Slope stability study for optimum design of an opencast project

Size: px
Start display at page:

Download "Slope stability study for optimum design of an opencast project"

Transcription

1 Journal of Scientific & Industrial Research Vol. 65, January 2006, pp Slope stability study for optiu design of an opencast project V K Singh* Slope Stability Departent, Central Mining Research Institute, Dhanbad Received 05 July 2005; revised 13 Septeber 2005; accepted 27 October 2005 The stability of an opencast ine slope, investigated by the liit equilibriu ethod, indicates that 148 deep open pit is stable with 60 overall slope angle. Geotechnical apping was undertaken to deterine the critical orientation of structural discontinuities. Geoechanical properties were deterined in the laboratory and subsequently odified to approxiate those of in situ rock ass. Sensitivity analysis was done to deterine the influence of the slope design paraeters on the safety factor. It was also used in deterining the ost suitable reedial easure for the critical slope. Slope onitoring did not reveal any oveent in and around the pit. Keywords: Rock excavation, Safety analysis, Slope stability, Surface ining Introduction The geotechnical study and slope design was conducted of an open pit copper ine (500 long, 200 wide) situated in Rajasthan, India. The ore body is 40 wide and 313 long. The ultiate pit depth is 148. The ore body is striking NNW-SSE with an average dip of 65 due west. It swelled centrally and pinching towards south. Mineralization is confined to aphibole felspathic quartzite that is exposed towards the hangingwall. Footwall is characterised by felspathic quartzite. A dyke dipping at 80 towards hangingwall is also present in the pit (Fig. 1). Since the ineralized body is sall and steeply dipping, profitability of the ine is largely dependent on the steepest possible final slope angle. Earlier, the open pit was designed with 45 overall slope angle. Therefore, the ine anageent sought the study for an optiu slope design of the open pit. The rock discontinuities were apped at the exposed benches of the pit as per ISRM 1. Geotechnical Field Investigations Geotechnical apping, using detail line apping ethod, was carried in and around the partially developed open pit. The apping locations, arked as A, B, C and D (Fig. 1), were selected at different working levels of the footwall and the hangingwall side of the ine to represent the coplete rock ass fabric of the ine. *Tel: E-ail: vks_slope@yahoo.co The statistical analysis of the orientation data was done (Fig. 2) with "SNAP" coputer prograe 2. The ean orientations of the joint sets are alost siilar at all the four locations. Therefore, the orientation data of the four locations were grouped to represent the discontinuity orientation of the whole pit. The contour plot of the grouped data is shown in Fig. 2. The statistical analysis of the discontinuity data indicated the presence of four steeply dipping sets and a single sub-horizontal joint set (Table 1). The joints are oderately to widely spaced (20-90 c, ISRM 1 ). The spacing of the bedding plane is greater than 3 and the rock ass ay be described as assively bedded. The wide spacing of the joints contributes to a rock quality designation (RQD) rating in excess of 80 per cent. Discontinuity sets J1 and J2 ay be classed as systeatic joint sets. J3 and J4 are sub-systeatic and J5 is non-systeatic joint set (ISRM 1 ). J1, J2 and J3 joint sets can be said to have high persistence, being traceable to distances of 20 in the direction of dip. Attepts were ade to easure the roughness precisely in the field. Although only a few discontinuities could be found suitable for roughness easureent due to inaccessibility of large exposed discontinuity surface. The dip direction and dip aount were obtained with the help of Clar copass by putting 5, 10, 20 and 40 c dia circular discs at various positions over a few discontinuity surfaces 3. The effective large-scale roughness angle, easured fro 40 c circular disc 4, in the direction of potential sliding is 3 for the joints of aphibole felspathic quartzite and felspathic quartzite both. The joints are

2 48 J SCI IND RES VOL 65 JANUARY 2006 Fig. 1 Geological ap of the copper open pit Table 1 Mean orientation of joint seats (719 observations) Joint set Mean orientation of joint seats Dip direction Dip aount, degree J1 N011±07 82±3 J2 N338±07 82±5 J3 N100±10 81±5 J4 N219±18 24±8 J5 N273±08 81±6 sooth planar. The surface atching ethod is also being to estiate shear strength 5. The ajority of joints (>90%) are closed. A few open fractures observed in the field appear to be the result of blasting operation. A sall nuber of joint aperture are filled with siliceous aterial which is derived by the weathering of the parent rock. The lack of hydraulic channels within the rock ass, the presence of properly aintained surface drains and an annual rainfall of only 500 ean that the slopes of the open pit can be regarded as effectively drained. Rock type Table 2 Realistic value of friction angles Aphibole Felespathic Quartizite Laboratory deterined friction angle (φ r ) of saw cut saple ean Large scale ean field roughness angle (i) Realistic value of friction angle (φ r +i) ean Felspathic Quartizite Geotechnical Laboratory Investigations Scale effect that is associated with laboratory testing of shear strength of discontinuities ay be overcoe through easureent of the residual angle of friction in the laboratory Realistic estiate of the shear strength of discontinuities ay be ade by adding the residual friction angle, deterined in the laboratory, to the large scale roughness angle, which is easured in the field 14,15. Residual friction angles were deterined fro saw cut saples in a shear box apparatus and the values obtained were added to large-scale roughness angles (Table 2).

3 SINGH: SLOPE STABILITY STUDY FOR OPTIMUM DESIGN OF AN OPENCAST PROJECT 49 Table 3 Back analysis for friction angle of failed hangingwall slope Slope height = 20.0 Slope angle = 75 o Dip of failure plane = 55 o Rock density = 2.68 ton/ 3 Water density = 1.0 ton/ 3 ZW = 3.5 Tension crack depth = 7 HW = 10 F = 1 Friction angle for drained slope without tension crack = 55.0 o Friction angle for drained slope with tension crack = 55.0 o Friction angle for undrained slope with tension crack = 64.6 o Friction angle for undrained slope without tension crack = 61.6 o Back analysis for friction angle of failed footwall slope Slope height = 20.0 Slope angle = 75 o Dip of failure plane = 50 o Rock density = 2.62 ton/ 3 Water density = 1.0 ton/ 3 ZW = 4.0 Tension crack depth = 8 HW = 10 F = 1 Fig. 2 Density plot of grouped orientation data of the discontinuities by SNAP An assessent of the angles of friction so derived was verified by back analysis of two bench scale slope failures. It is necessary to estiate the effective cohesion of joint surfaces that had been obilized at the tie of failure to arrive at the angles of friction. After having coplete configuration of the failed slopes, firstly it was decided to back calculate the effective friction angle obilized during the failure (Table 3). This back analysis was done with the assuption that effective cohesion along the failure plane would have been zero. The values of friction angles (Table 3) are very high to that of the laboratory tested values (Table 2). So, it was considered that there would have been soe effective cohesion along the failure plane. Accordingly, the back analyses were done with possible cobination of friction angles and corresponding cohesion (Table 4); wide variation was observed in the effective cohesion values for a given value of friction angle for four different geoining conditions. This variation is ainly due to different groundwater condition. So, to get the best estiate of the effective cohesion and friction angle, it is essential to know the ost likely groundwater condition during the slope failure. Friction angle for drained slope without tension crack = 50.0 o Friction angle for drained slope with tension crack = 50.0 o Friction angle for undrained slope with tension crack = 58.7 o Friction angle for undrained slope without tension crack = 55.1 o ZW is depth of water is tension crack HW is depth of water in slope without tension crack F is factor of safety 1 t/ 3 = 9.81kN/ 3 The rocks of the copper open pit are well jointed with oderate spacing. The ine is located in sei arid region with average annual precipitation at about 50 c and is generally torrential resulting into a runoff fro the surface in excess of percolation. The topography of the area is hilly which enables quick run-off to the rainwater. The pit reains dry, except in the rainy season. Suitable surface drains are provided to divert the rainwater away fro the pit. These surface drains are properly aintained, especially in rainy season, to keep the effective. The presence of tension crack cannot be ruled out due to the presence of well-developed nearly vertical joint set J1. So, it was concluded that the applicable geoining condition for the copper open pit slope ight be regarded as "drained slope with tension crack".

