to investigate the asymptotic dynamics in logistic type chemotaxis models in one space dimension with a free boundary or unbounded boundary. Such a model with a free boundary describes the spreading of a new or invasive species subject to the influence of some chemical substances in an environment with a free boundary representing the spreading front. In this first of the series, we investigated the dynamical behaviors of logistic type chemotaxis models on the half line R + , which are formally corresponding limit systems of the free boundary problems. In the second of the series, we establish the spreading-vanishing dichotomy in chemoattraction-repulsion systems with a free boundary as well as with double free boundaries.
“…Hence U (·, ·; u) ∈ E. By the similar arguments as those in [14,Lemma 4.3], we can prove that the mapping E ∋ u → U (·, ·; u) ∈ E is continuous and compact. Then there is u * ∈ E such that U (t, x; u * ) = u * (t, x).…”
The current series of research papers is to investigate the asymptotic dynamics in logistic type chemotaxis models in one space dimension with a free boundary or unbounded boundary. Such a model with a free boundary describes the spreading of a new or invasive species subject to the influence of some chemical substances in an environment with a free boundary representing the spreading front. In this first of the series, we investigated the dynamical behaviors of logistic type chemotaxis models on the half line R + , which are formally corresponding limit systems of the free boundary problems. In the second of the series, we establish the spreading-vanishing dichotomy in chemoattraction-repulsion systems with a free boundary as well as with double free boundaries.
“…Therefore, U (·, ·; u) ∈ E. By the similar arguments as those in [19,Lemma 4.3], the mapping E ∋ u → U (·, ·; u) ∈ E is continuous and compact, and then by Schauder's fixed theorem, it has a fixed point u * . Clearly (u * (·, ·), v 1 (·, ·; u * ), v 2 (·, ·; u * )) is a classical solution of (1.2).…”
The current series of research papers is to investigate the asymptotic dynamics in logistic type chemotaxis models in one space dimension with a free boundary or an unbounded boundary. Such a model with a free boundary describes the spreading of a new or invasive species subject to the influence of some chemical substances in an environment with a free boundary representing the spreading front. In this first part of the series, we investigate the dynamical behaviors of logistic type chemotaxis models on the half line R + , which are formally corresponding limit systems of the free boundary problems. In the second of the series, we will establish the spreading-vanishing dichotomy in chemoattraction-repulsion systems with a free boundary as well as with double free boundaries.
“…(2) In [38,37], the first two authors of the current paper obtained some constants c * low (χ, µ, a, b, λ, µ) < 2 √ a < c * up (χ, a, b, λ, µ) depending explicitly on the parameter χ, a, b, λ and µ such that…”
Section: Statement Of the Main Resultsmentioning
confidence: 91%
“…Some lower and upper bounds for the propagation speeds of solutions with compactly supported initial functions were derived, and some lower bound for the speeds of traveling wave solutions was also derived. It is proved that all these bounds converge to the spreading speed c * 0 = 2 √ a of (1.2) as χ → 0 (see [36], [37], [38]). The reader is also referred to [13] for the lower and upper bounds of propagation speeds of (1.1), and is referred to [1,2,12,16,24,28,31,43], etc., for the studies on traveling wave solutions of various types of chemotaxis models.…”
The current paper is concerned with the spatial spreading speed and minimal wave speed of the following Keller-Segel chemoattraction system,where χ, a, b, λ, and µ are positive constants. Assume b > χµ. Then if in addition, 1 + *
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