MATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES IN GREENHOUSES
|
|
- Dwain Banks
- 5 years ago
- Views:
Transcription
1 Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II: Forestry Wood Industry Agricultural Food Engineering MATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES IN GREENHOUSES Gheorghe BRĂTUCU Abstract: Preparing the gerination bed in greenhouses can be done by several technologies, ost of the including soil digging with a special achine anufactured for this purpose. The ain disadvantage of this achine refers to the relatively high energetic consuption, which increases the work cost. Starting fro the working process executed by the achine, the total energetic consuption is decoposed in representative coponents, for which the energetic coputation relations are given. Finally a coplex and general relation of the energetic consuption is obtained, by which interesting processing optiization solutions are being offered for this iportant functional paraeter, available for designers and anufactures but also for users. Key words: greenhouses, atheatical odel, soil digging achine.. Introduction Matheatical odeling of the energetic of soil digging achines in protected spaces eans to establish the relations of calculation of the necessary energy coponents in ground processing and their analysis in order to find ethods of reducing energy consuption in the work of preparing the seed-bed in greenhouses [], [ ], [4]. Based on the study of the energetic of the achinery on the work of preparing the gerination bed in greenhouses, the total echanical energy coponents for each of the were deterined, which are shown in Figure. Energy consuption in works of the soil, in general, are characterized by [3]: specific cutting surface of the soil S sp and the specific echanical work, L s. Specific surface for cutting the unit volue of the soil is the ratio of area and volue of the displaced soil in / 3. Specific echanical work is the work necessary for processing the deployent of the unit volue of soil, J/ 3 [5], [6].. Material and Method Energy consued during soil processing with soil digging achine, E ts, is used for the oveent of the working achine, for cutting and deployent of soil slices, for throwing the deployed slices, for self pushing and for covering the loss fro the transission of the achine, is: Dept. of Food Products Engineering, Transilvania University of Braşov.
2 44 Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II Total echanical energy required, E t E work, the energy required for processing soil Energy required carrying the achine Energy necessary to carry out the echanical processing operations E loss, the energy required to cover the loss in transission Analysis of coponents Fig.. Methodology of the study and atheatical odeling of total echanical energy E = E E E E E [J]. () ts oveent cut trow push loss Starting fro equation (), the total energy required to drive achinery to dig the soil with plain working coponent is calculated with: E ts = f G s v s π a B ρ g tg ψ v ϖ µ ρ g a b ϖ z sin ψ cos ψ π s E loss [J], s v s B a ρ v v x s () where: f is the coefficient of tire rolling resistance between the soil and the achine; G s - weight of the achine, [N]; v - achine speed, [/s]; t s - tie of digging, [s]; µ - friction coefficient between the soil and spade; ρ - soil voluetric weight, [N/ 3 ]; a, b - excavated soil slice size, []; ψ - angle of attack of the spade, [º]; z - nuber of spades; ω - angular speed of the crankshaft, [rad/s]; B - working width of the achine, []; v x - coponent of the relative speed to the direction of advance of the achine, [/s], [7]. In equation () are soe eleents for which there is insufficient data, such as the angle of attack of the spade ψ; forward direction coponent of velocity of a spade, v x. This data is established by theoretical calculations and graphical deterinations. For the theoretical study of the angle of attack a atheatical odel is built achieving: ψ = π θ = arccos α = ϕ ( θ ) ϕ ( θ r r r3 r4 r r4 cos θ r sin θ o (3) arctg α [ ], r r r r r cos θ r4 r cos θ 4 4 ) α = where: θ is the angle of the rotation of the leading eleent of the quadrilateral echanis of the digging achine; θ - angle of rotation of the driven eleent; α - constant
3 Brătucu, Gh.: Matheatical Model of the Energetic Consuption for Soil Digging Machines 45 angle fro the built; φ, φ - angles dependent on the angle θ ; r, r, r 3, r 4 - rectangle side length echanis. Angle of attack of the spade during work tie varies as the angle of rotation of the crankshaft is also variable in tie according to the relation: θ = ϖ t. The ediu value of the angle of attack is deterined graphically for the specific case of soil digging achine MSS-, 40. Diensions of the rectangular echanis of the achine MSS-, 40 are: r = 0.7 ; r = 0.35 ; r 3 = 0.6 ; r 4 = 0.40, α = 8. The variation of the angle of attack of the spade is shown in Figure. In deterining the average coponent tg ψ during digging the deterination of the rotation angle range in which the actual digging is ade is necessary. Figure 3 shows the trajectory of the top of the spade and deterines this interval graphically. Fro the graphics presented we can see that the range of crankshaft rotation angle in which the digging is executed is between T, T being the period of otion, which in this case is 360. Thus, while digging tg ψ average is equal to: tg ψ ed = 0.6. The ediu value of sin ψ cos ψ is considered: sin ψ ed cos ψ ed = Fig. 3. Trajectory of the top of the spade Fig.. Variation of the spades angle of attack depending on the angle of the crankshafts rotation Substituting the average values of coponents, deterined graphically, the relationship of total energy consuption of the work of the soil with the digging achine, one gets: E ts µ ρ g a b ϖ s = f Gs v s z v s 0.45 π B a ρ v ( 4.37) π s 0.6 a B ρ g v ϖ s E loss [J]. (5) Matheatical odel of energy consuption of the work of the soil with the digging achine, expressed by equation (5), provides inforation necessary to optiize achine paraeters to iniize its energy consuption. Energy necessary for the oveent of the soil digging achine, E oveent, is transfored into echanical work necessary for the oveent of the achine and in echanical work of deforation of the soil and of the transport wheels. G s is directly proportional to the weight of the achine and rolling resistance coefficient f
