Modeling the Total Surface Area and Volume of Potholes on a Length of Road

Size: px
Start display at page:

Download "Modeling the Total Surface Area and Volume of Potholes on a Length of Road"

Transcription

1 Modeling the Total Sufae Aea and Volue of Potholes on a Length of oad S.A. Oke, M.S. * and O. Ajayi 1 Depatent of Mehanial Engineeing, Uniesity of Lagos, Nigeia. * E-ail: sa_oke@yahoo.o ASTACT Potholes ae essentials in ino oad epais. Infoation about thei total sufae aea and olue ae useful in pediting the tie spent on oad epais, whih inole light aintenane paties. In addition, ost infoation ay be oputed using these data. This pape pesents a atheatial odel fo ealuating the total sufae aea and olue of potholes on a length of oad. The poble of potholes is appoahed fo diffeent dietions. One pespetie elates to the wea aused by the atiities of as on the sufae of oads wheeby the ties of the as ae assued to be ubbing the sufae of the oad as it oes along the oad. The othe dietion is the effets of eosion by wate of the bituen in aeas whee aks and depessions ou. A thid dietion is in fo of pobabilities of ouene on the oad with aeage (assue) adius fo the potholes. Case studies ae deeloped whih illustates the patial signifiane f the odel foulated. It is enisaged that the wok would benefit the stakeholdes in oad anageent. (Keywods: aea, olue, total aea, sufae of a -D objet, thee diensional geoety, oad engineeing, aintenane, epai) INTODUCTION Tanspotation odes ae of thee ajo ategoies: land, ai, and wate. Howee, oad tanspot, whih is a signifiant pat of land tanspotation, is of inteest to us in this pape. The oad on whih ehiles tael is of piay inteest to oad stakeholdes, patiulaly the goenent. Many oads hae potholes, equiing light aintenane paties to estoe the to an aeptable ondition. Unfotunately, sientifi estiation of the total sufae aea and olue of potholes on a length of a oad is a ajo poble. This has depied oad anages of adequate planning sine they annot asetain the aount of ateials and ost of the epais fo suh potholes. This pape attepts to odel the total olue, sufae aea and ost of efilling of potholes along oads in the Nigeian enionent onsideing fatos suh as aount of ainfall, ehiula speed, ass of ehiles (Mabsout et al., 4). It is assued that wate is the only ajo natual soue of pothole popagation on the oad. The otion of ehiles on the oads espeially the ubbing of the a ties on the sufae of the oad auses wea and the weight of ehiles ause depessions on the oad espeially if the speed of tael of suh ehiles ae not that uh and if suh ehiles ae heay ehiles. The depessions and aks whih ae aused by suh ehiles then allow fo the gatheing of wate in the ausing dissolution and weaing away of the bituen eating a pothole (Singh, 7). The pape attepts to inopoate ost of these fatos into this odel. Fo the liteatue eseah by Mabsout (4) and Singh (7) poides a stong suppot fo the study. Mabsout et al. (4) pesents a paaeti study of the effet of potholes on load distibution in einfoed onete slab bidges using finite-eleent analysis (FEA). Consideation was gien to the pothole loation. It was epoted that the pesene of one o two potholes in the fist two lanes eated at the idspan of a bidge ineased the iu longitudinal bending oent by about 5% when opaed with FEA esults of slabs with no potholes, and by as uh as 7% when opaed with the AASHTO standad speifiations. Singh (7) olleted data of 4 ases of pot-hole subsidene fo Son-Mahanadi Maste Coal asin and analyzed fo stand point of thei ausatie fatos, pedition, ehanis, and suggested itigation easues. The esults show that the isk of pothole subsidene is high when the pothole potential atings of ausatie fatos ae between 8 and 1. The stutue of the pape is as The Paifi Jounal of Siene and Tehnology 4 Volue 8. Nube. Noebe 7 (Fall)

2 follows. The intodution poides a stong otiation fo the study and its justifiation. Subsequent setions will pesent the ethodology of the study; disuss ase study appliation of the poble in eal life, and also pesent a disussion of esults. Conluding eaks ae gien in the final setion of ou pape. METHODOLOGY The poble of potholes will be appoahed fo diffeent dietions one will be by wea aused by the atiities of as on its sufae wheeby the ties of the as ae assued to be ubbing the sufae of the oad as it oes along the oad. And the othe will be the effets of eosion by wate of the bituen in aeas whee aks and depessions ou. Anothe way will be in the fo of pobabilities of ouene on the oad with aeage (assue) adius fo the potholes. f t n t W W f n V t fequeny of tuks nube f tuks (total) suation ean weight of as weight of as fequeny of as total nube of as eloity of tuks Assuing that as a a oes along the oad, as in Figue 1: Definition of Tes V eloity of as M ass of a a aeleation of a F b the bonding foe of bituen F foe fo the as ties.e bonding enegy, K.E kineti enegy, ½M V C speed of light p ass of one patile n p nube of patiles n p sufae aea of patile ass of tie adius of tie ω angula eloity of tie total ass of patiles displaed itial eloity at whih the patile of bituen ae detahed beadth of the tie adius of the tie X distane taeled by the as Sine total sufae won SA in 1 e. nube of eolutions No. of e. total distane π adius F foe A aea l length δ etension E odulus of elastiity/igidity ε longitudinal stain ν Poisson atio a 1 b 1 1 diensions of a epesentatie ube W t weight of tuks The Paifi Jounal of Siene and Tehnology 41 Figue 1: Ca Moeent Along the oad. The ties not only otate but also tanslates due only to a gain in oentu, as in Figue : Figue : Inteation of the Wheel and Tie with the Sufae of the oad. As the a oes, the tie not only uses the fition between it and the oad to oe but also soe of the fition is oeoe and thee is a oesponding sliding of the tie on the oad. F μ N : Sliding ous when M a > F Assuing also that fo otion of the a thee has to be fition between the tie and the oad sufae. Volue 8. Nube. Noebe 7 (Fall)

