Modelling of vibro-impact penetration of self-exciting
percussive-rotary drill bit A.D. Batako*, V.I. Babitsky, N.A. Halliwell Wolfson School of Mechanical and Manufacturing Engineering, Loughborough University, Loughborough, Leicestershire LE11 3TU, UK Received 17 September 2002; accepted 24 February 2003
The penetration of a drilling tool into a hard medium under periodicimpac t action is analyzed and the simulation model presented. This is further development of previously investigated model of a self-excited percussive-rotary drilling system. The system used the stick–slip phenomenon to generate an impact action superimposed on the drilling process. A phenomenological visco-elasto-plastic model of the media is used and the system response is studied numerically, first as a forced vibration and second as a result of a selfexcited vibro-impact process. Relief of the main drive has been obtained and an increase in the rate of penetration is observed with increased impact intensity and hardening of the medium. Results of the preliminary drilling experiment with superimposed dynamica ction have shown an improvement in the rate of penetration. r 2003 Elsevier Ltd. All rights reserved.
2. Early vibro-impact penetration concepts
The initial theoretical analysis of the vibro-penetration process was made by Neimark and Blekhman. Two models of the indenter–footing resistance were mainly used to reflect the primary experimental data. In the purely plasticmodel, the resistance was presented as weightless plug held in the borehole by the permanent force. The advance of the plug is possible when the sum of the applied forces exceeds the resistance force. Under these circumstances the plug followed to the movement of the indenter.An elasto-plastic model, known as Prandtl model, took into consideration the elasticity of the medium by adding an ideal spring between the indenter and plug. In this model, the movement of the plug is only possible when the elastic force of the spring exceeds the resistance of the medium. More complex rheological models of the medium were also used.
In percussive-rotary drilling the tool moves into the medium by an impact–scratching action and inherently removes off cuttings. This permits use of a simplified model to estimate the ROP due to impact. The model below takes into consideration the frontal resistance of the medium as an elasto-plastic process and viscous dissipation during the vibration of the bit.3 Study of the system under impact loading
From the UCS test, the stiffness of the rock cores was estimated to be 0.9, 1.6 and 2.11MN/m for the sandstone, limestone and the granite, respectively. The threshold force D was also obtained as 61.9, 140 and 204kN for the respective types of rock. The core samples and the test complied with the requirements of the ASTM and the British Standard BS1610. The diameter ?d? of the cores was 54mm and the height ?L? 108 mm; the ratio L=d is 2 and the standard requires that 2pL=dp4. The UCS test was carried out in the civil engineering laboratory of rock mechanics on the ‘‘Denison’’ Block Testing System. A load was applied to each core at the rate of 0.17 kN/s.The computer controlling the testing machine produced the plots of the load against the displacement. The UCS values for the limestone and the granite seem rather higher than average because the rock blocks were of a very good quality, fresh and dry. Consequently, the investigation was carried out within a range covering these values and the following settings were used: k3A[1,5] MN/m, DA[50,300]kN with a damping ratio zA[0.5,1.5]. These values of the damping ratio allow the observation of the underdamped, critically damped and overdamped motion of the system under impact excitation.