AFTER DISCOVERY OF CARBON NANOTUBE (CNT) BY IIJIMA [1] NUMEROUS STUDIES DEDICATED TO THE INVESTIGATIONS OF PROPERTIES AND APPLICATIONS OF THESE NOVEL MATERIALS [2, 3]. THE CONSIDERABLE STUDIES DEDICATED TO THE INVESTIGATION OF NON-CARBON BASED NANOTUBES THAT THE COUNTERPARTS OF GROUPS III AND V OF ELEMENTS, SUCH AS BORON NITRIDE, ALUMINIUM NITRIDE, GALLIUM NITRIDE, INDIUM NITRIDE, BORON PHOSPHIDE, ALUMINIUM PHOSPHIDE, GALLIUM PHOSPHIDE, AND INDIUM PHOSPHIDE COUNTERPARTS. THE THEORETICAL STUDIES SHOW THAT THE ELECTRONIC PROPERTY, BAND GAP OF ENERGY AND NMR PARAMETERS OF THESE NANOTUBES ARE ALMOST INDEPENDENT OF THE NUMBER OF WALLS [4]. IN THE PRESENT WORK, WE HAVE INVESTIGATED THE ELECTRONIC AND STRUCTURAL PROPERTIES OF ALUMINIUM PHOSPHIDE NANOTUBE (ALPNTS) BASED ON DFT METHODS .THE GEOMETRICAL STRUCTURES OF PRISTINE AND GE-DOPED (6, 0), (8, 0) AND (10, 0) ZIGZAG MODELS OF ALPNTS ARE OPTIMIZED BY USING B3LPY LEVEL OF THEORY AND 6-31G** BASE SET. THE STRUCTURAL PARAMETERS INVOLVING BOND LENGTH, BOND ANGLE, DOPING ENERGY, BAND GAP AND NQR PARAMETERS OF UNDOPED AND GE-DOPED OF ABOVE ZIGZAG MODELS OF ALPNTS ARE CALCULATED. THE RESULTS REVEAL THAT WITH DOPING GE THE BOND LENGTH OF NEIGHBOURHOOD OF GE DOPED AT THREE MODELS INCREASE FROM UNDOPED MODELS AND THE BOND ANGLE DECREASE. THE RESULTS SHOW THAT DOPING ENERGY AT (6, 0) ZIGZAG MODEL IS MORE NEGATIVE THAN OTHER MODELS. THE ENERGY OF INTERACTION BETWEEN 27AL NUCLEI WITH EFG TENSOR IS DEFINED AS QUADRUPOLE COUPLING CONSTANT (CQ) WHICH IS EITHER EXPERIMENTALLY MEASURED BY NQR SPECTROSCOPY OR COMPUTED BY QUANTUM CHEMICAL CALCULATIONS. THE RESULTS REVELS THAT THE VALUES OF CQ (27AL) AT FIRST LAYER OF ALL MODELS ARE LARGEST AMONG OTHER LAYERS. THE AL ATOMS PLACED AT THE FIRST LAYER PLAY DOMINANT ROLES IN DETERMINING THE ELECTRONIC BEHAVIOR OF NANOTUBE.