4 50 J SCI IND RES VOL 65 JANUARY 2006 Table 4 Back analysis for cohesion of hangingwall slope Slope height = 20.0 Slope angle = 75 degree Dip of failure plane = 55 degree Rock density = 2.68 ton/ 3 Water density = 1.0 ton/ 3 ZW = 3.5 F = 1 Tension crack depth = 7 HW = 10 I C CC CCC CCCC φ Back analysis for cohesion of footwall slope Slope height = 20.0 Slope angle = 75 degree Dip of failure plane = 50 degree Rock density = 2.62 ton/ 3 Water density = 1.0 ton/ 3 ZW = 4.0 F = 1 Tension crack depth = 8 HW = 10 I C CC CCC CCCC φ ZW, HW and F as entioned is Table 6 C is cohesion for drained slope without tension crack (ton/ 2 ) CC is cohesion for drained slope with tension crack (ton/ 2 ) CCC is cohesion for undrained slope with tension crack (ton/ 2 ) CCCC is cohesion for drained slope without tension crack (ton/ 2 ) φ is friction angle. 1 ton/ 2 = 9.81 kpa After getting the best estiate of likely ground water and geoining condition, now it is possible to estiate the effective shear strength for the failed slopes. For 35 friction angle (Table 4), cohesive strength for the joint surface of aphibole felspathic quartzite is 4.88 ton/ 2 for drained slope with tension crack condition. For 33 friction angle, the cohesion coes to be 5.09 ton/ 2 for the joint surface of felspathic quartzite. These values for joint surfaces of both the rock types were considered to be the realistic and the sae were used for the slope design purpose. Residual friction angles (32 and 30 ) were adopted, as final friction angles during stability analysis, for the J4 joint set and bedding planes in the aphibole felspathic quartzite and felspathic quartzite rock ass due to the rearkable planarity of both types of structure. The considerable persistence of the bedding plane and J4 joint set in the dip direction led to the assignent of a zero value of cohesion for use in the stability analysis. The hoogeneity/heterogeneity of the rock ass, at different locations and also at different depths in the open pit, was deterined with two-way analysis of variance technique 16. The fractal ethod can also be used to easure the statistical hoogeneity 17. Extensive diaetrical point load testing with liited uniaxial copressive strength test were done at different depths on NX size borehole saples of both the rock types drilled at nine different locations of the open pit (Table 5). It was used to develop a relationship (Table 6) between pint load index (Is) and uniaxial copressive strength (σ c ). This relationship was used to deterine the copressive strength of the rock types at different depths of the boreholes to be used for two-way analysis of variance technique (Table 7). By coparing the estiated variance ratio for respective degree of freedo at 5% level of significance (Table 8), it was observed that the strength is not significantly varying at different location and depth of the pit. Rock type Aphibole feldspathic quartzite Table 5 Coparison of uniaxial copressive and point load test results Point load index Uniaxial copressive strength ton/ 2 ton/ 2 No. of saple Mean Standard No. of saples Mean Standard tested deviation tested deviation Feldspathic quartzite

5 SINGH: SLOPE STABILITY STUDY FOR OPTIMUM DESIGN OF AN OPENCAST PROJECT 51 Slope Design by Liit Equilibriu Method Liit equilibriu ethod is the ost widely accepted and coonly perfored design tool in slope engineering. Slope Design of Hangingwall Slope Kineatic test of hangingwall slope (Fig. 3) is to know the types of failure possible. The critical discontinuity ust lie within 20 of the slope face for plane failure to occur. Only the J1 joint set strikes approx parallel to the hangingwall slope face. The ean dip direction of J1 joint set is N011, which is Rock type Depth of saple (MRL) Table 6 Correlation between σ c and Is Aphibole feldspathic quartzite Rock type Ratio between σ c and Is oblique to the ean dip direction of the hangingwall slope face of N030 (Fig. 3). Structures with dip directions between N010 to N050 (i.e. within 20 of the slope face) were therefore analyzed with the use of the SNAP progra to deterine the nuber of joints with dips greater than 35, the condition for sliding to occur (Table 9). The ajority of joints dip between 45 and 90, but less than 8.7% of the 172 Table 7 Uniaxial copressive strength at different depth Mean uniaxial copressive strength, kg/c 2 Bore hole nuber CS-1 CS-5 CS-6 CS-7 CS-10 CS-11 CS-13 CS AFQ AFQ AFQ AFQ AFQ AFQ FQ AFQ FQ FQ AFQ ` 389 FQ AFQ FQ FQ FQ FQ FQ kg/c 2 = 98.1 kpa AFQ stands for aphibole fespathic quartizite. FQ stands for felspathic quartizite Correlation coefficient Feldspathic quartzite Aphibole feldspathic quartzite and feldspathic quartzite together Table 8 Suary of coputations for analysis of variance Source of variation Variation of bore holes Variation of depth Degree of freedo Su of squares Mean su of squares Estiated variance ratio F Tabulated variance ratio Interaction Residual Total 319

