diquarks  axigluons and heavy vector bosons W and Z bosons  and the techi- ρ in color octet models. The 95% C.L. lower mass limits range from 630 GeV /c 2 for colorons to 1.25 TeV /c 2 for axigluons. The dijet angular distribution has been used to extend the limits on the quark compositeness mass scale  ADD large extra dimensions and the TeV − 1 extra dimensions. The 95% C.L. lower limit on the compositeness mass scale is 2.8 TeV. The 95% C.L. lower limit for compactification mass scale in the TeV − 1 model is 1.5 TeV. The limits on the ADD large extra dimensions range from 1.9 TeV to 1.3 TeV depending on the number of extra dimensions in the HLZ formalism. The 95% C.L. in the GRW formalism is 1.6 TeV. In most cases  these are the best limits to date. We thank Andrew Beretvas  Kenichi Hatakeyama and Marek Zielinski for reading the manuscript and for insightful comments. [1] Gross DJ  Wilczek F Phys. Rev. D 8:3633 (1973); Fritzsch H  Gell-Mann M  Leutwyler H Phys. Lett. B 47:365 (1973); Politzer HD  Phys. Rev. Lett. 30:1346 (1973) [2] Stenzel H Nucl. Phys. B (Proceedings Supplements) 152:23 (2006) [3] Gwenlan C Acta. Phys. Polon. B 35:377 (2004) [4] Fabjan C  McCubbin N Phys. Rep. 403:165 (2004) [5] Blazey GC  Flaugher BL Annu. Rev. Nucl. Part. Sci. 49:633 (1999) [6] Salam GP  arXiv:0906.1736v3 [hep-ph] 2 July 2009 [7] Gribov VN  Lipatov LN Sov. J. Nucl. Phys 15:438 (1972); Altarelli G  Parisi G Nucl. Phys. B 126:298 (1977); Dokshitzer Yu Sov. Phys. JETP 46:641 (1977) [8] Sj¨ ostrand T  et al. JHEP 0605:026 (2006) [9] Corcella G  et al. JHEP 0101:010 (2001) [10] Frixione S  Webber BR JHEP 0206:29 (2002) [11] Abulencia A  et al. J. Phys. G: Nucl. Part. Phys. 34:2457 (2007) [12] Abazov VM  et al. Nucl. Instrum. Methods Phys. Res. Sect. A 565:463 (2006) [13] Ellis RK  Stirling WJ  Webber BR QCD and Collider Physics   Cambridge Press. (1996) [14] Ellis SD  Kunszt Z  Soper DE Phys. Rev. Lett. 64:2121 (1990) [15] Giele WT  Glover EWN  Kosower DA Nucl. Phys. B 403:633 (1993) [16] Nagy Z Phys. Rev. D 68:094002 (2003) 36