3 As the tie otates we assue that soe patiles of bituen ae displaed o upooted due to the otion of the tie (Figue ). S A 4 b as i 1 πb 1 + πb + πb + + πb n when is onstant, S A 4 as i 1 whee b is onstant. π 1 b + π b + π b + + π n b, Figue : Inteation of the Tie/Wheel with the oad while in Motion. That is a fo of elation between the otation of the tie and the displaeent of the patiles. To deelop the fist, taking a iew at the patiulate leel (Figue 4): F Figue 4: Foe Analysis at the oad-tie/wheel Inteation. The tiny laye of bituen will detah itself when F > F b o oe, appopiately when K.E >.E, i.e. ½M V Δ, whee M, V and C ae onstant, Δ 1 MV C. Fo the seond assuption that soe patiles ae displaed as the tie otates, we assue onseation of enegy, i.e. ½ Iω ½ V, whee I, then n. p p The total sufae aea though whih the enegy is tansitted to the oad is A π 4. Fo as with diffeent tie adii and beadth, the total sufae aea won by these as will oe into play: This gies a double integal when eged beause of the fat that thee ae two aiables S A 4 ties. a in in πb d db in one otation of the Multiplying the esult of the integal by X X ties. d. Theefoe total adius d of the Total nube of eolutions in in in in πb d db π in in d d b d db d π d in d in d [( - in )( - in )] ( ) ( ) 4( in ) in Consideing the effets of the weight of a ehile on the bituen on the oad, we eaine the illustation of Figue 5. The Paifi Jounal of Siene and Tehnology 4 Volue 8. Nube. Noebe 7 (Fall)

4 Sine stess stain E F l E A δ beause all solid bodies hae a fo of elastiity befoe fatue. If the stess >>> E, thee will be a elatiely lage stain whih will ause a hange in olue of the bituen suh that: V o a 1 b in M g/ M g/ Figue 5: Foe Analysis at of the Vehile-oad Inteation. Fo Figue 6, it an be seen that the bituen epeienes opessie stess in the fo of Foe (weight)/aea: V f a 1 b 1 1 (1 + ε) (1 - νε) (1 - νε) a 1 b 1 1 (1 - νε + ε - νε ) (1 - νε) a 1 b 1 1 (1 - νε - νε + ν ε + ε - νε - νε + ν ε ) disegading all ultiples with powes: a 1 b 1 1 (1 - νε - νε + ε) a 1 b 1 1 (1 + ε - νε). When the elasti liit of the bituen has been eeeded aks and faults eege on the sufae of the oad. Assuing an eponential elationship between the weight of the ehile and the speed of the ehile, i.e. W W e -/1 suh that when, W W and when V V, W W M g/ M g/ 1 M g/ bituen onet soil Figue 6: Futhe Analysis of the Vehile-oad Inteation. The Paifi Jounal of Siene and Tehnology 4 Volue 8. Nube. Noebe 7 (Fall)

5 Fo this elationship, it an be seen that when fully loaded tuks play a oad at ey slow speeds thee is the tendeny that that oad will get bad fast if they ae not einfoed. Let us assue that a wide ange of ehiles ply a etain oad with a wide ange of weights and at aying eloities with diffeent fequenies on a ontinuous basis. The aeage o ean weight of the tuks Wtf Wtf t, while the ean weight of as, n t ft Wf Wf W, and the ean eloity n f Vtf t Vtf t of tuks, V t. Also, the ean n t f t Vf Vf eloity of as, V. n f Getting these alues and using the with the assued elationship between eloity and effetie weight of both the as and the tuks the tendeny of the oad to deelop potholes an be desibed (Nelkon and Pake, 1964). Using Fik s law of diffusion, the poess of disintegation of bituen an be eplained: dt d k(a ), C() Co whee C o onentation of the liquid initially C o < a a onentation of the diffusing body so that a (t) (a ())e -kt. Fo the dissoled patiles of bituen in oing wate, to desibe thei elatie oeent fo the enionent, ontinuity equations fo thee-diensional flow using Catesian oodinates will be ideal (i.e. assuing a ontol olue ACDEFGH) (Stoud, 1; Stoud and ooth, ). Figue 7 is taken in the fo of a etangula pis of sides δ, δy, δz in the, y, z dietions espetiely. While the aeage alues of the eloities in these dietions as V, Vy, Vz. Mass inflow though ACD in unit tie ρv. Taking a geneal ase whee ass density ρ and eloity V will hange in the dietion, the following equations apply: Y G A C H δy X D E δz δ Figue 7: Contol Volue. The Paifi Jounal of Siene and Tehnology 44 Volue 8. Nube. Noebe 7 (Fall)

6 Mass outflow though EFGH in unit tie ρv + ( ρv) δ Thus, net outflow in unit tie in dietion ( ρv) δ Siilaly, net outflow in unit tie in y dietion y ( ρvy) δ Net outflow in unit tie in z dietion z ( ρvz) δ Theefoe, total net outflow in unit tie y z ( ρv) + ( ρvy) + ( ρvz) δ also, sine unit tie. p t is the hange in ass density pe Change of ass in ontol olue in unit tie - p t δ (the negatie sign indiates that a net outflow has be assued). Then, total net outflow in unit tie hange of ass in ontol olue in unit tie. p - t y z ( ρv) + ( ρvy) + ( ρvz) δ δ y z ( ρv) + ( ρvy) + ( ρvz) Fo inopessible fluids like wate: ( V) ( Vy) ( Vz) 1995) + y + z - p t (Douglas et al., In this pape we hae assued potholes to be of a iula paaboloid shape with the foula z + y. Sine the ethod of getting the sufae aea of a funtion is: S z z y z z ds 1+ + s y fo a paaboloid ( y) Theefoe δ ( ) 4y and ddy ddy Coneting the oodinates to pola oodinates, whee: osθ, y sinθ + y, and ddy ddθ. + Theefoe δ 1 4 ddθ Taking the bounday onditions of the paaboloid fo to and θ to θ π, π δ 1 4 ddθ + π / 1 8/ 4 sufae aea of a paaboloid π 6 ( 1+ 4 ) dθ ( 1+ 4 ) The appoiate olue of a solid is found by haing a ultiple intenal of: V 1 1 Howee, V y y z z 1 dz dy d 1 1 fo pola oodinates. θ θ z1 dz z fo Catesian oodinates. d dθ Fo a paaboloid z y +, whee: The Paifi Jounal of Siene and Tehnology 45 Volue 8. Nube. Noebe 7 (Fall)