6 52 J SCI IND RES VOL 65 JANUARY 2006 Table 10 Factor of safety for hangingwall slope Overall slope height=148 Cohesion = 4.8 ton/ 2 Friction angle =35 0 Unit weight = 2.68 ton/ 2 Failure plane inclination Tension crack depth, F1 F2 F3 F4 60 o overall slope o overall slope Fig. 3 Kineatic analysis to know the types of failure Table 9 Dip ring analysis (172 observations) for hangingwall slope (18 ring of 5.0 degree each) Sr No Range, Nuber % joints in the range of dip directions, considered occur in the dip rings fro 40 to 60. However, the proportion of joints that daylight increases sharply in the dip range (Table 9). Furtherore, these joints have approx the sae strike and dip direction as the hangingwall slope face. F1 is factor of safety for slope with water up to half of the depth of the tension crack, F2 factor of safety for drained slope with tension crack, F3 factor of safety for drained slope without tension crack, F4 is factor of safety for slope with water up to half of the depth of slope, but without tension crack. If slope angle (> 60 ) is specified, the nuber of critical joints that could daylight in the slope face would be significant. The ain objective in the overall slope design is to iniize the risk of failure. Hence, it is iportant to iniise the nuber of potential failure planes that could daylight in a given slope. Plane failure analysis for overall slope was done to calculate the factor of safety for four different conditions (Table 10). The F2 condition (that of a drained slope with tension crack) was adopted as representative of the situation at the ine site (Table 10) because of the ine's location in a seiarid region and the potential for developent of tension cracks along the steeply dipping J1 joint set. A depth of 20 was assued for tension cracks in accordance with the observed persistence of the J1 set. A preliinary stability analysis indicated that joints with dips of less than 56 would be stable should they daylight in a hangingwall slope of 60 dip. So, detailed stability analysis with joint dip less than 56 was considered to be unnecessary. Siilarly it was judged that analyzing the stability of joints with dips greater than would be inappropriate as these joints would not daylight in a slope. So, it was decided to conduct stability analysis with 58 joint dip

7 SINGH: SLOPE STABILITY STUDY FOR OPTIMUM DESIGN OF AN OPENCAST PROJECT 53 Table 11 Dip ring analysis (75 observations) for footwall slope (18 rings of 5.0 degree each) Sr No Range, Nuber % Table 12 Factor of safety for footwall slope Overall slope height=77 Cohesion = 5.1t/ 2 Friction angle =33 0 Unit weight = 2.62 t/ 3 Failure plane inclination, Tension crack depth, 60 overall slope F1 F2 F3 F overall slope (the ost critical joint orientation) for an overall slope angle (60-65 ). The 60 hangingwall slope (drained slope with tension crack, F2 of Table 10) is stable with failure plane dipping at 58 with the available joint shear strength. The sae 60 slope becoes unstable with 55 joint dip (Table 10). Only 10 joints (5.8%) are having dip less than 58, which ay for critical plane failure geoetry (Table 10). As such, these few observations are not representative of the overall structure and also do not coe fro the sae area. At the sae tie, 65 slope becoes unstable with 55 and 58 joint inclinations both and critically stable with 63 joint dip with critical tension crack depth (Table 10). Hence, ore critical joints are exposed in 65 slope face. Therefore, 60 overall slope angle is a logical choice. Slope Design of Footwall Slope The kineatic analysis of footwall slope indicated that J5 is the only critical joint set for plane failure which has a dip direction of N270 (Fig. 3). A dip ring analysis revealed that only one joint is found to be dipping at less than 55 in the relevant range of dip directions of N250 -N290 (Table 11). However, about 9 percent joints are having dip between 60 and 65. Hence, it was decided once ore to carry out stability analysis with 58 joint dip, the ost critical orientation for a footwall slope angle in the range The single daylighting joint (Table 12) is stable in 60 footwall slope, because it is dipping at an angle (20-25 ) less than friction angle (33 ). However, the 65 slope is critically stable with few joints having inclination between 60 and 65. Hence, 60 pit slope angle is safe fro plane failure condition. Wedge Failure Analysis The kineatic analysis of the structural data indicated that the footwall and hangingwall slopes would be free of critical wedge geoetry (Fig. 3). Moreover, the etabasic dyke will not cause unstable condition because of its location in the iddle part of the pit, which will be reoved in the course of ining. At depth, the steeply dipping dyke is favourable oriented within the hangingwall slope and so would have no undesirable effect on slope stability. Sensitivity Analysis of Slopes The ain ai of sensitivity analysis was to deterine the influence of different paraeters on the safety factor. The decisive influence of water was observed in tension crack, in coparison to other paraeters, on safety factor (Fig. 4). The slopes are stable without water in tension crack with any cobination of cohesion and friction angle. Hence, the slope is stable in the ost likely geoining condition (drained slope with tension crack). For half

8 54 J SCI IND RES VOL 65 JANUARY 2006 Fig. 4 Sensitivity analysis for hangingwall slope Fig. 5 Sensitivity analysis for footwall slope water filled tension crack condition, the slope is stable only with cohesion greater than 5 ton/ 2. For fully suberged tension crack condition, the slope is only stable with cohesion greater than 6.5 ton/ 2. The available cohesive strength along joints ay decrease with tie due to weathering and the slope ay becoe unstable. Therefore, it is necessary to avoid any entry of water in tension crack and it's further extension to greater depth. Any visible tension crack should be filled with pereable aterial. Any ipereable aterial covers the top of the crack. The pereable aterial within the crack will allow ground water flow across the tension crack. The ipereable aterial at the top of tension crack will not allow surface water to enter within the crack. The suitably filled-up tension crack will change the condition fro "undrained slope with tension crack" to "undrained slope without tension crack". Half suberged slope without tension crack (Fig. 4) is stable even with the lowest values of cohesion and friction angle. For constant aterial properties of the sliding surface, an increase of the cohesion by 2.0 ton/ 2 causes an increase of safety factor by 0.39 (Fig. 4). The influence of the friction angle by contrast is saller. In this way, this sensitivity analysis is very useful for selecting a ore justified and suitable reedial easure. Proper drainage will influence the stability ost, and artificial reinforceent will also be beneficial to retain the axiu available shear strength of joints. The sensitivity analyses of footwall slope have also revealed the sae results (Fig. 5). Controlled Blasting A presplit blasting prograe was adopted in order to iprove the stability of the ultiate pit walls. Perfection of the presplitting at this site was achieved by conducting any experiental blasts in the ine (Table 13). The 150 dia vertical holes are drilled to the depth of Decoupled explosive charge (1 kg) was attached to the cordex at a spacing of 1 extending throughout the hole. Slurry explosive (8 kg, cartridge dia 50 ) is charged in each hole. To avoid an under fragented toe, an additional cartridge of 6.25 kg (125 ) is also placed at the botto of each hole (a total 14 kg explosive in each hole). Steing, kept to 1.8, is less than the noral. The presplit holes are drilled at 1.5 spacing. The next row of holes is drilled en echelon at a distance of 2.5 (burden), which is average back- Spacing Table 13 Paraeters for drilling Burden Depth of holes Height of bench Dia of hole Rearks O. B. drilling Ore drilling Pre-split drilling