4 46 Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II between the transportation wheel and soil: E = f f, G ). oveent ( s Reducing energy consuption for hauling the soil digging achine is to reduce these two eleents. Weight reduction of the achine starting fro the design and construction phase ay be obtained by using lighter aterials, but adequate in ters of resistance to echanical stress. The coponent of forward otion of the speed of the spade v x is deterined graphically for the case β = 0. The variation of the coponent of the speed of spade on the otion direction v x is shown in Figure 4. Fig. 4. Variation of the speed coponents of the spade during advancing direction Fro the chart presented results that the average speed of the spade during digging is equal to: v x = 4.37 [/s]. Reducing rolling resistance coefficient can be provided by using wheels with diaeters and widths as high as possible, with low tire pressure. Mechanical energy necessary to carry out operations, E cut and E trow is used to cut, deployent and disposal of soil slice. Energy required to cut and slice the soil displaceent depends on the diensions of the displaceent of the soil, being directly proportional to the depth and width of the spade so the nuber of spades in the soil at a tie and physical and echanical properties of soil, naely: E cut = f (a, b, z, µ, ρ). The energy for throwing the slices deployed depends on the diensions of the displaced soil and physical properties of the processed soil: E throw = f (a, B, ρ). Reduction of the energy required by the echanical spading operations ay be achieved by reducing the chip size of the displaced soil by doing the work once the soil has optiu physical and echanical properties in ters of work. Energy consued for self pushing, E push, occurs due to friction between the spade and the soil. It is an inconvenience which anifests itself by converting echanical energy of rotation received fro the tractor P.T.O for self pushing. Energy consued for this is directly proportional to the depth of work, width of the spade, forward speed, but inversely proportional to the rotational speed of the crankshaft: E push = f (a, b, ρ, v, /ω). It is indicated that forward speed be saller than the coponent of the speed of the spade in the direction of advance, which is confired in the specific case studied. Fig. 5. Slice diensions of soil displaced by the digging achine
5 Brătucu, Gh.: Matheatical Model of the Energetic Consuption for Soil Digging Machines 47 Energy consued by transission loss due to friction occurring in achine echaniss. The reduction of loss can be achieved by reducing the oving bodies and by reducing friction through lubrication. Specific cutting surface is a geoetrical paraeter of the displaced soil slices []. It is the ratio of the cutting surface of the soil displaced and its volue: St Ssp = V [ / 3 ], (6) where: S t cut surface of the displaced soil, in ; V - volue of soil displaceent in 3. The cut surface of the displaced soil is calculated fro the geoetry shown in Figure 5, such as: S = S t CBFG S EFGH S ABFE a b b s a s [ ], (7) the concrete conditions of work, b = 0. ; v = 0.3 /s; ω = 6 rad/s (Figure 6). Fig. 6. Influence of working depth on the variation of specific cutting surface of soil work with the digging achine Cutting surface area decreases with increasing work rate, which is observed fro the diagra drawn for the concrete conditions of work: a = 0.3, b = 0., ω = 6 rad/s (Figure 7). where notations correspond to those in Figure 5 and have the following eanings: a working depth in ; b - thickness of the slice at the surface of the soil, in ; s - the step of the achine in. Step of the achine is calculated: π s = v []. (8) ϖ Dislocated soil volue by a spade can be considered equal with: V = s a b [ 3 ]. (9) Substituting relations (7) and (9) in the forula of the specific cutting surface forula is obtained: S sts ω = [ / 3 ]. (0) π v a b Cutting surface area is inversely proportional to increasing working depth, which is observed fro the diagra drawn for Fig. 7. Influence of work speed on the variation of specific cutting surface of the work of the soil with digging achine Specific cutting surface is inversely proportional to the increase of the width of spades, which is observed fro the diagra drawn for the concrete conditions of work, a = 0.3, v = 0.3 /s, ω = 6 rad/s (Figure 8). Specific echanical work is the work needed for the deployent of the unit volue of soil, J/ 3. The specific echanical work in working of the soil by the digging achine is calculated reporting the echanical work done on a rotation of the crankshaft to the volue of soil displaced in a rotation, is:
6 48 Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II P rot - crankshaft rotation required power in W; τ - tie of a rotation, period of the crankshaft rotary otion, in s. 3. Results and Discussions Moveent during rotation is calculated as: Fig. 8. Influence of the width of the spades on the variation of the specific cutting surface in working the soil with the digging achine L L P τ rot rot ss = = [J], () Vrot Vrot where: L rot is the echanical work done by the digging achine at a rotation of the achine shaft in J; V rot - volue of soil displaced in a rotation of the rotor shaft, in 3 ; π τ = [rad/s]. () ω Dislocated soil volue to a rotation of the crankshaft is calculated with: V rot = s a B [ 3 ], (3) where B is the width of the digging achine, in. Crankshaft rotation power required is calculated as: µ ρ g a b v ω t B a ρ v vx rot = f Gs v z R sin P sinψ cosψ π ψ v [W]. (4) Making substitutions in equation () the forula of specific echanical work changes in: L s ss = x f G a B µ ρ g a b z ρ v B sin ψ cosψ π ρ g tg ψ v ϖ [J/ 3 ]. (5) In equation (5) notations correspond to those of equation (). Relationship (5) provides inforation on factors that influence specific echanical work and also on the energy consuption of the digging work. Working depth, working speed, width of spades influences the specific echanical work of the soil with digging achine with the soil. To study the influence of each factor, in the theoretical part are considered the concrete conditions of theoretical study as: f = 0.5, G s = 600 N, ρ = 500 kg/ 3, µ = 0.36 between soil and steel; tg ψ ed = 0.6; ω = 7 rad/s; B =.4 ; v xed = 4.37 /s; b = 0. ; z = 6; a = 0.3 ; v = 0.4 /s. Fro the graph shown in Figure 9 it results that the depth variation is inversely proportional to the variation of echanical work specifically. With increasing depth, occurs the decrease of the echanical work needed in the processing of the unit volue of soil by digging. Fro the graphics shown in Figures 0, results that by increasing the working speed and width of the spades results an increase in the necessary echanical work needed for processing the unit volue of the soil by digging.