7 y sinθ osθ ddy d dθ z sin θ + os θ (sin θ + os θ) (1) Theefoe olue of a paaboloid (iula) π V π π 4 π 4 dz d dθ d dθ d dθ dθ 4 π olue of a paaboloid (iula) Due to the any paaetes o aiables affeting the foation of potholes on a patiula length of oad, we would use pobability to desibe the ouene of potholes on a oad suh that: The epeted nube of potholes on the entie length of a oad total length of the oad pobability of a pothole ouing on 1k of oad, i.e. E NX P(A), whee E is the epetation, N is the total pobability spae, while P(A) is the pobability saple. Using an aeage adius fo eah pothole the total sufae aea and total olue fo the potholes on the oad an be dedued. CASE STUDY AND DISCUSSION OF ESULTS Case Study 1: On the Lagos-Ibadan epessway, it was notied that fo eey 1k taele thee seeed to be between 1 to potholes with an aeage adius of.6. To find the total sufae aea and total olue fist of all, we find the epetation of potholes on the oad. Taking the length of the oad as 1k a pobability of a pothole as between.1 and.. Using.1 the epeted nube of potholes 1 potholes on the entie length of the oad and 6 potholes when using., all with an aeage adius of.6. Using this alue we get a total sufae aea of π [ 1+ 4(.6) ].57 fo one pothole, and π olue fo one pothole. Fo these figues and using the pobability of.1, thee will be a total pothole sufae aea of and a total olue of Case Study : On a oad of 1.5k an annual ainfall of about 1, lites of wate falls on it and the ean speed of flow of the wate off the oad is 11.11s -1. On this oad also is assued that about 1, as ply it annually with ties with a ean adius of.8 and a ass of 8kg (inluding the i). The iniu tie beadth and iu tie beadth ae.9 and.1 espetiely. The as that ply this oad ae assued to go at 1k/h. The oad has the following popeties: Its onentation is 1kg/ and a eady 9kg/ dissoles annually when wate aies. The density of one patile of bituen is about kg/, adius of.5 and diffusion onstant of 1-6 s -1. Citial eloity of bituen patile 1 8. Solution: Gien that δ 1.5k, V 1 lites 1, 11.11s -1, n 1. + in ,.8, 8kg, 1k/h, w (of ties) 99.ad/s. a 1kg/, C o 9kg/, g kg/, p.5, k 1-6 s -1, and 1 8. Sufae aea (total) 4 (.5) ( 1 ) + 4(.1) The Paifi Jounal of Siene and Tehnology 46 Volue 8. Nube. Noebe 7 (Fall)

8 Volue ( ) 8 ( 1 ) ( 1-9) Case Study : Total sufae aea won sufae aea won by the otion of ties + sufae of patiles won by eosion. 4 Sufae aea of patiles n p π p (using the sufae aea of a sphee as standad). Theefoe p 4 πp, Fo ½ Iω ½, Iω and taking I as, ω. Sufae aea won by ties 4( in ). Theefoe Total Sufae Aea + 4 ( in ) Volue of bituen won e ω 4 π p total ass won density of bituen total ass due to wea ing + ol.of ain diffusion ate density of bituen Iω Volue ω ω + ol.of wate - a - Whee: n p nube of patiles, p adius of patiles, total ass of patiles, g ( a - C ) o e -k δ p ass of one patile, ass of tie, adius of tie, eloity (itial) fo the eoal of a patile, iu beadth of ties, in iniu beadth of ties, a onentation of diffusing bodies, C o onentation of diffusing body in liquid, K diffusing oeffiient, δ distane taeled, and eloity of fluid (ean). Case Study 4: The fat that potholes do not ou ontinuously but andoly on a steth of oad akes the poble of odeling the total sufae aea of potholes on a steth of oad pobabilisti one. The potion on whih potholes ae found an be assued to be haateized by a weak soil unde laye with high seeping of goundwate into the onete foundation of the oad dissoling it. Fo this stateent, it an be seen that the nube of potholes that will ou on a oad, the depth and the size in tes of adius ae pobles of both statistis and pobability. Unde this peise theefoe, the odeling that will be deeloped will be on the dynais of the foation of a pothole whose soil undelaye is being o has been washed away fo unde the oads foundation. The only ausal fato fo the foation of potholes that is assued is that of wate. Assuing that the piniple o steps that poeed befoe the appeaane of a pothole on a oad ae these: (i) infiltation, (ii) dissolution, (iii) ass oeent of soil, (i) defletion of oad unde its own weight, () gatheing of wate on the sufae of the oad, (i) dissolution and washing away of the bituen. Infiltation: Assuing that the poess of infiltation is poweed by both apillay ation and soil wate table pessue. The total height h eahed by the wate o head of the wate is H H + H w, H apillay head, H w wate table head, Whee H 4σ osθ/ρgd. Note that: σ sufae tension, θ angle of ontat, d diaete of apillay as θ and d δd, dh i 4σ/ρgδd, H i 4nσ/ρgd The Paifi Jounal of Siene and Tehnology 47 Volue 8. Nube. Noebe 7 (Fall)

9 While Hw p/ρg; h 4nσ/ρgd + p/ρg 1 nσ + p ρg d The dissolution ate of any solute in a solent is k(t) ((o - ov) - (t) ), whee V is the olue of V the solute. Using the ontinuity equations, the oeent of soils an be odeled. Assuing a ontol olue ACDEFGH is taken in the fo of a etangula pis of sides δ, δy, δz in the, y, z dietions espetiely. While the aeage alues of the eloities in these dietions ae V, Vy, Vz.. Mass inflow though ACD in unit tie ρv. Taking a geneal ase whee ass density ρ and eloity V will hange in the α-dietion. Mass outflow though EFGH in unit tie ρv + ( ρv ) δ. Thus, net inflow in unit tie in -dietion ( ρv ) δ. Siilaly, net outflow in unit tie in y-dietion ( ρvy ) δ. Net outflow y in unit tie in z-dietion ( ρvz ) δ. z Theefoe, total net outflow in unit tie ( ρv ) ( ρvy ) ( ρvz ) δ y z + +. Also, ρ sine is the hange in ass density pe unit t tie. Change of ass in ontol olue in unit tie ρ δ (the negatie sign indiates that a t net outflow has been assued). Then, total net outflow in unit tie Change ass in ontol olue in unit tie y ρ δ t z ( ρv ) + ( ρv ) + ( ρv ) δ y Theefoe ( ρv ) + ( ρvy ) + ( ρvz ) y z ρ. Now fo the oeent of ass in wate we t assue a one-diensional flow i.e. ( ) ρv ρ. t z Y G A F δy C H δz X D E Z δ Figue 8: Futhe Analysis Contol Volue. The Paifi Jounal of Siene and Tehnology 48 Volue 8. Nube. Noebe 7 (Fall)