9 SINGH: SLOPE STABILITY STUDY FOR OPTIMUM DESIGN OF AN OPENCAST PROJECT 55 Fig. 6 Working plan showing location of onitoring stations break of blast. A 4 spacing is kept between the holes. Another row of holes is drilled at distance of 3.5 (burden) with 4 spacing, which is the usual burden, and spacing of holes. The 150 dia vertical holes of the ain blast are charged at the rate of 0.75 kg/ 3. The total volue of rock break in a single blast is used to be about One long delay detonator (LDD) of 500.s. (p + sec) was connected between the presplit holes and the first hole of the production blast. The row of presplit holes is fired before the ain charge. The other holes of the production blast were subsequently fired with short delay detonator (SDD) of 25.s. The blasting results are excellent at the ine by keeping the above paraeters. After blasting, a sooth bench face is fored. Slope Monitoring A slope-onitoring prograe has subsequently been undertaken. The observation stations are located on the crest of the open pit and on in-pit benches. Monitoring stations have also been installed on 384 and 404 bers (Fig. 6). An electronic distance eter (Wild DI4L) and a precise level (Wild NA2) have been used to deterine displaceents of the rock ass. Till date, no oveent has been observed. Conclusions A new ethod was introduced to deterine the optiu discontinuity orientation and can also be used for optiu slope design. A correlation has been developed between point load index and uniaxial copressive strength. It is very useful during physical

10 56 J SCI IND RES VOL 65 JANUARY 2006 characterization of the slope aterial of any open pit. The two-way analysis of variance technique was successfully utilized for the first tie in the process of open pit slope design to deterine the heterogeneity/ hoogeneity of the slope aterial at different depths and at different locations of an open pit. The whole open pit was designed with the axiu 60 overall slope angle; before this geotechnical study, the open pit was designed at 45 overall slope angle. The height of the individual benches was 10 to 12. It is the steepest slope angle peritted by Directorate General of Mines Safety (DGMS) for 148 deep open pit ine (20 bench height) in India. Initially, 10 high benches are developed but at the pit liits two benches are joined together to ake ultiate bench height of 20. The open cast ining has been successfully copleted up to 148 depth. Acknowledgeents Author is grateful to Director, CMRI, Dhanbad, for giving perission to publish the paper. Author is also thankful to the ine anageent for providing all necessary inforation and facility during field study. References 1 ISRM, Suggested ethods for the quantitative description of discontinuities in rock asses, Coission on the Standardization of Laboratory and Field Tests in Rock Mechanics, Jeran P W & Mashey J R, A coputer progra for the stereographic analysis of coal fractures and cleats, United States Departent of the Interior, Bureau of ines, IC 8454, Hoek E & Bray J W, Rock Slope Engineering, 3rd edn (Inst Min Met, London) Fecker E & Rengers N, Measureent of large-scale roughness of rock planes by eans of profilograph and geological copass, Proc Int Sy Rock Fracture, Nancy, 1971, Zhao J, Joint surface atching and shear strength, J Rock Mech Min Sci, 34 (1997) Coulson J H, The effects of surface roughness on the shear strength of joints in rocks, Technical report MRD 270, Missouri river division, Corps of engineers, Oaha, Nebraska, Barton N, Review of a new shear strength criteria for rock joints, Eng Geo, 7 (1973) Hoek E & Londe P, The design of rock slopes and foundations, General report 3rd Cong ISRM, Denver, Barton N & Choubey V, The shear strength of rock joints in theory and practice, Rock Mech, 10 (1977) McMahon B K, Soe practical considerations of the estiation of shear strength of joints and other discontinuities, Proc Int Syp Fundaentals of Rock Joints, Lulea, 1985, Bandis S C, Mechanical properties of rock joints, Proc Int Syp Rock Joints, Norway, 1990, Yu X & Vayssade B, Joint profiles and their roughness paraeters, Int J Rock Mech Min Sci & Geoech Abstr, 28 (1991) Huang S L, Oelgke S M & Speck RC, Applicability of fractal characterization and odelling to rock joint profiles, Int J Rock Mec Min Sci & Geoech Abstr, 29 (1992) Mohaad N, Reddish D J & Stace L R, The relation between in-situ and laboratory rock properties used in nuerical odelling, J Rock Mech Min Sci, 34 (1997) Hoek E & Brown E T, Practical estiates of rock ass strength, Int J Rock Mech Min Sci, 34 (998) Croxton F E, Cowden DJ & Klein S, Appllied General Statistics, 3rd edn (Prentice-Hall, New Delhi) 1982, Kulatilake P H S W, Fiedler R & Panda B B, Box fractal diension as a easure of statistical hoogeneity of jointed rock asses, Eng Geol, 48 (1997)

Uniaxial compressive stress strain model for clay brick masonry

Uniaxial compressive stress strain model for clay brick masonry Uniaxial copressive stress strain odel for clay brick asonry Heant B. Kaushik, Durgesh C. Rai* and Sudhir K. Jain Departent of Civil Engineering, Indian Institute of Technology Kanpur, Kanpur 208 016,

More information

Proc. of the IEEE/OES Seventh Working Conference on Current Measurement Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES

Proc. of the IEEE/OES Seventh Working Conference on Current Measurement Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES Proc. of the IEEE/OES Seventh Working Conference on Current Measureent Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES Belinda Lipa Codar Ocean Sensors 15 La Sandra Way, Portola Valley, CA 98 blipa@pogo.co

More information

DESIGN OF THE DIE PROFILE FOR THE INCREMENTAL RADIAL FORGING PROCESS *

DESIGN 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 information

Supplementary Information for Design of Bending Multi-Layer Electroactive Polymer Actuators

Supplementary 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 information

Extension of CSRSM for the Parametric Study of the Face Stability of Pressurized Tunnels

Extension of CSRSM for the Parametric Study of the Face Stability of Pressurized Tunnels Extension of CSRSM for the Paraetric Study of the Face Stability of Pressurized Tunnels Guilhe Mollon 1, Daniel Dias 2, and Abdul-Haid Soubra 3, M.ASCE 1 LGCIE, INSA Lyon, Université de Lyon, Doaine scientifique

More information

Experimental Design For Model Discrimination And Precise Parameter Estimation In WDS Analysis

Experimental 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 information

Non-Parametric Non-Line-of-Sight Identification 1

Non-Parametric Non-Line-of-Sight Identification 1 Non-Paraetric Non-Line-of-Sight Identification Sinan Gezici, Hisashi Kobayashi and H. Vincent Poor Departent of Electrical Engineering School of Engineering and Applied Science Princeton University, Princeton,

More information

Data-Driven Imaging in Anisotropic Media

Data-Driven Imaging in Anisotropic Media 18 th World Conference on Non destructive Testing, 16- April 1, Durban, South Africa Data-Driven Iaging in Anisotropic Media Arno VOLKER 1 and Alan HUNTER 1 TNO Stieltjesweg 1, 6 AD, Delft, The Netherlands

More information

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START Laboratory Section: Last Revised on Deceber 15, 2014 Partners Naes: Grade: EXPERIMENT 8 Electron Beas 0. Pre-Laboratory Work [2 pts] 1. Nae the 2 forces that are equated in order to derive the charge to