7 Brătucu, Gh.: Matheatical Model of the Energetic Consuption for Soil Digging Machines 49 Fig. 9. Influence of the depth of working on specific echanical work of digging achine with the soil The energetic optiization possibility application on the soil digging work based on the atheatical odeling ade in this paper presuppose the collaboration between designers and anufactures for soil digging technical equipents, but also a superior training of the agriculture operators. These ust assure optial adjustent for technical syste oveent speed concordant to physicalcheical soil characteristics, to existent grass quantity etc. Through applying the research results obtained by the atheatical odeling proposed in this paper a contribution can be brought to the achieveent of soe agricultural works of superior quality in optial econoical conditions. 4. Conclusions Fig. 0. Influence of work speed on specific echanical work of digging achine with the soil Fig.. Influence of the width of the spades on the specific echanical work of the soil with the digging achine Using the soil digging achine in preparing the gerination bed in greenhouses is justified in working the soil at greater depths but with lower work speed. The digging achine which has wide spades requires a larger aount of echanical work for the unit volue of the soil processed. Conclusion that refers to the width of the spades is benefic when. Designing the achine or when purchasing it, it can serve as basis for decision. The reduced diensions of the deployed slices of the soil lead to higher specific surfaces, at the sae tie high energy consuption in working of the soil by digging achine. Higher working speeds result in high advances at oving forward, so big slices are deployed, reducing the energy required for processing by digging of the soil. Using the soil digging achine for preparation of the gerination bed in greenhouses is justified through the working of the soil at greater depths.
8 50 Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II References. Brătucu, Gh.: Agricultural Technologies. Braşov. Transilvania University Publishing House, Drunek, L.J.: Researches on the Energy Optiization of the Preparation Works of the Gerination Bed in Greenhouses. In: Ph.D. Thesis, Transilvania University of Braşov, Ros, V., et al.: Matheatical Model for Energetically Analysis of the Soil Work Process. In: Trans Agra Tech Conference, Cluj-Napoca, 7-8 October 998, p Rus, Fl.: Machines for Soil Works, Sowing and Crop Maintenance, Braşov. Transilvania University Publishing House, Şandru, A., at al.: Energetic Consuption Reduction through Rational Using of the Agricultural Aggregate. Craiova. Scrisul Roanesc Publishing House, Toa, D., et al.: Econoic Use of the Energy in Agricultural Mechanization. Bucureşti. Ceres Publishing House, Voican, V., Lăcătuş, V.: The Protected Cultivation of the Vegetables in Greenhouses and Solarius. Bucureşti. Ceres Publishing House, 004.
THE EFFECT OF SOLID PARTICLE SIZE UPON TIME AND SEDIMENTATION RATE
Bulletin of the Transilvania University of Braşov Series II: Forestry Wood Industry Agricultural Food Engineering Vol. 5 (54) No. 1-1 THE EFFECT OF SOLID PARTICLE SIZE UPON TIME AND SEDIMENTATION RATE
More informationOPTIMIZATION OF SPECIFIC FACTORS TO PRODUCE SPECIAL ALLOYS
5 th International Conference Coputational Mechanics and Virtual Engineering COMEC 2013 24-25 October 2013, Braşov, Roania OPTIMIZATION OF SPECIFIC FACTORS TO PRODUCE SPECIAL ALLOYS I. Milosan 1 1 Transilvania
More informationME Machine Design I. FINAL EXAM. OPEN BOOK AND CLOSED NOTES. Friday, May 8th, 2009
ME 5 - Machine Design I Spring Seester 009 Nae Lab. Div. FINAL EXAM. OPEN BOOK AND LOSED NOTES. Friday, May 8th, 009 Please use the blank paper for your solutions. Write on one side of the paper only.