10 ρ n Now assuing that ate of dissolution: t t no - n(t) Kn(t) - o as δ V ( V ) d( V ) d, theefoe no - n(t) Kn(t) - o. V d( V ) d Whee: n ass pe unit tie of solute o iu onentation of ass pe unit tie of solute V olue of solent K oeffiient of dissolution (o assuing diffusion) ρ V o1 V Kn(t) (integating fo to ) ( n - n V) - n(t) o Assuing that eah ateial has its own ate of dissolution, theefoe Kn(t) ( no - nov) - n(t) an be epesented by p (Tioshenko, 195). p(t) Theefoe ass, whee length o adius V of aea, and t tie. Now due to the loss of the oad unde laye at a potion, that potion of oad an be assued to deflet unde its own weight. Assuing the oad to be a siply suppoted bea of span aying a unifoly distibuted load w pe unit un oe the whole span. Theefoe, the defletion at id-span whih is the 5wl 4 iu defletion aailable y, whee E 84EI the odulus of igidity, and I the oent of inetia of the bea/oads oss-setion. This y that has been got an be used as a alue of head if the effet of pessue of a pool of wate wee to be onsideed. ut sine the effet of the defletion being onsideed is that of the aking of the sufae, it an be negleted. o Sine only the effet of wate in dissoling and washing away the bituen is onsideed we an use the sae foula deied peiously fo the pt sufae eoal of the bituen i.e.. To get the olue obtained fo the pothole,, while fo the total sufae aea. ρ Assuing that all the patiles ae sphees, theefoe the sufae aea adius of patile. Theefoe total sufae aea n p p ass of one patile. 4 V π p, whee p n p 4 π p. ut, whee n p nube of patiles, and p Assuing that diffeent substanes in whatee fo hae a onstant diffusion ate, theefoe assuing fo bituen p kg/se and the adius of a patile is taken as 1 while the ass of one patile is also taken as.5g with a bituen of density of,kg -s assued. Theefoe the foulae beoes: (t), V and V,. The sufae aea π.1 Case Study 5: If a pothole wee to ou on a potion of a oad, it is desied to know the sufae aea and olue of bituen that will be washed away in yeas if the adius of the pothole would be about.5. The eloity of wate that noally flow on the sufae of that oad due to the egion it -1 is in, is s. Gien that t yeas ,.5, V 11.11s -1. The Paifi Jounal of Siene and Tehnology 49 Volue 8. Nube. Noebe 7 (Fall)

11 The ass that will be washed away is () kg kg. -4 Now the olue is V , while the sufae aea is about With the ase study just onluded, the total sufae aea and the total olue of potholes on a oad an be effetiely found, out afte onsideing and analyzing the data fo the diffeent paaetes that affet its foation. CONCLUSION With the ineasing effots by goenents to epai oads, the issue of pope planning and budgeting has been a ajo hallenge. Suh a poble has liited the popt epais of potholes on oads, whih equie light aintenane paties. The otiation to sole this ipotant poble has podued the uent study. Consequently, a odel is deeloped to analyze the total sufae aea and olue of potholes on oads. The odel deied within this pape an effetiely gie an epeted aount of potholes on any length of oad. 7. Tioshenko, S.P Stength of Mateials. MGaw Hill Publishes: New Yok, NY. AOUT THE AUTHOS Sunday A. Oke, M.S. gaduated in Industial Engineeing fo the Uniesity of Ibadan, Nigeia with a ahelo and Maste's degees in 1989 and 199, espetiely. He woked fo the IDM Seies Liited as a onsultant. M. Oke letues in the Depatent of Mehanial Engineeing, Uniesity of Lagos. He has eiewed papes fo seeal intenational jounals. Oluwadailae Ajayi, is an undegaduate student of the Depatent of Mehanial Engineeing, Uniesity of Lagos. SUGGESTED CITATION Oke, S.A. and O. Ajayi. 7. Modeling the Total Sufa e Aea and Volue of Potholes on a Length of oad. Paifi Jounal of Siene and Tehnology. 8():4-5. Paifi Jounal of Siene and Tehnology EFEENCES 1. Douglas, J.F., Gasioek, J.M., and Swaffield, J.A., Fluid Mehanis. Longan Goup: London, UK. ISN Mabsout M., Tahini K., Awwad E., and Fedeik G. 4. Effet of Potholes on Load Distibution in Conete Slab idges. Pat. Peiodial on Stut. Des. and Const.. 9(): Nelkon, M. and Pake, P. 1964, Adaned Leel Physis. Heineann Eduational Publishes: London, UK. 4. Singh, K.. 7. Pot-Hole Subsidene in Son- Mahanadi Maste Coal asin. Engineeing Geology, 89(1-): Stoud, K.A. and ooth D.J.. Adaned Engineeing Matheatis (4th edition). Palgae. ISN Stoud, K.A. 1. Engineeing Matheatis, 5th Edition. Palgae. ISN The Paifi Jounal of Siene and Tehnology 5 Volue 8. Nube. Noebe 7 (Fall)

Determine the Stress Calculating Mode of Sliding Failure of Soil Mass under the Push-Extend Multi-under-Reamed Pile

Determine the Stress Calculating Mode of Sliding Failure of Soil Mass under the Push-Extend Multi-under-Reamed Pile Engineeing, 014, 6, 54-59 Published Online Apil 014 in SiRes. http://www.sip.og/jounal/eng http://dx.doi.og/10.436/eng.014.6509 Deteine the Stess Calulating Mode of Sliding Failue of Soil Mass unde the

More information

Red Shift and Blue Shift: A realistic approach

Red Shift and Blue Shift: A realistic approach Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,

More information

Recitation PHYS 131. must be one-half of T 2

Recitation PHYS 131. must be one-half of T 2 Reitation PHYS 131 Ch. 5: FOC 1, 3, 7, 10, 15. Pobles 4, 17, 3, 5, 36, 47 & 59. Ch 5: FOC Questions 1, 3, 7, 10 & 15. 1. () The eloity of a has a onstant agnitude (speed) and dietion. Sine its eloity is

More information

GRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION

GRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION GAVITOELECTOMAGNETIM AND NEWTON LAW O UNIVEAL GAVITATION Antoine Ake etied Pofesso, Depatent Industial ienes Uniesity Collee Kaho int-lieen Gent - Beliu ant.ake@skynet.be Abstat In this atile it is shown

