# Maximum principle of harmonic function without mean value formula

Are there any way to prove maximum principle of harmonic functions without the mean value formula? In other words I would like to show $$\max_{\overline{\Omega}}(f)=\max_{\partial \Omega}(f)$$ for a harmonic function $f$ on a bounded domain $\Omega$ without using the formula $$f(x)=\frac{1}{V(B(x,r)}\int_{B(x,r)}f(z)dz.$$

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Yes, just think of the 1D-case: $f''=0$ on $(a,b)$. The function $f$ attains a maximum in $[a,b]$, and you must exclude that this maximum point lies in $(a,b)$. You first treat the situation where $f''>0$ in $(a,b)$, and then perturb $f$, for example $f(x)+\varepsilon x^2$.