More informationChapter 2: Introduction to Damping in Free and Forced Vibrations
Chapter 2: Introduction to Daping in Free and Forced Vibrations This chapter ainly deals with the effect of daping in two conditions like free and forced excitation of echanical systes. Daping plays an
More informationULTRASONIC WELDING OF COMPOSITE MATERAILS. ULTRASONIC BOOSTER DESIGN AND FEM SIMULATION
ULTRASONIC WELDING OF COMPOSITE MATERAILS. ULTRASONIC BOOSTER DESIGN AND FEM SIMULATION Gh. AMZA, Zoia Apostolescu, Dan NITOI University Politehnica fro Bucharest, aza@aza.cais.pub.ro Keywords: ultrasonic,
More informationActuators & Mechanisms Actuator sizing
Course Code: MDP 454, Course Nae:, Second Seester 2014 Actuators & Mechaniss Actuator sizing Contents - Modelling of Mechanical Syste - Mechaniss and Drives The study of Mechatronics systes can be divided
More informationNUMERICAL MODELLING OF THE TYRE/ROAD CONTACT
NUMERICAL MODELLING OF THE TYRE/ROAD CONTACT PACS REFERENCE: 43.5.LJ Krister Larsson Departent of Applied Acoustics Chalers University of Technology SE-412 96 Sweden Tel: +46 ()31 772 22 Fax: +46 ()31
More informationWIRELESS DRIVE OF PIEZOELECTRIC COMPONENTS SATYANARAYAN BHUYAN 2011
WIRELESS DRIVE OF PIEZOELECTRIC COMPONENTS SATYANARAYAN BHUYAN 011 WIRELESS DRIVE OF PIEZOELECTRIC COMPONENTS SATYANARAYAN BHUYAN SCHOOL OF ELECTRICAL & ELECTRONIC ENGINEERING 011 SATYANARAYAN BHUYAN WIRELESS
More informationChapter 1: Basics of Vibrations for Simple Mechanical Systems
Chapter 1: Basics of Vibrations for Siple Mechanical Systes Introduction: The fundaentals of Sound and Vibrations are part of the broader field of echanics, with strong connections to classical echanics,
More informationModel Fitting. CURM Background Material, Fall 2014 Dr. Doreen De Leon
Model Fitting CURM Background Material, Fall 014 Dr. Doreen De Leon 1 Introduction Given a set of data points, we often want to fit a selected odel or type to the data (e.g., we suspect an exponential
More information2.003 Engineering Dynamics Problem Set 2 Solutions
.003 Engineering Dynaics Proble Set Solutions This proble set is priarily eant to give the student practice in describing otion. This is the subject of kineatics. It is strongly recoended that you study
More informationAiMT Advances in Military Technology
AiT Advances in ilitary Technology Vol. 14, No. 1 (2019), pp. 47-57 ISSN 1802-2308, eissn 2533-4123 DOI 10.3849/ait.01247 odelling issile Flight Characteristics by Estiating ass and Ballistic Paraeters
More information2.141 Modeling and Simulation of Dynamic Systems Assignment #2
2.141 Modeling and Siulation of Dynaic Systes Assignent #2 Out: Wednesday Septeber 20, 2006 Due: Wednesday October 4, 2006 Proble 1 The sketch shows a highly siplified diagra of a dry-dock used in ship
More informationIn the session you will be divided into groups and perform four separate experiments:
Mechanics Lab (Civil Engineers) Nae (please print): Tutor (please print): Lab group: Date of lab: Experients In the session you will be divided into groups and perfor four separate experients: (1) air-track
More informationREDUCTION OF FINITE ELEMENT MODELS BY PARAMETER IDENTIFICATION
ISSN 139 14X INFORMATION TECHNOLOGY AND CONTROL, 008, Vol.37, No.3 REDUCTION OF FINITE ELEMENT MODELS BY PARAMETER IDENTIFICATION Riantas Barauskas, Vidantas Riavičius Departent of Syste Analysis, Kaunas
More information2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL
(Del I, teori; 1 p.) 1. In fracture echanics, the concept of energy release rate is iportant. Fro the fundaental energy balance of a case with possible crack growth, one usually derives the equation where
More informationXI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com
XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.co https://prootephysics.wordpress.co [MOTION] CHAPTER NO. 3 In this chapter we are going to discuss otion in one diension in which we
More informationDESIGN OF THE DIE PROFILE FOR THE INCREMENTAL RADIAL FORGING PROCESS *
IJST, Transactions of Mechanical Engineering, Vol. 39, No. M1, pp 89-100 Printed in The Islaic Republic of Iran, 2015 Shira University DESIGN OF THE DIE PROFILE FOR THE INCREMENTAL RADIAL FORGING PROCESS
More information8.1 Force Laws Hooke s Law
8.1 Force Laws There are forces that don't change appreciably fro one instant to another, which we refer to as constant in tie, and forces that don't change appreciably fro one point to another, which
More informationCinematic and Kinetic Analyses of the Slider-Crank Mechanism in Engine of MF-285 Tractor
Australian Journal of Basic and Applied Sciences, 5(12): 3112-3121, 2011 ISSN 1991-8178 Cineatic and Kinetic Analyses of the Slider-Crank Mechanis in Engine of MF-285 Tractor 1 Mohaad Reza Asadi, 1 Heidar
More informationAt the end of this lesson, the students should be able to understand
Instructional Objectives At the end of this lesson, the students should be able to understand Power screw echanis. The thread fors used in power screws. Torque required to raise and lower a load in a power
More informationAn Approximate Model for the Theoretical Prediction of the Velocity Increase in the Intermediate Ballistics Period
An Approxiate Model for the Theoretical Prediction of the Velocity... 77 Central European Journal of Energetic Materials, 205, 2(), 77-88 ISSN 2353-843 An Approxiate Model for the Theoretical Prediction
More informationForecasting Financial Indices: The Baltic Dry Indices
International Journal of Maritie, Trade & Econoic Issues pp. 109-130 Volue I, Issue (1), 2013 Forecasting Financial Indices: The Baltic Dry Indices Eleftherios I. Thalassinos 1, Mike P. Hanias 2, Panayiotis
More informationReading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.
PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction
More informationBlock designs and statistics
Bloc designs and statistics Notes for Math 447 May 3, 2011 The ain paraeters of a bloc design are nuber of varieties v, bloc size, nuber of blocs b. A design is built on a set of v eleents. Each eleent
More informationAbout the definition of parameters and regimes of active two-port networks with variable loads on the basis of projective geometry
About the definition of paraeters and regies of active two-port networks with variable loads on the basis of projective geoetry PENN ALEXANDR nstitute of Electronic Engineering and Nanotechnologies "D
More informationIDENTIFICATION OF STABILITY OF CONCRETE TUNNEL LINING USING COUPLED MODELING
IDENTIFICATION OF STABILITY OF CONCRETE TUNNEL LINING USING COUPLED MODELING Kaila Weiglová, Technical University in Brno, Institute of Geoechanics, Brno, Czech Republic Petr Procházka*, Czech Association
More informationKinetic Theory of Gases: Elementary Ideas
Kinetic Theory of Gases: Eleentary Ideas 17th February 2010 1 Kinetic Theory: A Discussion Based on a Siplified iew of the Motion of Gases 1.1 Pressure: Consul Engel and Reid Ch. 33.1) for a discussion
More informationLecture #8-3 Oscillations, Simple Harmonic Motion
Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.