More information

8.1 Force Laws Hooke s Law

8.1 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 information

Easy Evaluation Method of Self-Compactability of Self-Compacting Concrete

Easy 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 information

National 5 Summary Notes

National 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 information

Simulation of Geomechanical Behavior during SAGD Process using COMSOL Multiphysics

Simulation of Geomechanical Behavior during SAGD Process using COMSOL Multiphysics Siulation of Geoechanical Behavior during SAGD Process using COMSOL Multiphysics X. Gong 1, R.Wan *2 Departent of Civil Engineering, University of Calgary, Calgary, Alberta, Canada. *Corresponding author:

More information

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta 1 USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS By: Ian Bloland, Augustana Capus, University of Alberta For: Physics Olypiad Weeend, April 6, 008, UofA Introduction: Physicists often attept to solve

More information

Settlement Estimations of Peat during Centrifuge Experiments

Settlement Estimations of Peat during Centrifuge Experiments Settleent Estiations of Peat during Centrifuge Experients Riccardo Cappa 1, Sauel Yniesta 2, Anne Lenitzer 3, Scott J. Brandenberg 4, Ali Shafiee 5 1 PhD Candidate, S.M.ASCE, University of California at

More information

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL

2. 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 information

Feature Extraction Techniques

Feature 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 information

Designing for the Road User. Maximum Spiral Transition Lengths

Designing for the Road User. Maximum Spiral Transition Lengths IPENZ Transportation Conference 11 October 2006 Queenstown, New Zealand Designing for the Road User Maxiu Spiral Transition Lengths K H M Weale Northern Region Technical Developent Leader MWH New Zealand

More information

Department of Building Science, Tsinghua University, Beijing , China

Department of Building Science, Tsinghua University, Beijing , China Supporting Inforation A SPME based C a -history ethod for easuring SVOC diffusion coefficients in clothing aterial Jianping Cao 1,, Ningrui Liu 1,, Yinping Zhang 1,,* 1 Departent of Building Science, Tsinghua

More information

Block designs and statistics

Block 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 information

Ph 20.3 Numerical Solution of Ordinary Differential Equations

Ph 20.3 Numerical Solution of Ordinary Differential Equations Ph 20.3 Nuerical Solution of Ordinary Differential Equations Due: Week 5 -v20170314- This Assignent So far, your assignents have tried to failiarize you with the hardware and software in the Physics Coputing

More information

Numerical Modeling of Self-Compacting Mortar Flow Using Discrete Element Method

Numerical 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 information

NUMERICAL MODELLING OF THE TYRE/ROAD CONTACT

NUMERICAL 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 information

Two Dimensional Consolidations for Clay Soil of Non-Homogeneous and Anisotropic Permeability

Two Dimensional Consolidations for Clay Soil of Non-Homogeneous and Anisotropic Permeability Two Diensional Consolidations for Clay Soil of Non-Hoogeneous and Anisotropic Pereability Ressol R. Shakir, Muhaed Majeed Thiqar University, College of Engineering, Thiqar, Iraq University of Technology,

More information

3D acoustic wave modeling with a time-space domain dispersion-relation-based Finite-difference scheme

3D acoustic wave modeling with a time-space domain dispersion-relation-based Finite-difference scheme P-8 3D acoustic wave odeling with a tie-space doain dispersion-relation-based Finite-difference schee Yang Liu * and rinal K. Sen State Key Laboratory of Petroleu Resource and Prospecting (China University

More information

Keywords: Estimator, Bias, Mean-squared error, normality, generalized Pareto distribution

Keywords: Estimator, Bias, Mean-squared error, normality, generalized Pareto distribution Testing approxiate norality of an estiator using the estiated MSE and bias with an application to the shape paraeter of the generalized Pareto distribution J. Martin van Zyl Abstract In this work the norality

More information

Ocean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers

Ocean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers Ocean 40 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers 1. Hydrostatic Balance a) Set all of the levels on one of the coluns to the lowest possible density.

More information

OBJECTIVES INTRODUCTION

OBJECTIVES INTRODUCTION M7 Chapter 3 Section 1 OBJECTIVES Suarize data using easures of central tendency, such as the ean, edian, ode, and idrange. Describe data using the easures of variation, such as the range, variance, and

More information

Use of 3D Laser Scanner Technology to Monitor Coal Pillar Deformation

Use of 3D Laser Scanner Technology to Monitor Coal Pillar Deformation University of Wollongong Research Online Coal Operators' Conference Faculty of Engineering and Inforation Sciences 2016 Use of 3D Laser Scanner Technology to Monitor Coal Pillar Deforation Radovan Kukutsch

More information

Grid performance models using Design of Experiments (DoE) methods

Grid performance models using Design of Experiments (DoE) methods Grid perforance odels using Design of Experients (DoE) ethods IEPC 25-139 Presented at the 29 th International Electric Propulsion Conference, Princeton University, October 31 Noveber, 25 Michael Tartz

More information

General Properties of Radiation Detectors Supplements

General Properties of Radiation Detectors Supplements Phys. 649: Nuclear Techniques Physics Departent Yarouk University Chapter 4: General Properties of Radiation Detectors Suppleents Dr. Nidal M. Ershaidat Overview Phys. 649: Nuclear Techniques Physics Departent

More information

EFFECT OF SURFACE ASPERITY TRUNCATION ON THERMAL CONTACT CONDUCTANCE

EFFECT OF SURFACE ASPERITY TRUNCATION ON THERMAL CONTACT CONDUCTANCE EFFECT OF SURFACE ASPERITY TRUNCATION ON THERMAL CONTACT CONDUCTANCE Fernando H. Milanez *, M. M. Yovanovich, J. R. Culha Microelectronics Heat Transfer Laboratory Departent of Mechanical Engineering University

More information

An Approximate Model for the Theoretical Prediction of the Velocity Increase in the Intermediate Ballistics Period

An 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 information

TEST OF HOMOGENEITY OF PARALLEL SAMPLES FROM LOGNORMAL POPULATIONS WITH UNEQUAL VARIANCES

TEST OF HOMOGENEITY OF PARALLEL SAMPLES FROM LOGNORMAL POPULATIONS WITH UNEQUAL VARIANCES TEST OF HOMOGENEITY OF PARALLEL SAMPLES FROM LOGNORMAL POPULATIONS WITH UNEQUAL VARIANCES S. E. Ahed, R. J. Tokins and A. I. Volodin Departent of Matheatics and Statistics University of Regina Regina,

More information

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2! Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In