More information

GRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION

GRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION GAVITOELECTOMAGNETIM AND NEWTON LAW O UNIVEAL GAVITATION Antoine Ake etied Pofesso, Depatent Industial ienes Uniesity Collee Kaho int-lieen Gent - Beliu ant.ake@skynet.be Abstat Takin into aount the kineatis

More information

SAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2

SAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2 SAMPLE LABORATORY SESSION FOR JAVA MODULE B Calulations fo Sample Coss-Setion. Use Input. Setion Popeties The popeties of Sample Coss-Setion ae shown in Figue and ae summaized below. Figue : Popeties of

More information

1 Fundamental Solutions to the Wave Equation

1 Fundamental Solutions to the Wave Equation 1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation One example is to onside aousti adiation

More information

Physics 218, Spring March 2004

Physics 218, Spring March 2004 Today in Physis 8: eleti dipole adiation II The fa field Veto potential fo an osillating eleti dipole Radiated fields and intensity fo an osillating eleti dipole Total satteing oss setion of a dieleti

More information

Extra Examples for Chapter 1

Extra Examples for Chapter 1 Exta Examples fo Chapte 1 Example 1: Conenti ylinde visomete is a devie used to measue the visosity of liquids. A liquid of unknown visosity is filling the small gap between two onenti ylindes, one is

More information

4) Magnetic confinement of plasma

4) Magnetic confinement of plasma 4) Magneti onfineent of plasa Due to the shielding in the plasa, thee is alost no ontol with eleti fields. A ontol is possible with agneti fields, as patiles ae bound to the field lines. This is alled

More information

Torque, Angular Momentum and Rotational Kinetic Energy

Torque, Angular Momentum and Rotational Kinetic Energy Toque, Angula Moentu and Rotational Kinetic Enegy In ou peious exaples that inoled a wheel, like fo exaple a pulley we wee always caeful to specify that fo the puposes of the poble it would be teated as

More information

Khmelnik S.I. Mathematical Model of Dust Whirl

Khmelnik S.I. Mathematical Model of Dust Whirl Khmelnik S.I. Mathematial Model of Dust Whil Abstat The question of the soue of enegy in a dust whil is onsideed. Atmosphei onditions annot be the sole soue of enegy, as suh dust whils exist on Mas, whee

More information

ATMO 551a Fall 08. Diffusion

ATMO 551a Fall 08. Diffusion Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path

More information

Example 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example

Example 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example 014-11-18 Centipetal Aeleation 13 Exaple with full olution Exaple 1 A 1500 kg a i oing on a flat oad and negotiate a ue whoe adiu i 35. If the oeffiient of tati fition between the tie and the oad i 0.5,

More information

Circular Motion Problem Solving

Circular Motion Problem Solving iula Motion Poblem Soling Aeleation o a hange in eloity i aued by a net foe: Newton nd Law An objet aeleate when eithe the magnitude o the dietion of the eloity hange We aw in the lat unit that an objet

More information

From E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018

From E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018 Fom E.G. Haug Esape eloity To the Golden Ratio at the Blak Hole Banko Zivlak, bzivlak@gmail.om Novi Sad, May 018 Abstat Esape veloity fom the E.G. Haug has been heked. It is ompaed with obital veloity

More information

Revolving Ferrofluid Flow due to Rotating Disk

Revolving Ferrofluid Flow due to Rotating Disk Poeedings of the Wold Congess on Engineeing 1 Vol III WCE 1, July - 6, 1, London, U.K. Reoling Feofluid Flow due to Rotating isk Paas Ram, Kushal Shama bstat - eoling flow of feofluid oe a otating disk

More information

The Concept of the Effective Mass Tensor in GR. Clocks and Rods

The Concept of the Effective Mass Tensor in GR. Clocks and Rods The Concept of the Effective Mass Tenso in GR Clocks and Rods Miosław J. Kubiak Zespół Szkół Technicznych, Gudziądz, Poland Abstact: In the pape [] we pesented the concept of the effective ass tenso (EMT)

More information

For circular motion with tangential acceleration we get:

For circular motion with tangential acceleration we get: FW Phys 13 E:\Exel files\h1-18 Fomulas eiew fo final4.do page 1 of 1 Last pinted 5/19/4 :4: PM Kinemati fomulas: x = a = onstant (1.1) = α = onstant Pojetile Motion: 1 The inemati equation eto t () = at

More information

OBSTACLE DETECTION USING RING BEAM SYSTEM

OBSTACLE DETECTION USING RING BEAM SYSTEM OBSTACLE DETECTION USING RING BEAM SYSTEM M. Hiaki, K. Takamasu and S. Ozono Depatment of Peision Engineeing, The Univesity of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo, Japan Abstat: In this pape, we popose

More information

Time Dilation in Gravity Wells

Time Dilation in Gravity Wells Time Dilation in Gavity Wells By Rihad R. Shiffman Digital Gaphis Asso. 038 Dunkik Ave. L.A., Ca. 9005 s@isi.edu This doument disusses the geneal elativisti effet of time dilation aused by a spheially

More information

(conservation of momentum)

(conservation of momentum) Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational

More information

8.022 (E&M) Lecture 13. What we learned about magnetism so far

8.022 (E&M) Lecture 13. What we learned about magnetism so far 8.0 (E&M) Letue 13 Topis: B s ole in Mawell s equations Veto potential Biot-Savat law and its appliations What we leaned about magnetism so fa Magneti Field B Epeiments: uents in s geneate foes on hages

More information

momentum change via particle gain/

momentum change via particle gain/ Letue 6 asi plasa dynais Ou fluid euations that we developed befoe ae: f ( n n )+ v v n + v v M v f P+ n E+ v 3 4 34 oentu lost via ollisions oentu hange via patile gain/ loss We have looked ollisions

More information

Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0

Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0 IOECONOMIC MODEL OF A FISHERY (ontinued) Dynami Maximum Eonomi Yield In ou deivation of maximum eonomi yield (MEY) we examined a system at equilibium and ou analysis made no distintion between pofits in

More information

AVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES

AVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES ELECTROMAGNETIC THEORY SOLUTIONS GATE- Q. An insulating sphee of adius a aies a hage density a os ; a. The leading ode tem fo the eleti field at a distane d, fa away fom the hage distibution, is popotional

More information

1121 T Question 1

1121 T Question 1 1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed

More information

Physics Courseware Modern Physics

Physics Courseware Modern Physics Physis Cousewae oden Physis Enegy and oentu Relatiisti oentu: p γ Kineti enegy: K. E. ( γ ) Auxiliay equation: E + 4 p whee is the est ass and E is total enegy. Poble.- What has oe ass at est: i) A sodiu