More informationKinetic Theory of Gases: Elementary Ideas
Kinetic Theory of Gases: Eleentary Ideas 9th February 011 1 Kinetic Theory: A Discussion Based on a Siplified iew of the Motion of Gases 1.1 Pressure: Consul Engel and Reid Ch. 33.1) for a discussion of
More informationNational 5 Summary Notes
North Berwick High School Departent of Physics National 5 Suary Notes Unit 3 Energy National 5 Physics: Electricity and Energy 1 Throughout the Course, appropriate attention should be given to units, prefixes
More informationCONTRIBUTIONS TO ULTRASONIC WELDING OF INTELLIGENT COMPOSITE MATERIALS USED IN VEHICLE MANUFACTURING
The 4th International Conference Advanced Coposite Materials Engineering COMAT 01 18-0 October 01, Brasov, Roania CONTRIBUTIONS TO ULTRASONIC WELDING OF INTELLIGENT COMPOSITE MATERIALS USED IN VEHICLE
More informationMassachusetts Institute of Technology Quantum Mechanics I (8.04) Spring 2005 Solutions to Problem Set 4
Massachusetts Institute of Technology Quantu Mechanics I (8.04) Spring 2005 Solutions to Proble Set 4 By Kit Matan 1. X-ray production. (5 points) Calculate the short-wavelength liit for X-rays produced
More informationFeature Extraction Techniques
Feature Extraction Techniques Unsupervised Learning II Feature Extraction Unsupervised ethods can also be used to find features which can be useful for categorization. There are unsupervised ethods that
More informationModern Control Systems (ECEG-4601) Instructor: Andinet Negash. Chapter 1 Lecture 3: State Space, II
Modern Control Systes (ECEG-46) Instructor: Andinet Negash Chapter Lecture 3: State Space, II Eaples Eaple 5: control o liquid levels: in cheical plants, it is oten necessary to aintain the levels o liquids.
More informationAnalysis of Impulsive Natural Phenomena through Finite Difference Methods A MATLAB Computational Project-Based Learning
Analysis of Ipulsive Natural Phenoena through Finite Difference Methods A MATLAB Coputational Project-Based Learning Nicholas Kuia, Christopher Chariah, Mechatronics Engineering, Vaughn College of Aeronautics
More informationOpen Access The Study on the Dynamic Multi-objective Recognition and Estimation Algorithm of Infrared Imaging Based on Particle Swarms Collaboration
Send Orders for Reprints to reprints@benthascience.ae 1400 The Open Autoation and Control Systes Journal, 014, 6, 1400-1404 Open Access The Study on the Dynaic Multi-objective Recognition and Estiation
More informationA Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair
Proceedings of the 6th SEAS International Conference on Siulation, Modelling and Optiization, Lisbon, Portugal, Septeber -4, 006 0 A Siplified Analytical Approach for Efficiency Evaluation of the eaving
More informationSupervised assessment: Modelling and problem-solving task
Matheatics C 2008 Saple assessent instruent and indicative student response Supervised assessent: Modelling and proble-solving tas This saple is intended to infor the design of assessent instruents in
More informationACCUMULATION OF FLUID FLOW ENERGY BY VIBRATIONS EXCITATION IN SYSTEM WITH TWO DEGREE OF FREEDOM
ENGINEERING FOR RURAL DEVELOPMENT Jelgava, 9.-.5.8. ACCUMULATION OF FLUID FLOW ENERGY BY VIBRATION EXCITATION IN YTEM WITH TWO DEGREE OF FREEDOM Maris Eiduks, Janis Viba, Lauris tals Riga Technical University,
More informationThe determination of values of the specific heat capacity of the selected thermal insulation materials used in track bed structure
The deterination of values of the specific heat capacity of the selected theral insulation aterials used in track bed structure Peter Dobeš 1,*, Libor Ižvolt 1, Martin Mečár 1, and Jana Malachová 2 1 University
More informationMagnetorheological Fluid for Levitation Migration Technology
66 The Open Materials Science Journal, 2011, 5, 66-71 Magnetorheological Fluid for Levitation Migration Technology Guang Yang * and ZhuPing Chen * Open Access Faculty of Mechanical Engineering, Jiei University,
More informationTactics Box 2.1 Interpreting Position-versus-Time Graphs
1D kineatic Retake Assignent Due: 4:32p on Friday, October 31, 2014 You will receive no credit for ites you coplete after the assignent is due. Grading Policy Tactics Box 2.1 Interpreting Position-versus-Tie
More informationWork, Energy and Momentum
Work, Energy and Moentu Work: When a body oves a distance d along straight line, while acted on by a constant force of agnitude F in the sae direction as the otion, the work done by the force is tered
More informationChapter 8 Deflection. Structural Mechanics 2 Dept of Architecture
Chapter 8 Deflection Structural echanics Dept of rchitecture Outline Deflection diagras and the elastic curve Elastic-bea theory The double integration ethod oent-area theores Conjugate-bea ethod 8- Deflection
More informationEasy Evaluation Method of Self-Compactability of Self-Compacting Concrete
Easy Evaluation Method of Self-Copactability of Self-Copacting Concrete Masanori Maruoka 1 Hiroi Fujiwara 2 Erika Ogura 3 Nobu Watanabe 4 T 11 ABSTRACT The use of self-copacting concrete (SCC) in construction