More information

Model Fitting. CURM Background Material, Fall 2014 Dr. Doreen De Leon

Model 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 information

COS 424: Interacting with Data. Written Exercises

COS 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 information

Stress Increment Solution Charts for Soil Consolidation Analysis

Stress Increment Solution Charts for Soil Consolidation Analysis Global Journal of Researches in Engineering General Engineering Volue 1 Issue 4 Version Year 01 Type: Double Blind Peer Reviewed International Research Journal Publisher: Global Journals Inc. (USA) Online

More information

Modelling of damage in composite materials using interface elements

Modelling of damage in composite materials using interface elements 5 th European LS-DYNA Users Conference Coposites Modelling of daage in coposite aterials using interface eleents Authors: W.G. Jiang, Departent of Aerospace Engineering, University of Bristol S.R. Hallett,

More information

XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com

XI 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 information

Support Vector Machine Classification of Uncertain and Imbalanced data using Robust Optimization

Support 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 information

ANALYTICAL INVESTIGATION AND PARAMETRIC STUDY OF LATERAL IMPACT BEHAVIOR OF PRESSURIZED PIPELINES AND INFLUENCE OF INTERNAL PRESSURE

ANALYTICAL 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 information

SHEAR BEHAVIOUR OF JOINTED ROCK: A STATE OF ART

SHEAR BEHAVIOUR OF JOINTED ROCK: A STATE OF ART IGC 2009, Guntur, INDIA SHEAR BEHAVIOUR OF JOINTED ROCK: A STATE OF ART A.K. Shrivastava Lecturer, Department of Civil Engineering, Delhi College of Engineering, Delhi 110 042, India. E-mail: aksrivastava@dce.ac.in

More information

Chapter 11 Simple Harmonic Motion

Chapter 11 Simple Harmonic Motion Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion

More information

Research in Area of Longevity of Sylphon Scraies

Research in Area of Longevity of Sylphon Scraies IOP Conference Series: Earth and Environental Science PAPER OPEN ACCESS Research in Area of Longevity of Sylphon Scraies To cite this article: Natalia Y Golovina and Svetlana Y Krivosheeva 2018 IOP Conf.

More information

THERMAL ENDURANCE OF UNREINFORCED UNSATURATED POLYESTERS AND VINYL ESTER RESINS = (1) ln = COMPOSITES & POLYCON 2009

THERMAL ENDURANCE OF UNREINFORCED UNSATURATED POLYESTERS AND VINYL ESTER RESINS = (1) ln = COMPOSITES & POLYCON 2009 Aerican Coposites Manufacturers Association January 15-17, 29 Tapa, FL USA Abstract THERMAL ENDURANCE OF UNREINFORCED UNSATURATED POLYESTERS AND VINYL ESTER RESINS by Thore M. Klaveness, Reichhold AS In

More information

CHAPTER ONE. Physics and the Life Sciences

CHAPTER ONE. Physics and the Life Sciences Solution anual for Physics for the Life Sciences 2nd Edition by Allang Link download full: http://testbankair.co/download/solution-anual-forphysics-for-the-life-sciences-2nd-edition-by-allang/ CHAPTER

More information

A NEW APPROACH FOR CALCULATING AVERAGE CROSS SECTIONS IN THE UNRESOLVED ENERGY REGION

A NEW APPROACH FOR CALCULATING AVERAGE CROSS SECTIONS IN THE UNRESOLVED ENERGY REGION Nuclear Matheatical Coputational Sciences: A Century in Review, A Century Anew Gatlinburg, Tennessee, April 6-, 2003, on CD-ROM, Aerican Nuclear Society, LaGrange Park, IL (2003) A NEW APPROACH FOR CALCULATING

More information

BALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass

BALLISTIC 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 information

UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC STANDARDS

UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC STANDARDS Paper Published on the16th International Syposiu on High Voltage Engineering, Cape Town, South Africa, 2009 UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC

More information

Example A1: Preparation of a Calibration Standard

Example A1: Preparation of a Calibration Standard Suary Goal A calibration standard is prepared fro a high purity etal (cadiu) with a concentration of ca.1000 g l -1. Measureent procedure The surface of the high purity etal is cleaned to reove any etal-oxide

More information

Department of Physics Preliminary Exam January 3 6, 2006

Department of Physics Preliminary Exam January 3 6, 2006 Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.

More information

Some Perspective. Forces and Newton s Laws

Some Perspective. Forces and Newton s Laws Soe Perspective The language of Kineatics provides us with an efficient ethod for describing the otion of aterial objects, and we ll continue to ake refineents to it as we introduce additional types of

More information

Basic properties and weathering process of strong weathered granite

Basic properties and weathering process of strong weathered granite Japanese Geotechnical Society Special Publication The 6th Japan-China Geotechnical Syposiu Basic properties and weathering process of strong weathered granite Xirong Niu i, iv), Yanfang Sun ii, iii), Yangping

More information

Chapter 4: Hypothesis of Diffusion-Limited Growth

Chapter 4: Hypothesis of Diffusion-Limited Growth Suary This section derives a useful equation to predict quantu dot size evolution under typical organoetallic synthesis conditions that are used to achieve narrow size distributions. Assuing diffusion-controlled

More information

Spine Fin Efficiency A Three Sided Pyramidal Fin of Equilateral Triangular Cross-Sectional Area

Spine Fin Efficiency A Three Sided Pyramidal Fin of Equilateral Triangular Cross-Sectional Area Proceedings of the 006 WSEAS/IASME International Conference on Heat and Mass Transfer, Miai, Florida, USA, January 18-0, 006 (pp13-18) Spine Fin Efficiency A Three Sided Pyraidal Fin of Equilateral Triangular

More information

Inspection; structural health monitoring; reliability; Bayesian analysis; updating; decision analysis; value of information

Inspection; structural health monitoring; reliability; Bayesian analysis; updating; decision analysis; value of information Cite as: Straub D. (2014). Value of inforation analysis with structural reliability ethods. Structural Safety, 49: 75-86. Value of Inforation Analysis with Structural Reliability Methods Daniel Straub

More information

LAB MECH8.COMP From Physics with Computers, Vernier Software & Technology, 2003.

LAB MECH8.COMP From Physics with Computers, Vernier Software & Technology, 2003. LAB MECH8.COMP Fro Physics with Coputers, Vernier Software & Technology, 003. INTRODUCTION You have probably watched a ball roll off a table and strike the floor. What deterines where it will land? Could

More information

COULD A VARIABLE MASS OSCILLATOR EXHIBIT THE LATERAL INSTABILITY?

