We study the blow-up and/or global existence of the following $p$-Laplacian evolution equation with variable source power $$u_t(x,t)=\textrm{div}(| \nabla u|^{p-2} \nabla u)+u^{q(x)} \quad\textrm{in} \quad\Omega \times (0,T),$$ where $ \Omega$ is either a bounded domain or the whole space $\mathbb{R}^N$, and $ q(x)$ is a positive and continuous function defined in $ \Omega$ with $0<q_-=\inf q(x)\leq q(x)\leq \sup q(x)=q_+<\infty$. It is demonstrated that the equation with variable source power has much richer dynamics with interesting phenomena which depends on the interplay of $q(x)$ and the structure of spatial domain $ \Omega$, compared with the case of constant source power. For the case that $\Omega$ is a bounded domain, the exponent $p-1$ plays a crucial role. If $q_+>p-1$, there exist blow-up solutions, while if $q_+<p-1$, all the solutions are global. If $q_->p-1$, there exist global solutions, while for given $q_-<p-1<q_+$, there exist some function $q(x)$ and $\Omega$ such that all nontrivial solutions will blow up, which is called the Fujita phenomenon. For the case $\Omega= \mathbb{R}^N$, the Fujita phenomenon occurs if $1<q_-\leq q_+\leq p-1+p/N$, while if $q_->p-1+p/N$, there exist global solutions.
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