More information

Dissolution of Solid Particles in Liquids: A Shrinking Core Model

Dissolution of Solid Particles in Liquids: A Shrinking Core Model Wold Aademy of Siene, Engineeing and Tehnology 5 9 Dissolution of Solid Patiles in Liquids: A Shining oe Model Wei-Lun Hsu, Mon-Jyh Lin, and Jyh-Ping Hsu Astat The dissolution of spheial patiles in liquids

More information

Chapter 4. Sampling of Continuous-Time Signals

Chapter 4. Sampling of Continuous-Time Signals Chapte 4 Sampling of Continuous-Time Signals 1 Intodution Disete-time signals most ommonly ou as epesentations of sampled ontinuous-time signals. Unde easonable onstaints, a ontinuous-time signal an be

More information

Molecular Energy Changes During a Reaction

Molecular Energy Changes During a Reaction Reation Kinetis Moleula Enegy Changes Duing a Reation Chemial Enegy of Speies E xn E* +BP E* P+B Moleules above this enegy level (defined somewhat abitaily) ae alled ativated omplexes Poduts Reatants Pogession

More information

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid: hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of

More information

1 Fundamental Solutions to the Wave Equation

1 Fundamental Solutions to the Wave Equation 1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation. One example is to onside aousti adiation

More information

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March EN4: Dynaics and Vibations Midte Exaination Tuesday Mach 8 16 School of Engineeing Bown Univesity NME: Geneal Instuctions No collaboation of any kind is peitted on this exaination. You ay bing double sided

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

Lecture 23: Central Force Motion

Lecture 23: Central Force Motion Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces

More information

Photographing a time interval

Photographing a time interval Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals

More information

Generalized Vapor Pressure Prediction Consistent with Cubic Equations of State

Generalized Vapor Pressure Prediction Consistent with Cubic Equations of State Genealized Vapo Pessue Pedition Consistent with Cubi Equations of State Laua L. Petasky and Mihael J. Misovih, Hope College, Holland, MI Intodution Equations of state may be used to alulate pue omponent

More information

Einstein s Transverse Doppler Effect Proven Wrong. The Complete Proof. Copyright 2006 Joseph A. Rybczyk

Einstein s Transverse Doppler Effect Proven Wrong. The Complete Proof. Copyright 2006 Joseph A. Rybczyk Einstein s Tansese Dopple Effet Poen Wong The Complete Poof Copyight 006 Joseph A. Rybzyk Abstat Stit adheene to the sientifi method in oelating the piniples of light popagation with the piniples of elatiisti

More information

FARADAY'S LAW dt

FARADAY'S LAW dt FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,

More information

Mass Transfer (Stoffaustausch)

Mass Transfer (Stoffaustausch) Mass Tansfe (Stoffaustaush) Examination 3. August 3 Name: Legi-N.: Edition Diffusion by E. L. Cussle: none nd 3 d Test Duation: minutes The following mateials ae not pemitted at you table and have to be

More information

Optimum Settings of Process Mean, Economic Order Quantity, and Commission Fee

Optimum Settings of Process Mean, Economic Order Quantity, and Commission Fee Jounal of Applied Science and Engineeing, Vol. 15, No. 4, pp. 343 352 (2012 343 Optiu Settings of Pocess Mean, Econoic Ode Quantity, and Coission Fee Chung-Ho Chen 1 *, Chao-Yu Chou 2 and Wei-Chen Lee

More information

Flight Loads Analysis of a Maneuvering Transport Aircraft

Flight Loads Analysis of a Maneuvering Transport Aircraft Flight Loads Analysis of a Maneuveing Tanspot Aiaft Hui hang, a, Jie Li, b, Qiong Liu, Shool of Aeonautis, Nothesten Polytehnial Univesity, China Univesidad Politénia de Madid, Spain a hanghui_@6.o, b

More information

Revised Newtonian Formula of Gravity and Equation of Cosmology in Flat Space-Time Transformed from Schwarzschild Solution

Revised Newtonian Formula of Gravity and Equation of Cosmology in Flat Space-Time Transformed from Schwarzschild Solution Intenational Jounal of Astonomy and Astophysis,,, 6-8 http://dx.doi.og/.46/ijaa.. Published Online Mah (http://www.sip.og/jounal/ijaa) evised Newtonian Fomula of Gavity and Equation of Cosmology in Flat

More information

Special Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k.

Special Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k. Speial Relativit in Aousti and Eletomagneti Waves Without Phase Invaiane and Loentz Tansfomations Benhad Rothenstein bothenstein@gmail.om Abstat. Tansfomation equations fo the phsial quantities intodued

More information

Electric Anisotropy, Magnetic Anisotropy, Uniaxial and Biaxial Materials, Bianisotropic Media (Definitions)

Electric Anisotropy, Magnetic Anisotropy, Uniaxial and Biaxial Materials, Bianisotropic Media (Definitions) leti nisotop agneti nisotop Uniaial and iaial ateials ianisotopi edia efinitions medium is alled eletiall anisotopi if tenso Note that and ae no longe paallel medium is magnetiall anisotopi if tenso Note

More information

LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle

LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle LINEAR MOMENTUM Physical quantities that we have been using to chaacteize the otion of a paticle v Mass Velocity v Kinetic enegy v F Mechanical enegy + U Linea oentu of a paticle (1) is a vecto! Siple

More information

Answers to Coursebook questions Chapter 2.11

Answers to Coursebook questions Chapter 2.11 Answes to Couseook questions Chapte 11 1 he net foe on the satellite is F = G Mm and this plays the ole of the entipetal foe on the satellite, ie mv mv Equating the two gives π Fo iula motion we have that

More information

1131 T Question 1

1131 T Question 1 1131 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, taelling on the sae path in the sae diection as you, at a constant speed

More information

matschek (ccm2548) Ch17-h3 chiu (57890) 1

matschek (ccm2548) Ch17-h3 chiu (57890) 1 matshek m2548) Ch17-h3 hiu 5789) 1 This pint-out should have 16 questions. Multiple-hoie questions may ontinue on the next olumn o page find all hoies efoe answeing. 1 1. points A student said, The eleti

More information

Charged particle motion in magnetic field

Charged particle motion in magnetic field Chaged paticle otion in agnetic field Paticle otion in cued agnetic fieldlines We diide the equation of otion into a elocity coponent along the agnetic field and pependicula to the agnetic field. Suppose