More informationComputer Model For Sieves Vibrations Analysis, Using an Algorithm Based on the False-Position Method
Aerican Journal of Applied Sciences 6 (): 48-56, 9 ISSN 546-939 9 Science Publications Coputer Model For Sieves Vibrations Analysis, Using an Algorith Based on the False-Position Method Dinu I. Stoicovici,
More informationSEISMIC SAFETY OF BRIDGE CRANE STEEL STRUCTURES OPERATING IN NPP
SEISMIC SAFETY OF BRIDGE CRANE STEEL STRUCTURES OPERATING IN NPP Kalin RADLOV*, Vesko PANOV** *University of Architecture, Civil Engineering and Geodesy Sofia, Bulgaria **Technical University Sofia, Bulgaria
More informationŞtefan ŞTEFĂNESCU * is the minimum global value for the function h (x)
7Applying Nelder Mead s Optiization Algorith APPLYING NELDER MEAD S OPTIMIZATION ALGORITHM FOR MULTIPLE GLOBAL MINIMA Abstract Ştefan ŞTEFĂNESCU * The iterative deterinistic optiization ethod could not
More informationDesign of 25 KA Current Injection Transformer Core with Finite Element Method
1 Design of 5 KA Current Injection Transforer Core ith Finite Eleent Method HOSSEIN HEYDARI, MOHSEN ARIANNEJAD, FARAMARZ FAGHIHI Iran University of Science and Technology, Tehran, Iran Abstract.Since Current
More informationNumerical Modeling of Self-Compacting Mortar Flow Using Discrete Element Method
Nuerical Modeling of Self-Copacting Flow Using Discrete Eleent Method - Technical Paper - Miansong HUANG *1, Xuehui AN *, Takayuki OBARA *3 and Masahiro OUCHI *4 ABSTRACT A nuerical odeling of Self-Copacting
More informationH Technical Reference
Reference H- H Reference... H-2 H-2 H-8 H-29... H-30... H-34... H-42... H-44 /... H-47... H-49 /... H-56 H- H-2 For Selecting a otor that satisfies the specifications required by your equipent is an iportant
More informationOptimization of Flywheel Weight using Genetic Algorithm
IN: 78 7798 International Journal o cience, Engineering and Technology esearch (IJET) Volue, Issue, March 0 Optiization o Flywheel Weight using Genetic Algorith A. G. Appala Naidu*, B. T.N. Charyulu, C..C.V.aanaurthy
More informationTribology in Industry. Friction and Wear Processes Thermodynamic Approach
Vol. 36, No. 4 (2014) 341 347 Tribology in Industry www.tribology.fink.rs RESEARCH Friction and Wear Processes Therodynaic Approach M. Banjac a, A. Vencl a, S. Otović a a University of Belgrade Faculty
More informationSPECIFICATIONS FOR OBTAINING MINIMUM DIMENSIONS OF THE PELTON WATER WHEEL, WHEN THE DEBIT AND FALL OF WATER HEAD ARE GIVEN
Scientific Bulletin of the Politehnica University of Tiisoara Transactions on echanics Special issue The 6 th International Conference on Hydraulic achinery and Hydrodynaics Tiisoara, Roania, October -,
More informationA DESIGN GUIDE OF DOUBLE-LAYER CELLULAR CLADDINGS FOR BLAST ALLEVIATION
International Journal of Aerospace and Lightweight Structures Vol. 3, No. 1 (2013) 109 133 c Research Publishing Services DOI: 10.3850/S201042862013000550 A DESIGN GUIDE OF DOUBLE-LAYER CELLULAR CLADDINGS
More informationBEF BEF Chapter 2. Outline BASIC PRINCIPLES 09/10/2013. Introduction. Phasor Representation. Complex Power Triangle.
BEF 5503 BEF 5503 Chapter BASC PRNCPLES Outline 1 3 4 5 6 7 8 9 ntroduction Phasor Representation Coplex Power Triangle Power Factor Coplex Power in AC Single Phase Circuits Coplex Power in Balanced Three-Phase
More informationQuestion number 1 to 8 carries 2 marks each, 9 to 16 carries 4 marks each and 17 to 18 carries 6 marks each.
IIT-JEE5-PH-1 FIITJEE Solutions to IITJEE 5 Mains Paper Tie: hours Physics Note: Question nuber 1 to 8 carries arks each, 9 to 16 carries 4 arks each and 17 to 18 carries 6 arks each. Q1. whistling train
More informationOSCILLATIONS AND WAVES
OSCILLATIONS AND WAVES OSCILLATION IS AN EXAMPLE OF PERIODIC MOTION No stories this tie, we are going to get straight to the topic. We say that an event is Periodic in nature when it repeats itself in
More informationBioTechnology. BioTechnology. An Indian Journal FULL PAPER KEYWORDS ABSTRACT
ISSN : 974-7435 Volue 8 Issue 1 BTAIJ, 8(1), 13 [135-133] The atheatic siulation of banana kick in football based on echanical odel Jia Yang College of Science, Jiangxi University of Science and Technology,
More informationSupport Vector Machine Classification of Uncertain and Imbalanced data using Robust Optimization
Recent Researches in Coputer Science Support Vector Machine Classification of Uncertain and Ibalanced data using Robust Optiization RAGHAV PAT, THEODORE B. TRAFALIS, KASH BARKER School of Industrial Engineering
More informationForce and dynamics with a spring, analytic approach
Force and dynaics with a spring, analytic approach It ay strie you as strange that the first force we will discuss will be that of a spring. It is not one of the four Universal forces and we don t use
More informationCOS 424: Interacting with Data. Written Exercises
COS 424: Interacting with Data Hoework #4 Spring 2007 Regression Due: Wednesday, April 18 Written Exercises See the course website for iportant inforation about collaboration and late policies, as well
More informationthe static friction is replaced by kinetic friction. There is a net force F net = F push f k in the direction of F push.
