Commercial Tree Chipper: The Leg Pull-In Hypothesis

Author(s):  
Dennis B. Brickman

This paper addresses a commercial mobile tree chipper with a mechanical infeed system that is manually fed. The purpose of this paper is to show that tree branches and brush presented to a disc chipper through the infeed hopper will not pull an erectly standing operator’s leg off the ground and into the feed wheels given the conditions set forth in this test program. In order for an erectly standing operator’s leg to contact the feed wheels, it is necessary for the leg to be pulled off the ground and over the bottom leading edge of the infeed hopper. Experiments demonstrate that the operator’s leg is pulled up against the lower leading edge of the infeed hopper and lodges there during pull-in scenarios using a winch, cable, and rope attached to the operator’s ankle. Two safety devices, an infeed extension pan and a safety control bar are explored in this paper.

Author(s):  
Pengfei Liu ◽  
Ayhan Akinturk ◽  
Moqin He ◽  
Mohammed Fakhrul Islam ◽  
Brian Veitch

Fluid-structure interaction between an ice sheet on the water surface and a podded R-Class propeller was examined and analyzed in terms of numerical simulation using a newly enhanced unsteady time-domain, multiple body panel method model. The numerical model was validated and verified and also checked against various previous in-house experimental measurements. The simulation was performed in a real unsteady case, that is, the ice piece stands still and the podded propeller moves and approaches the ice piece until collision occurs. Experimental data were taken from a previous cavitation tunnel test program for a bare R-Class ice breaker propeller under open water conditions, for the R-Class propeller approaching a blade-leading-edge contoured large size ice block under the proximity condition, and from an ice tank test program for a tractor type podded/strutted R-Class propeller under open water conditions. Comparison between experimental and numerical results was made. A general agreement was obtained. The magnitude of force fluctuations during the interaction increased significantly at the instant immediately before the impact between the propeller blades and the ice piece.


Author(s):  
Dennis B. Brickman

This paper addresses the ability of a human worker to activate safety devices to stop and reverse the mechanical infeed system inside a commercial tree chipper infeed hopper. Studies were performed using a tray equipped commercial tree chipper incorporating a safety control bar and safety cables to stop and reverse the mechanical infeed system. The test results indicate that the human test subject was able to successfully activate the safety control bar and the safety cables from a variety of body positions around and within the tree chipper infeed hopper.


Author(s):  
J. Furlan ◽  
K. Pagalthivarthi ◽  
H. Tian ◽  
P. Barsh ◽  
R. Visintainer

Abstract Empirical wear coefficients are used in concert with computational fluid dynamics (CFD) codes which model highly loaded slurry flows through centrifugal pumps in order to predict erosive wear in wet-end components. In practice, separate sets of wear coefficients are used to determine the contributions of sliding and impact wear to the total erosive wear at the wetted surface. In this study, experiments were performed in order to obtain the impact wear coefficients for sand in a water slurry impinging on high chrome white iron alloys that are commonly used in the construction of heavy duty centrifugal slurry pumps. Two separate sets of tests were completed using two different types of narrowly graded sand, with mass median particle diameters of approximately 600 μm and 300 μm respectively. The tests were performed in a closed loop containing a slurry pump, flow meter, inverted U loop for determination of the solids concentration, and 8 sample sections arranged serially. Each sample section was constructed from polyurethane, with rectangular flow cross sections of 1 inch (25.4 mm) width and 2 inch (50.8 mm) height and lengths of 1 foot (305 mm). One metal sample was placed into each sample holder so that it spanned across the 1 inch (25.4 mm) width and was exposed to the slurry flow, with its edges being supported by the flat polyurethane walls on either side. The samples were machined to have constant angles on the leading edge faces which varied from 10 to 60 degrees (from sample to sample), in order to obtain a range of impact angles (angle between the particle trajectory and the wetted surface) of the particles impinging on the sample leading edge faces. Tests were run at 12 % concentration by volume and at mean channel-sectional flow velocities of 10 m/s, with run times varying from 30 minutes to 180 minutes over the course of the test program. Slurry loop samples were taken at the beginning and end of each run in order to determine the particle size distribution and to monitor degradation of solids through sieve and micrograph analysis. The worn wedge face surfaces were scanned at intermittent times throughout the testing using an optical profilometer, and the local erosive wear was determined on the slanted face of, as well as at the tip of, the wedge-shaped samples. The progression of wear over the course of the test program was measured and analyzed in this manner. The local solids concentration, velocity, and impact angle was then predicted using in-house CFD codes formulated in the same manner as the pump wear models. The experimental wear profiles, together with the predicted local solids concentration, velocity, and impact angle, were then used to calculate the specific energy coefficient (or impact wear coefficient) at multiple impact angles. A formulation for the impact wear coefficient as a function of impact angle at a given particle size was then produced at each of the two different particle diameters. By comparing the data between the two different particle diameters, an adjustment factor for particle diameter was then formulated. This paper primarily focuses on the experimental test program, providing a description of the experiments, results, and data analysis, as well as a discussion of the results and some description of the test-derived wear coefficient formulations.


Author(s):  
Pengfei Liu ◽  
Ayhan Akinturk ◽  
Moqin He ◽  
Mohammed Fakhrul Islam ◽  
Brian Veitch

Fluid-structure interaction between an ice sheet on the water surface and a podded R-Class propeller was examined and analyzed in terms of numerical simulation using a newly enhanced unsteady time-domain, multiple body panel method model. The numerical model was validated and verified and also checked against various previous in-house experimental measurements. The simulation was performed in a real unsteady case, that is, the ice piece stands still and the podded propeller moves and approaches the ice piece until collision occurs. Experimental data were taken from a previous cavitation tunnel test program for a bare R-Class ice breaker propeller under open water conditions, for the R-Class propeller approaching a blade-leading-edge contoured large size ice block under the proximity condition, and from an ice tank test program for a tractor type podded/strutted R-Class propeller under open water conditions. Comparison between experimental and numerical results was made. A general agreement was obtained. The magnitude of force fluctuations during the interaction increased significantly at the instant immediately before the impact between the propeller blades and the ice piece.


Author(s):  
John J. Friel

Committee E-04 on Metallography of the American Society for Testing and Materials (ASTM) conducted an interlaboratory round robin test program on quantitative energy dispersive spectroscopy (EDS). The test program was designed to produce data on which to base a precision and bias statement for quantitative analysis by EDS. Nine laboratories were sent specimens of two well characterized materials, a type 308 stainless steel, and a complex mechanical alloy from Inco Alloys International, Inconel® MA 6000. The stainless steel was chosen as an example of a straightforward analysis with no special problems. The mechanical alloy was selected because elements were present in a wide range of concentrations; K, L, and M lines were involved; and Ta was severely overlapped with W. The test aimed to establish limits of precision that could be routinely achieved by capable laboratories operating under real world conditions. The participants were first allowed to use their own best procedures, but later were instructed to repeat the analysis using specified conditions: 20 kV accelerating voltage, 200s live time, ∼25% dead time and ∼40° takeoff angle. They were also asked to run a standardless analysis.


2013 ◽  
Author(s):  
Yuenghsiang E. Huang ◽  
Peter Y. Chen ◽  
Autumn D. Krauss ◽  
Apryl Rogers

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