COULD A VARIABLE MASS OSCILLATOR EXHIBIT THE LATERAL INSTABILITY? Kragujevac J. Sci. 3 (8) 3-44. UDC 53.35 3 COULD A VARIABLE MASS OSCILLATOR EXHIBIT THE LATERAL INSTABILITY? Nebojša Danilović, Milan Kovačević and Vukota Babović Institute of Physics, Faculty of Science,

More information

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams Chapter 15 ewton s Laws #2: inds of s, Creating ree Body Diagras 15 ewton s Laws #2: inds of s, Creating ree Body Diagras re is no force of otion acting on an object. Once you have the force or forces

More information

Interactive Markov Models of Evolutionary Algorithms

Interactive Markov Models of Evolutionary Algorithms Cleveland State University EngagedScholarship@CSU Electrical Engineering & Coputer Science Faculty Publications Electrical Engineering & Coputer Science Departent 2015 Interactive Markov Models of Evolutionary

More information

DETERMINATION OF ADSORTION LAYERS ON SILICON SORPTION ARTIFACTS USING MASS COMPARISON

DETERMINATION OF ADSORTION LAYERS ON SILICON SORPTION ARTIFACTS USING MASS COMPARISON DETERMINATION OF ADSORTION LAYERS ON SILICON SORPTION ARTIFACTS USING MASS COMPARISON Unurbileg Daraa 2 1, Jin Wan Chung 1 and Sungjun Lee 1, Seung Na Park 1* 1 Korea Research Institute of Standards and

More information

ANALYSIS OF HALL-EFFECT THRUSTERS AND ION ENGINES FOR EARTH-TO-MOON TRANSFER

ANALYSIS OF HALL-EFFECT THRUSTERS AND ION ENGINES FOR EARTH-TO-MOON TRANSFER IEPC 003-0034 ANALYSIS OF HALL-EFFECT THRUSTERS AND ION ENGINES FOR EARTH-TO-MOON TRANSFER A. Bober, M. Guelan Asher Space Research Institute, Technion-Israel Institute of Technology, 3000 Haifa, Israel

More information

Estimation of Combined Wave and Storm Surge Overtopping at Earthen Levees

Estimation of Combined Wave and Storm Surge Overtopping at Earthen Levees May 008 Estiation of Cobined Wave and Stor Surge Overtopping at Earthen Levees by Steven A. Hughes PURPOSE: This Coastal and Hydraulics Engineering Technical Note (CHETN) provides epirical equations for

More information

Accuracy of the Scaling Law for Experimental Natural Frequencies of Rectangular Thin Plates

Accuracy of the Scaling Law for Experimental Natural Frequencies of Rectangular Thin Plates The 9th Conference of Mechanical Engineering Network of Thailand 9- October 005, Phuket, Thailand Accuracy of the caling Law for Experiental Natural Frequencies of Rectangular Thin Plates Anawat Na songkhla

More information

A Note on the Applied Use of MDL Approximations

A Note on the Applied Use of MDL Approximations A Note on the Applied Use of MDL Approxiations Daniel J. Navarro Departent of Psychology Ohio State University Abstract An applied proble is discussed in which two nested psychological odels of retention

More information

An Extension to the Tactical Planning Model for a Job Shop: Continuous-Time Control

An Extension to the Tactical Planning Model for a Job Shop: Continuous-Time Control An Extension to the Tactical Planning Model for a Job Shop: Continuous-Tie Control Chee Chong. Teo, Rohit Bhatnagar, and Stephen C. Graves Singapore-MIT Alliance, Nanyang Technological Univ., and Massachusetts

More information

SHAPE IDENTIFICATION USING DISTRIBUTED STRAIN DATA FROM EMBEDDED OPTICAL FIBER SENSORS

SHAPE IDENTIFICATION USING DISTRIBUTED STRAIN DATA FROM EMBEDDED OPTICAL FIBER SENSORS 16 H INERNAIONAL CONFERENCE ON COMPOSIE MAERIALS SHAPE IDENIFICAION USING DISRIBUED SRAIN DAA FROM EMBEDDED OPICAL FIBER SENSORS Mayuko Nishio*, adahito Mizutani*, Nobuo akeda* *he University of okyo Keywords:

More information

EFFECT OF WALL REINFORCEMENTS, APPLIED LATERAL FORCES AND VERTICAL AXIAL LOADS ON SEISMIC BEHAVIOR OF CONFINED CONCRETE MASONRY WALLS

EFFECT OF WALL REINFORCEMENTS, APPLIED LATERAL FORCES AND VERTICAL AXIAL LOADS ON SEISMIC BEHAVIOR OF CONFINED CONCRETE MASONRY WALLS EFFECT OF WALL REINFORCEMENTS, APPLIED LATERAL FORCES AND VERTICAL AXIAL LOADS ON SEISMIC BEHAVIOR OF CONFINED CONCRETE MASONRY WALLS 984 Koji YOSHIMURA 1, Kenji KIKUCHI 2, Masauki KUROKI 3, Lizhen LIU

More information

IMPROVEMENTS IN DESCRIBING WAVE OVERTOPPING PROCESSES

IMPROVEMENTS IN DESCRIBING WAVE OVERTOPPING PROCESSES IMPROVEMENS IN DESCRIBING WAVE OVEROPPING PROCESSES Steven Hughes 1, Christopher hornton 2, Jentsje van der Meer 3, and Bryon Scholl 4 his paper presents a new epirical relation for the shape factor in

More information

IDENTIFICATION OF STABILITY OF CONCRETE TUNNEL LINING USING COUPLED MODELING

IDENTIFICATION 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 information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #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 information

The ballistic pendulum

The ballistic pendulum (ta initials) first nae (print) last nae (print) brock id (ab17cd) (lab date) Experient 4 The ballistic pendulu In this Experient you will learn how to deterine the speed of a projectile as well as the

More information

DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION

DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION Masaki WAKUI 1 and Jun IYAMA and Tsuyoshi KOYAMA 3 ABSTRACT This paper shows a criteria to detect

More information

Analysis of ground vibration transmission in high precision equipment by Frequency Based Substructuring

Analysis of ground vibration transmission in high precision equipment by Frequency Based Substructuring Analysis of ground vibration transission in high precision equipent by Frequency Based Substructuring G. van Schothorst 1, M.A. Boogaard 2, G.W. van der Poel 1, D.J. Rixen 2 1 Philips Innovation Services,

More information

Ufuk Demirci* and Feza Kerestecioglu**

Ufuk Demirci* and Feza Kerestecioglu** 1 INDIRECT ADAPTIVE CONTROL OF MISSILES Ufuk Deirci* and Feza Kerestecioglu** *Turkish Navy Guided Missile Test Station, Beykoz, Istanbul, TURKEY **Departent of Electrical and Electronics Engineering,

More information

A DESIGN GUIDE OF DOUBLE-LAYER CELLULAR CLADDINGS FOR BLAST ALLEVIATION

A 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 information

Star Zinc Project Gravity Forward Modelling along 7 Profiles

Star Zinc Project Gravity Forward Modelling along 7 Profiles E A R T H M A P S C O N S U L T I N G Earthaps Consulting CC P.O.Box 267 Swakopund NAMIBIA www.earthapsconsulting.co kknupp@africaonline.co.na Star Zinc Project Gravity Forward Modelling along 7 Profiles

