This paper is concerned with a reaction–diffusion system with gradient terms under Robin boundary conditions { ( h ( u ) ) t = ∇ ⋅ ( | ∇u | p − 2 ∇u ) + f ( u , v , | ∇u | 2 , t ) in Ω × ( 0 , t ∗ ) , ( r ( v ) ) t = ∇ ⋅ ( | ∇v | q − 2 ∇v ) + g ( u , v , | ∇v | 2 , t ) in Ω × ( 0 , t ∗ ) , ∂ u ∂ ν + γu = 0 , ∂ v ∂ ν + σv = 0 on ∂Ω × ( 0 , t ∗ ) , u ( x , 0 ) = u 0 ( x ) ≥ 0 , v ( x , 0 ) = v 0 ( x ) ≥ 0 in Ω ¯ , where p, q>2 and Ω ⊂ R N ( N ≥ 2 ) is a bounded domain with smooth boundary. Under some suitable assumptions, a sufficient condition that ensures the positive solution blows up in a finite time is obtained. Meanwhile, the upper bound for the blow-up time and the upper estimate for the blow-up rate are derived. The key to the research is to use the maximum principles and differential inequality technique. In addition, as an application of the abstract results obtained in this paper, an example is given.
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