The dimensional nonlinear Kompaneets (NLK) equation \({u_{t} = x^{-2}[x^{4}(\alpha{u}_{x} + \beta{u} + \gamma{u}^{2})]_{x}}\) describes the spectra of photons interacting with a rarefied electron gas. Recently, Ibragimov obtained some time-dependent exact solutions for several approximations of this equation. In this paper, we use the nonclassical method to construct time-dependent exact solutions for the NLK equation \({u_{t} = x^{-2}[x^{4}(\alpha{u}_{x} + \gamma{u}^{2})]_{x}}\) for arbitrary constants α > 0, γ > 0. Solutions arising from “nonclassical symmetries” are shown to yield wider classes of time-dependent exact solutions for the NLK equation \({u_{t} = x^{-2}[x^{4}(\alpha{u}_{x} + \gamma{u}^{2})]_{x}}\) beyond those obtained by Ibragimov. In particular, for five classes of initial conditions, each involving two parameters, previously unknown explicit time-dependent solutions are obtained. Interestingly, each of these solutions is expressed in terms of elementary functions. Three of the classes exhibit quiescent behavior, i.e., \({\lim_{t\rightarrow \infty}u(x,t) = 0}\) , and the other two classes exhibit blow-up behavior in finite time. As a consequence, it is shown that the corresponding nontrivial stationary solutions are unstable.
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