More information

REDUCTION OF FINITE ELEMENT MODELS BY PARAMETER IDENTIFICATION

REDUCTION 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 information

In this chapter, we consider several graph-theoretic and probabilistic models

In this chapter, we consider several graph-theoretic and probabilistic models THREE ONE GRAPH-THEORETIC AND STATISTICAL MODELS 3.1 INTRODUCTION In this chapter, we consider several graph-theoretic and probabilistic odels for a social network, which we do under different assuptions

More information

Torsion Experiment. Encoder #3 ( 3 ) Third encoder/disk for Model 205a only. Figure 1: ECP Torsion Experiment

Torsion Experiment. Encoder #3 ( 3 ) Third encoder/disk for Model 205a only. Figure 1: ECP Torsion Experiment Torsion Experient Introduction For the Torsion lab, there are two required experients to perfor and one extra credit assignent at the end. In experient 1, the syste paraeters need to be identified so that

More information

Kinetic Theory of Gases: Elementary Ideas

Kinetic 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 information

NUMERICAL MODELING AND EXPERIMENTAL VALIDATION OF SEISMIC UPLIFT PRESSURE VARIATIONS IN CRACKED CONCRETE DAMS

NUMERICAL MODELING AND EXPERIMENTAL VALIDATION OF SEISMIC UPLIFT PRESSURE VARIATIONS IN CRACKED CONCRETE DAMS 13 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-6, 24 Paper No. 1976 NUMERICAL MODELING AND EXPERIMENTAL VALIDATION OF SEISMIC UPLIFT PRESSURE VARIATIONS IN CRACKED CONCRETE

More information

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.

Reading 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 information

Vendetta Mining Announces Maiden Assay Results from the 2014 Zone 5 Drilling Program at the Pegmont Lead-Zinc Project

Vendetta Mining Announces Maiden Assay Results from the 2014 Zone 5 Drilling Program at the Pegmont Lead-Zinc Project FOR IMMEDIATE RELEASE February 10 th, 2015 (VTT2015 NR # 2) Vendetta Mining Announces Maiden Assay Results fro the 2014 Zone 5 Drilling Progra at the Pegont Lead-Zinc Project Vancouver, BC February 10,

More information

2002 University of Porto, Faculty of Engineering (FEUP)

2002 University of Porto, Faculty of Engineering (FEUP) Holberg H, Ahtila P. Drying phenoenon in a fixed bed under the bio fuel ulti stage drying. In: Oliveira A, Afonso C, Riffat S, editors. Proceedings of the st International Conference on Sustainable Energy

More information

DYNAMIC STRENGTH OF GRAVELY SAND WITH EMPHASIS ON THE EFFECT OF MEMBRANE COMPLIANCE

DYNAMIC STRENGTH OF GRAVELY SAND WITH EMPHASIS ON THE EFFECT OF MEMBRANE COMPLIANCE DYNAMIC STRENGTH OF GRAVELY SAND WITH EMPHASIS ON THE EFFECT OF MEMBRANE COMPLIANCE ABSTRACT: S.M. Haeri 1, M.R. Shakeri 2 and S.A. Shahcheraghi 3 1 Professor, School of Civil Engineering, Sharif University

More information

Ch 12: Variations on Backpropagation

Ch 12: Variations on Backpropagation Ch 2: Variations on Backpropagation The basic backpropagation algorith is too slow for ost practical applications. It ay take days or weeks of coputer tie. We deonstrate why the backpropagation algorith

More information

Hysteresis model for magnetic materials using the Jiles-Atherton model

Hysteresis model for magnetic materials using the Jiles-Atherton model Hysteresis odel for agnetic aterials using the Jiles-Atherton odel Predrag Petrovic Technical faculty Svetog Save 65 32 Cacak, pegi@ei.yu Nebojsa itrovic Technical faculty Svetog Save 65 32 Cacak, itar@tfc.tfc.kg.ac.yu

More information

U ms = U mf (gD c ) 0.5

U ms = U mf (gD c ) 0.5 Indian Journal of Cheical Technology Vol. 15, January 2008, pp.85-89 Prediction of iniu slugging velocity, bubbling bed index and range of bubbling fluidization in cylindrical and non-cylindrical gas-solid

More information

A Simple Regression Problem

A Simple Regression Problem A Siple Regression Proble R. M. Castro March 23, 2 In this brief note a siple regression proble will be introduced, illustrating clearly the bias-variance tradeoff. Let Y i f(x i ) + W i, i,..., n, where

More information

Experiment 2: Hooke s Law

Experiment 2: Hooke s Law COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance

More information

Qualitative Modelling of Time Series Using Self-Organizing Maps: Application to Animal Science

Qualitative Modelling of Time Series Using Self-Organizing Maps: Application to Animal Science Proceedings of the 6th WSEAS International Conference on Applied Coputer Science, Tenerife, Canary Islands, Spain, Deceber 16-18, 2006 183 Qualitative Modelling of Tie Series Using Self-Organizing Maps:

More information

Name Period. What force did your partner s exert on yours? Write your answer in the blank below:

Name Period. What force did your partner s exert on yours? Write your answer in the blank below: Nae Period Lesson 7: Newton s Third Law and Passive Forces 7.1 Experient: Newton s 3 rd Law Forces of Interaction (a) Tea up with a partner to hook two spring scales together to perfor the next experient:

More information

Warning System of Dangerous Chemical Gas in Factory Based on Wireless Sensor Network

Warning 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 information

1 The properties of gases The perfect gas

1 The properties of gases The perfect gas 1 The properties of gases 1A The perfect gas Answers to discussion questions 1A. The partial pressure of a gas in a ixture of gases is the pressure the gas would exert if it occupied alone the sae container

More information

Part I: How Dense Is It? Fundamental Question: What is matter, and how do we identify it?

Part 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 information

Intelligent Systems: Reasoning and Recognition. Perceptrons and Support Vector Machines

Intelligent Systems: Reasoning and Recognition. Perceptrons and Support Vector Machines Intelligent Systes: Reasoning and Recognition Jaes L. Crowley osig 1 Winter Seester 2018 Lesson 6 27 February 2018 Outline Perceptrons and Support Vector achines Notation...2 Linear odels...3 Lines, Planes

More information

Physically Based Modeling CS Notes Spring 1997 Particle Collision and Contact

Physically Based Modeling CS Notes Spring 1997 Particle Collision and Contact Physically Based Modeling CS 15-863 Notes Spring 1997 Particle Collision and Contact 1 Collisions with Springs Suppose we wanted to ipleent a particle siulator with a floor : a solid horizontal plane which

More information

Energy and Momentum: The Ballistic Pendulum

Energy and Momentum: The Ballistic Pendulum Physics Departent Handout -10 Energy and Moentu: The Ballistic Pendulu The ballistic pendulu, first described in the id-eighteenth century, applies principles of echanics to the proble of easuring the

More information