More information

Reflectance spectra for Si

Reflectance spectra for Si Refletane speta fo Si Notie R and ε i and ε show onsideable stutues in the fom of peas and shouldes. These stutues aise fom the optial tansitions between alene bands to the ondution bands. 16 Miosopi Theoy:

More information

AN ELECTROMAGNETIC LAUNCH SYSTEM FOR UAVs

AN ELECTROMAGNETIC LAUNCH SYSTEM FOR UAVs Tehnial Sienes and Applied athematis AN ELECTROAGNETIC LAUNCH SYSTE FOR UAVs Lauian GHERAN Depatment of Eletonis and Infomatis, Faulty of Aeonautial anagement, Heni Coandă Ai Foe Aademy, Basov, Romania

More information

Study of the Endface Friction of the Revolving Vane Mechanism

Study of the Endface Friction of the Revolving Vane Mechanism Pudue Univesity Pudue e-pubs Intenational Compesso Engineeing Confeene Shool of Mehanial Engineeing 010 Study of the Endfae Fition of the Revolving Vane Mehanism Alison Subiantoo Shool of Mehanial and

More information

30 The Electric Field Due to a Continuous Distribution of Charge on a Line

30 The Electric Field Due to a Continuous Distribution of Charge on a Line hapte 0 The Electic Field Due to a ontinuous Distibution of hage on a Line 0 The Electic Field Due to a ontinuous Distibution of hage on a Line Evey integal ust include a diffeential (such as d, dt, dq,

More information

The Radii of Baryons

The Radii of Baryons Jounal Heading Yea; Vol. (No.): page ange DOI: 0.592/j.xxx.xxxxxxxx.xx The Radii of Bayons Maio Evealdo de Souza Depatmento de Físia, Univesidade Fedeal de Segipe, São Cistovão, 4900-000, Bazil Astat Consideing

More information

Gravitoelectromagnetism. II. Speed of Light in Gravitational Field

Gravitoelectromagnetism. II. Speed of Light in Gravitational Field Zbigniew Osiak aitoeletomagnetism. II. May 9, 8 aitoeletomagnetism. II. peed of Light in aitational Field Zbigniew Osiak E-mail: zbigniew.osiak@gmail.om http://oid.og/--57-36x http://ixa.og/autho/zbigniew_osiak

More information

CHAPTER 6: UNIFORM CIRCULAR MOTION AND GRAVITATION

CHAPTER 6: UNIFORM CIRCULAR MOTION AND GRAVITATION College Physics Student s Manual Chapte 6 CHAPTER 6: UIORM CIRCULAR MOTIO AD GRAVITATIO 6. ROTATIO AGLE AD AGULAR VELOCITY. Sei- taile tucks hae an odoete on one hub of a taile wheel. The hub is weighted

More information

Ion-sound waves (electrostatic low frequency waves)

Ion-sound waves (electrostatic low frequency waves) OTHER TYPES of WAVES Ion-sound waves (eletostati low fequeny waves) ae longitudinal waves simila lassial sound in gas s kt k M B plasma sound is slow fo eletons, but fast fo ions Eleton density is in eah

More information

Circular Motion. x-y coordinate systems. Other coordinates... PHY circular-motion - J. Hedberg

Circular Motion. x-y coordinate systems. Other coordinates... PHY circular-motion - J. Hedberg Cicula Motion PHY 207 - cicula-motion - J. Hedbeg - 2017 x-y coodinate systems Fo many situations, an x-y coodinate system is a geat idea. Hee is a map on Manhattan. The steets ae laid out in a ectangula

More information

NEW ROTATIONAL DYNAMICS

NEW ROTATIONAL DYNAMICS NEW OTATIONAL DYNAMICS haate of statis Inetia toque piniple and the foe oent the GuagSan Yu ( Habin Mao Dynais Institute. 50066, P.. China ) E-ail:sxzyu5@hotail.o ( 04.8.7 04.9.0 ) Abstat: Textual point

More information

DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH 1. INTRODUCTION

DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH 1. INTRODUCTION DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH Mugu B. RĂUŢ Coesponding autho: Mugu RĂUŢ, E-mail: m_b_aut@yahoo.om Abstat In this pape I popose a oetion to the well-known Newtonian gavitational

More information

Thermodynamic and Kinetic Modeling of Phase Transitions for CH4/CO2 Hydrates

Thermodynamic and Kinetic Modeling of Phase Transitions for CH4/CO2 Hydrates Reent Advanes in Meanis, eat & Mass Tansfe and Biology Teodynai and Kineti Modeling of Pase Tansitions fo C/CO ydates BJØRN KAMME, KURAM BAIG, MUAMMAD QASIM, JORDAN BAUMAN Depatent of Pysis and Tenology

More information

Effects of Thermal Loads on Concrete Cover of FRP Reinforced Elements: Theoretical and Experimental Analysis

Effects of Thermal Loads on Concrete Cover of FRP Reinforced Elements: Theoretical and Experimental Analysis Aiello, M.A., F. Foai, and A. Nanni, Effets of hemal Loads on Conete Cove of FRP Reinfoed Elements: heoetial and Expeimental Analysis, ACI Mateials Jounal, Vol. 98, No. 4, July-Aug., pp. 33-339. Effets

More information

Mass- and light-horizons, black holes' radii, the Schwartzschild metric and the Kerr metric

Mass- and light-horizons, black holes' radii, the Schwartzschild metric and the Kerr metric 006-010 Thiey De Mees Mass- and light-hoizons, blak holes' adii, the Shwatzshild meti and the Ke meti mpoved alulus. (using gavitomagnetism) T. De Mees - thieydm@pandoa.be Abstat Blak holes geneally ae

More information

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE Fundamental Jounal of Mathematical Physics Vol. 3 Issue 1 13 Pages 33-44 Published online at http://www.fdint.com/ ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES

More information

Chapter 6 Differential Analysis of Fluid Flow

Chapter 6 Differential Analysis of Fluid Flow 1 Chapte 6 Diffeential Analysis of Fluid Flow Inviscid flow: Eule s equations of otion Flow fields in which the sheaing stesses ae zeo ae said to be inviscid, nonviscous, o fictionless. fo fluids in which