the static friction is replaced by kinetic friction. There is a net force F net = F push f k in the direction of F push. Exaple of kinetic friction. Force diagra for kinetic friction. Again, we find that
More informationIn this chapter we will start the discussion on wave phenomena. We will study the following topics:
Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical
More informationHomework 3 Solutions CSE 101 Summer 2017
Hoework 3 Solutions CSE 0 Suer 207. Scheduling algoriths The following n = 2 jobs with given processing ties have to be scheduled on = 3 parallel and identical processors with the objective of iniizing
More informationOn the characterization of non-linear diffusion equations. An application in soil mechanics
On the characterization of non-linear diffusion equations. An application in soil echanics GARCÍA-ROS, G., ALHAMA, I., CÁNOVAS, M *. Civil Engineering Departent Universidad Politécnica de Cartagena Paseo
More informationMonetary Policy Effectiveness in a Dynamic AS/AD Model with Sticky Wages
Monetary Policy Effectiveness in a Dynaic AS/AD Model with Sticky Wages H J Departent of Econoics University of Copenhagen Version 1.0, April 12, 2012 Teaching note for M.Sc. course on "Monetary Econoics:
More informationINTELLECTUAL DATA ANALYSIS IN AIRCRAFT DESIGN
INTELLECTUAL DATA ANALYSIS IN AIRCRAFT DESIGN V.A. Koarov 1, S.A. Piyavskiy 2 1 Saara National Research University, Saara, Russia 2 Saara State Architectural University, Saara, Russia Abstract. This article
More informationChapter 11: Vibration Isolation of the Source [Part I]
Chapter : Vibration Isolation of the Source [Part I] Eaple 3.4 Consider the achine arrangeent illustrated in figure 3.. An electric otor is elastically ounted, by way of identical isolators, to a - thick
More informationNew Linkage with Linear Actuator for Tracking PV Systems with Large Angular Stroke
744 CHINESE JOURNAL OF MECHANICAL ENGINEERING Vol. 24,aNo. 5,a20 DOI: 0.390/CJME.20.05.744, available online at www.cjenet.co; www.cjenet.co.cn New Linkage with Linear Actuator for Tracking PV Systes with
More information9 HOOKE S LAW AND SIMPLE HARMONIC MOTION
Experient 9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Objectives 1. Verify Hoo s law,. Measure the force constant of a spring, and 3. Measure the period of oscillation of a spring-ass syste and copare it
More informationANALYTICAL INVESTIGATION AND PARAMETRIC STUDY OF LATERAL IMPACT BEHAVIOR OF PRESSURIZED PIPELINES AND INFLUENCE OF INTERNAL PRESSURE
DRAFT Proceedings of the ASME 014 International Mechanical Engineering Congress & Exposition IMECE014 Noveber 14-0, 014, Montreal, Quebec, Canada IMECE014-36371 ANALYTICAL INVESTIGATION AND PARAMETRIC
More informationNow multiply the left-hand-side by ω and the right-hand side by dδ/dt (recall ω= dδ/dt) to get:
Equal Area Criterion.0 Developent of equal area criterion As in previous notes, all powers are in per-unit. I want to show you the equal area criterion a little differently than the book does it. Let s
More informationSetting Load Parameters for Viable Fatigue Testing of Gears in Powertrain Axles
Setting Load Paraeters for Viable Fatigue Testing of Gears in Powertrain Axles Part I: Single-Reduction Axles Ernő Fülöp This presentation introduces a new procedure that derived fro exact calculations
More informationModeling & Analysis of the International Space Station
Modeling & Analysis of the International Space Station 1 Physical Syste Solar Alpha Rotary Joints Physical Syste Rotor Stator Gear Train Solar Array Inboard Body Outboard Body +x Solar Array 3 Physical
More informationTutorial Exercises: Incorporating constraints
Tutorial Exercises: Incorporating constraints 1. A siple pendulu of length l ass is suspended fro a pivot of ass M that is free to slide on a frictionless wire frae in the shape of a parabola y = ax. The
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics Physics 115.3 MIDTERM TEST October 22, 2008 Tie: 90 inutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please
More informationPart I: How Dense Is It? Fundamental Question: What is matter, and how do we identify it?
