Rock/Bit-Tooth Interaction for Conical Bit Teeth

1971 ◽  
Vol 11 (02) ◽  
pp. 162-170 ◽  
Author(s):  
T.W. Miller ◽  
J.B. Cheatham

Abstract Insert-type bit teeth are axially symmetric and therefore cannot be properly described by a two-dimensional, plane-strain analysis of a wedge-shaped tooth. Since few exact plasticity solutions exist for axially symmetric problems, an approximate method is developed and applied to the interaction of a conical bit tooth with rock. Numerical results of the approximate method compare favorably with the known exact solutions. Alter making allowance for the experimental result of little or no lip formation around an indentation, numerical results using the approximate method correlate well with experimental measurements for the indentation of conical teeth into marble and sandstone. Introduction Previous studies of the interaction of bit teeth with rock have been concerned primarily with two-dimensional wedge-shaped teeth. This provides a good approximation to the shape of most bit teeth, and the two-dimensional analysis simplifies the problem. However, some bits have inserts or so-called "buttons", which cannot be adequately represented by a wedge. Also, "end effects" exist for the finite-length wedges, whereas cones, flat-circular cylinders and hemispheres, while axially symmetric, are truly three-dimensional. These axially symmetric punches pose a more difficult problem analytically; hence one of the objectives of this paper is to provide an approximate method for analysis of this class of problems. problems. The analysis of problems concerned with the indentation of a rigid/plastic half space by an axially symmetric indenter is more difficult than the analogous problem in plane strain due to the radial expansion that occurs with increased distance from the axis of symmetry. The axially symmetric solutions are also of interest because they give insight into other practical problems, such as analysis of Rockwell-type hardness tests and end effect corrections for plane-strain solutions. DISCUSSION OF EXACT SOLUTIONS Ishlinski has solved the problem of the indentation of a plastic half space by a perfectly smooth, flat punch by tedious hand calculations, whereas Shield and Cox et al. have rigorously solved the perfectly smooth, flat-punch problem for metals and soils, respectively, using finite-difference techniques requiring a digital computer. Mroz has developed a graphics technique for the above problem for metals, but it, too, is a long, tedious procedure. Lockett has solved problems for the indentation of metals by perfectly smooth, conical indenters with half-cone angles between 52.5 degrees and 90 degrees, also using finite-difference equations. Berezancev has presented values of average pressure on cones with hall-cone angles of 15 degrees and 30 degrees for indentation of both metals and soils. Eason and Shield have given the solution for the indentation of metals by a perfectly rough, flat indenter, again using finite-difference equations. Problems for perfectly rough, flat indenters Problems for perfectly rough, flat indenters penetrating soils and perfectly rough, conical penetrating soils and perfectly rough, conical indenters penetrating soils and metals have not yet been solved to the authors' knowledge. Spencer has presented an approximate solution for an annular, flat punch using perturbation methods. This method does not seem applicable to conical indenters, however, since it requires a fixed punch radius that is large with respect to other dimensional quantities of the problem. If the approximate method presented here were applied to the annular punch problem, it would give results corresponding to Spencer's first-order solution. It is the purpose of the present paper to compare the results of the approximate method of finding pressure distributions on a conical indenter with pressure distributions on a conical indenter with some of the exact results discussed above; and then to use other results of the approximate method to analyze experimental data. The numerical results used to analyze experimental data are calculated using a modified slip-line field for a formation. SPEJ P. 162

Author(s):  
H. C. Bolton ◽  
H. I. Scoins

ABSTRACTA discussion is given of the convergence of the eigenvalues Λ (N) of two-dimensional finite-difference equations towards the eigenvalues Λ of the corresponding second-order differential equation, and it is shown thatwhere h = N−1 and ν2 is a constant. As in our previous paper (4), this can be used to make an accurate estimate of λ by extrapolating to h = 0. After an account of the relaxation method used for computing Λ(N) and a discussion of the residual vector, results are presented for an approximation to the lowest spatially symmetric and antisymmetric states of two electrons in a sphere, interacting through their Coulomb potential.


1979 ◽  
Vol 101 (2) ◽  
pp. 276-283 ◽  
Author(s):  
P. Orlandi ◽  
D. Cunsolo

A finite difference procedure is employed to evaluate the primary flow field in two typical elbows. The first has an internal wall radius equal to the width; the internal radius of the second sharper elbow is equal to one half of the width. Two dimensional flow is assumed and a 20 by 20 grid network is employed in both cases. The field is transformed into a rectangular one by generalized curvilinear coordinates. Velocity profiles and streamline patterns are presented and discussed. In both cases the outflow attains the parabolic profile assumed for the inflow. The pressure distributions on the internal and external walls have been calculated.


