A method for construction of the multipartite Clauser-Horne-Shimony-Holt (CHSH) type Bell inequalities, for the case of local binary observables, is presented. The standard CHSH-type Bell inequalities can be obtained as special cases. A unified framework to establish all kinds of CHSHtype Bell inequalities by increasing step by step the number of observers is given. As an application, compact Bell inequalities, for eight observers, involving just four correlation functions are proposed. They require much less experimental effort than standard methods and thus is experimentally friendly in multi-photon experiments.PACS numbers: 03.65. Ta, 03.65.Ud, 42.50.Xa Quantum mechanics is incompatible with local realism [1]. Bell inequalities reveal this fact. The more Bell inequalities we know, the more we know about the boundaries between Einstein's local realism and the genuinely non-classical areas of quantum physics, which are potentially useful in quantum information applications. For N observers, each choosing between two local dichotomic observables, the complete set of tight CHSHtype [2] Bell inequalities has been obtained [6,7]. Such inequalities have been pointed out to possess a common structure [8]. However, in the case of more complicated situations (i.e., with more local settings, more parties, or more measurement outcomes), it is still an open task to obtain the complete set of tight Bell inequalities.Many methods have been put forward to establish Bell inequalities for different situations, such as using the algebraic properties of local observables [9,10], the stabilizer group of quantum states [11], and so on. Among these methods, there exists a very important method, which bases on the fact that the set of local realistic models forms a polytope [12], usually called the correlation polytope, whose vertices are the deterministic events. The facets of correlation polytope define tight Bell inequalities. Despite the fact that all vertices of such a correlation polytope are known, it is still difficult to determine all its facets [13]. In the simpler case of three qubits, with to numerical methods one may obtain all facets of correlation polytope [14,15]. The geometrical concept of correlation polytopes is also helpful for building some new Bell inequalities for more complicated cases [8,[16][17][18].Nevertheless, observations of violations of local realism in the case of multipartite correlations are a challenging task. Generation of multipartite entangled states is a challenge itself [19]. Usually, polarization entangled states are generated. The two-photon polarization entangled state (Bell states) can be generated using the technique announced in [20]. Using methods put forward in [21], the three-photon Greenberger-HorneZeilinger (GHZ) state can be generated [22]. Pan's group has generated five-photon [23] and six-photon [24] GHZ states. Very recently, an eight-photon GHZ entanglement has been generated [25,26]. However, such experiments require long time to gather data to get the value of a correlati...