Part I: How Dense Is It? Fundaental Question: What is atter, and how do we identify it? 1. What is the definition of atter? 2. What do you think the ter ass per unit volue eans? 3. Do you think that a
More informationGeneralized Rayleigh Wave Dispersion in a Covered Half-space Made of Viscoelastic Materials
Copyright 7 Tech Science Press CMC vol.53 no.4 pp.37-34 7 Generalized Rayleigh Wave Dispersion in a Covered Half-space Made of Viscoelastic Materials S.D. Akbarov and M. Negin 3 Abstract: Dispersion of
More informationDetermination of Cold Spot Location for Conduction-Heated Canned Foods Using an Inverse Approach
10 International Journal of Food Processing Technology, 015,, 10-17 Deterination of Cold Spot Location for Conduction-Heated Canned Foods Using an Inverse Approach Ibrahi O. Mohaed * Food Engineering Consultant,
More information= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12
Oscillation: the vibration of an object Oscillations and Waves Eaple of an Oscillating Syste A ass oscillates on a horizontal spring without friction as shown below. At each position, analyze its displaceent,
More informationWarning System of Dangerous Chemical Gas in Factory Based on Wireless Sensor Network
565 A publication of CHEMICAL ENGINEERING TRANSACTIONS VOL. 59, 07 Guest Editors: Zhuo Yang, Junie Ba, Jing Pan Copyright 07, AIDIC Servizi S.r.l. ISBN 978-88-95608-49-5; ISSN 83-96 The Italian Association
More informationOptimum Value of Poverty Measure Using Inverse Optimization Programming Problem
International Journal of Conteporary Matheatical Sciences Vol. 14, 2019, no. 1, 31-42 HIKARI Ltd, www.-hikari.co https://doi.org/10.12988/ijcs.2019.914 Optiu Value of Poverty Measure Using Inverse Optiization
More informationBALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass
BALLISTIC PENDULUM INTRODUCTION: In this experient you will use the principles of conservation of oentu and energy to deterine the speed of a horizontally projected ball and use this speed to predict the
More informationInternational Journal of Scientific & Engineering Research, Volume 5, Issue 7, July-2014 ISSN IJSER
International Journal of Scientific & Engineering Research, Volue 5, Issue 7, July-4 ISSN 9-558 74 Advanced Dynaics & Control Lab Dept. of Mech Engg. CET, Kerala, India rajanakash@gail.co Dept. of Mech
More informationSolidification of Porous Material under Natural Convection by Three Phases Modeling
Solidification of Porous Material under Natural Convection by Three Phases Modeling Hassan Basirat Tabrizi, Meber, IAENG and F. Sadeghpour Abstract The perforance of natural convective flow over a rectangular
More informationPrincipal Component Analysis Based Fault Detection and Diagnosis of Active Magnetic Bearing System
MIT International Journal of Mechanical Engineering, Vol. 5, No. 1, January 2015, pp. 01-05 1 Principal Coponent Analysis Based Fault Detection and Diagnosis of Active Magnetic Bearing Syste Mohaad Wasee
More informationSupplementary Information for Design of Bending Multi-Layer Electroactive Polymer Actuators
Suppleentary Inforation for Design of Bending Multi-Layer Electroactive Polyer Actuators Bavani Balakrisnan, Alek Nacev, and Elisabeth Sela University of Maryland, College Park, Maryland 074 1 Analytical
More informationQuestion 1. [14 Marks]
6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is
More informationABSTRACT INTRODUCTION
Wave Resistance Prediction of a Cataaran by Linearised Theory M.INSEL Faculty of Naval Architecture and Ocean Engineering, Istanbul Technical University, TURKEY A.F.MOLLAND, J.F.WELLICOME Departent of
More informationPattern Recognition and Machine Learning. Learning and Evaluation for Pattern Recognition
Pattern Recognition and Machine Learning Jaes L. Crowley ENSIMAG 3 - MMIS Fall Seester 2017 Lesson 1 4 October 2017 Outline Learning and Evaluation for Pattern Recognition Notation...2 1. The Pattern Recognition
More informationFUZZY PARAMETRIC GEOMETRIC PROGRAMMING WITH APPLICATION IN FUZZY EPQ MODEL UNDER FLEXIBILITY AND RELIABILITY CONSIDERATION
ISSN 1746-7659, England, UK Journal of Inforation and Coputing Science Vol. 7, No. 3, 1, pp. 3-34 FUZZY PARAMERIC GEOMERIC PROGRAMMING WIH APPLICAION IN FUZZY EPQ MODEL UNDER FLEXIBILIY AND RELIABILIY
More informationMonetary Policy E ectiveness in a Dynamic AS/AD Model with Sticky Wages
Monetary Policy E ectiveness in a Dynaic AS/AD Model with Sticky Wages Henrik Jensen Departent of Econoics University of Copenhagen y Version.0, April 2, 202 Teaching note for M.Sc. course on "Monetary
More informationExperimental Design For Model Discrimination And Precise Parameter Estimation In WDS Analysis
City University of New York (CUNY) CUNY Acadeic Works International Conference on Hydroinforatics 8-1-2014 Experiental Design For Model Discriination And Precise Paraeter Estiation In WDS Analysis Giovanna
More informationDesign and Experimental Research of Atomizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu WANG, Yin ZHEN, Juan SONG and A-chun ZHU
217 3rd International Conference on Applied Mechanics and Mechanical Autoation (AMMA 217) ISBN: 978-1-6595-479- Design and Experiental Research of Atoizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu
More informationSelf-Erecting Inverted Pendulum: Swing up and Stabilization Control
Self-Erecting Inverted Pendulu: Swing up and Stabilization Control S. McGilvray (Winner of the IEEE Life Meber ward for best paper fro the Central Canada Council for the IEEE Student Paper Contest, ) Contents
More informationMathematical Models to Determine Stable Behavior of Complex Systems
Journal of Physics: Conference Series PAPER OPEN ACCESS Matheatical Models to Deterine Stable Behavior of Coplex Systes To cite this article: V I Suin et al 08 J. Phys.: Conf. Ser. 05 0336 View the article
More informationLesson 24: Newton's Second Law (Motion)
Lesson 24: Newton's Second Law (Motion) To really appreciate Newton s Laws, it soeties helps to see how they build on each other. The First Law describes what will happen if there is no net force. The
More informationNumerical simulations of isotropic and die compaction of powder by the discrete element method
Nuerical siulations of isotropic and die copaction of powder by the discrete eleent ethod J-F. Jerier, B. Harthong, B. Chareyre, D. Ibault, F-V. Donzé & P. Doréus Laboratoire Sols, Solides, Structures,
More information