Geophysics ◽  
1974 ◽  
Vol 39 (1) ◽  
pp. 39-48 ◽  
Author(s):  
Ian C. Briggs

Machine contouring must not introduce information which is not present in the data. The one‐dimensional spline fit has well defined smoothness properties. These are duplicated for two‐dimensional interpolation in this paper, by solving the corresponding differential equation. Finite difference equations are deduced from a principle of minimum total curvature, and an iterative method of solution is outlined. Observations do not have to lie on a regular grid. Gravity and aeromagnetic surveys provide examples which compare favorably with the work of draftsmen.


2001 ◽  
Vol 6 (2) ◽  
pp. 3-14 ◽  
Author(s):  
R. Baronas ◽  
F. Ivanauskas ◽  
I. Juodeikienė ◽  
A. Kajalavičius

A model of moisture movement in wood is presented in this paper in a two-dimensional-in-space formulation. The finite-difference technique has been used in order to obtain the solution of the problem. The model was applied to predict the moisture content in sawn boards from pine during long term storage under outdoor climatic conditions. The satisfactory agreement between the numerical solution and experimental data was obtained.


1968 ◽  
Vol 19 (1) ◽  
pp. 1-19 ◽  
Author(s):  
H. McDonald

SummaryRecently two authors, Nash and Goldberg, have suggested, intuitively, that the rate at which the shear stress distribution in an incompressible, two-dimensional, turbulent boundary layer would return to its equilibrium value is directly proportional to the extent of the departure from the equilibrium state. Examination of the behaviour of the integral properties of the boundary layer supports this hypothesis. In the present paper a relationship similar to the suggestion of Nash and Goldberg is derived from the local balance of the kinetic energy of the turbulence. Coupling this simple derived relationship to the boundary layer momentum and moment-of-momentum integral equations results in quite accurate predictions of the behaviour of non-equilibrium turbulent boundary layers in arbitrary adverse (given) pressure distributions.


2020 ◽  
Vol 7 (1) ◽  
pp. 48-55 ◽  
Author(s):  
Bolat Duissenbekov ◽  
Abduhalyk Tokmuratov ◽  
Nurlan Zhangabay ◽  
Zhenis Orazbayev ◽  
Baisbay Yerimbetov ◽  
...  

AbstractThe study solves a system of finite difference equations for flexible shallow concrete shells while taking into account the nonlinear deformations. All stiffness properties of the shell are taken as variables, i.e., stiffness surface and through-thickness stiffness. Differential equations under consideration were evaluated in the form of algebraic equations with the finite element method. For a reinforced shell, a system of 98 equations on a 8×8 grid was established, which was next solved with the approximation method from the nonlinear plasticity theory. A test case involved computing a 1×1 shallow shell taking into account the nonlinear properties of concrete. With nonlinear equations for the concrete creep taken as constitutive, equations for the quasi-static shell motion under constant load were derived. The resultant equations were written in a differential form and the problem of solving these differential equations was then reduced to the solving of the Cauchy problem. The numerical solution to this problem allows describing the stress-strain state of the shell at each point of the shell grid within a specified time interval.


2021 ◽  
Vol 136 (3) ◽  
pp. 791-812
Author(s):  
Peder A. Tyvand ◽  
Jonas Kristiansen Nøland

AbstractThe onset of thermal convection in two-dimensional porous cavities heated from below is studied theoretically. An open (constant-pressure) boundary is assumed, with zero perturbation temperature (thermally conducting). The resulting eigenvalue problem is a full fourth-order problem without degeneracies. Numerical results are presented for rectangular and elliptical cavities, with the circle as a special case. The analytical solution for an upright rectangle confirms the numerical results. Streamlines penetrating the open cavities are plotted, together with the isotherms for the associated closed thermal cells. Isobars forming pressure cells are depicted for the perturbation pressure. The critical Rayleigh number is calculated as a function of geometric parameters, including the tilt angle of the rectangle and ellipse. An improved physical scaling of the Darcy–Bénard problem is suggested. Its significance is indicated by the ratio of maximal vertical velocity to maximal temperature perturbation.


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