More information

The Research of AQI Index Changing Regularity Mainly in Tianjin Ziyu Guo

The Research of AQI Index Changing Regularity Mainly in Tianjin Ziyu Guo nd Intenational Confeene on Eduation Tehnology, Management and Humanities Siene (ETMHS 06 The Reseah of AQI Index Changing Regulaity Mainly in Tianjin Ziyu Guo Shool of Institute of Eletial and Eletoni

More information

TORSIONAL VIBRATIONS IN THE SAW UNIT OF A KIND OF CIRCULAR SAW. NUMERICAL INVESTIGATIONS OF THE NATURAL FREQUENCIES AND MODE SHAPES

TORSIONAL VIBRATIONS IN THE SAW UNIT OF A KIND OF CIRCULAR SAW. NUMERICAL INVESTIGATIONS OF THE NATURAL FREQUENCIES AND MODE SHAPES TRIESKOVÉ A BEZTRIESKOVÉ OBRÁBANIE DREVA, 8(): 7 78, Zvolen, Tehniká univezita vo Zvolene, ISBN 978-8-8-85- 7 TORSIONAL VIBRATIONS IN THE SAW UNIT OF A KIND OF CIRCULAR SAW NUMERICAL INVESTIGATIONS OF

More information

Introduction to Money & Banking Lecture notes 3/2012. Matti Estola

Introduction to Money & Banking Lecture notes 3/2012. Matti Estola Intoduction to Mone & Banking Lectue notes 3/22 Matti Estola Inteest and pesent value calculation Tansfoation equations between inteest ates Inteest calculation Inteest ate (/t is the ate of etun of an

More information

Application of Poisson Integral Formula on Solving Some Definite Integrals

Application of Poisson Integral Formula on Solving Some Definite Integrals Jounal of Copute and Electonic Sciences Available online at jcesblue-apog 015 JCES Jounal Vol 1(), pp 4-47, 30 Apil, 015 Application of Poisson Integal Foula on Solving Soe Definite Integals Chii-Huei

More information

Microscopic Momentum Balances

Microscopic Momentum Balances 013 Fluids ectue 6 7 Moison CM3110 10//013 CM3110 Tanspot I Pat I: Fluid Mechanics Micoscopic Momentum Balances Pofesso Faith Moison Depatment of Chemical Engineeing Michigan Technological Uniesity 1 Micoscopic

More information

dp p v= = ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945).

dp p v= = ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945). ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945). It is shown that at lage distanes fom the body, moving with a. veloity exeeding that of

More information

LECTURE 15. Phase-amplitude variables. Non-linear transverse motion

LECTURE 15. Phase-amplitude variables. Non-linear transverse motion LETURE 5 Non-linea tansvese otion Phase-aplitude vaiables Second ode (quadupole-diven) linea esonances Thid-ode (sextupole-diven) non-linea esonances // USPAS Lectue 5 Phase-aplitude vaiables Although

More information

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09 FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this

More information

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

Physics 2A Chapter 10 - Moment of Inertia Fall 2018 Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.

More information

Tidal forces. m r. m 1 m 2. x r 2. r 1

Tidal forces. m r. m 1 m 2. x r 2. r 1 Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.

More information

Simulation of a Shielded Thermocouple

Simulation of a Shielded Thermocouple ISSN 1014-4874 DOI : http://dx.doi.og/10.4314/j.v27i1.1 Siulation of a Shielded Theoouple Fedik Bentsson 1, Fidèle Ndahayo, Yves Nyalihaa and, Jean Maie Vianney Munyeshyaka 2 1 Linköping Univesity, S-581

More information

Gravitational Equivalent Frequency, the Planck Length and Matter Waves

Gravitational Equivalent Frequency, the Planck Length and Matter Waves Gaitational Equialent Fequeny, te Plank Lengt and Matte Waes by Roge Ellman Abstat Analysis of gaitation and of matte waes disloses a geate signifiane tan eetofoe eognized fo te fequeny, wae, osillation

More information

Newton s E = mc 2 Two Hundred Years Before Einstein? Newton = Einstein at the Quantum Scale

Newton s E = mc 2 Two Hundred Years Before Einstein? Newton = Einstein at the Quantum Scale Newton s E = Two Hunded Yeas Befoe Einstein? Newton = Einstein at the Quantu Scale Espen Gaade Haug Nowegian Uniesity of Life Sciences August 7, 07 Abstact The ost faous Einstein foula is E =, while Newton

More information

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS 5.4 Radian Measue So fa, ou hae measued angles in degees, with 60 being one eolution aound a cicle. Thee is anothe wa to measue angles called adian measue. With adian measue, the ac length of a cicle is

More information

Class #16 Monday, March 20, 2017

Class #16 Monday, March 20, 2017 D. Pogo Class #16 Monday, Mach 0, 017 D Non-Catesian Coodinate Systems A point in space can be specified by thee numbes:, y, and z. O, it can be specified by 3 diffeent numbes:,, and z, whee = cos, y =

More information

The Geometric Concept of Matter

The Geometric Concept of Matter The Geoeti Conept of Matte Zoan Ozie * Mah 5, 008 A B S T R A C T The geoeti onept of atte efines the funaental stutue of the eleentay ateial patile as a otating-ibating sphee. All the essential popeties

More information

Adsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity

Adsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity The Open-Access Jounal fo the Basic Pinciples of Diffusion Theoy, Expeient and Application Adsoption and Desoption Kinetics fo Diffusion Contolled Systes with a Stongly Concentation Dependent Diffusivity

More information

DYNAMICS OF UNIFORM CIRCULAR MOTION

DYNAMICS OF UNIFORM CIRCULAR MOTION Chapte 5 Dynamics of Unifom Cicula Motion Chapte 5 DYNAMICS OF UNIFOM CICULA MOTION PEVIEW An object which is moing in a cicula path with a constant speed is said to be in unifom cicula motion. Fo an object

More information

A New I 1 -Based Hyperelastic Model for Rubber Elastic Materials

A New I 1 -Based Hyperelastic Model for Rubber Elastic Materials A New I -Based Hypeelastic Model fo Rubbe Elastic Mateials Osca Lopez-Paies SES Octobe -4, Evanston, IL Neo-Hookean odel W ìï ï ( I - ) = ( if l + l + l - ) lll = = í ï + othewise ïî (*). Matheatical siplicity

More information

The Kerr-metric, mass- and light-horizons, and black holes' radii.

The Kerr-metric, mass- and light-horizons, and black holes' radii. 006 Thiey De Mees The Ke-meti, mass- and light-hoizons, and blak holes' adii. (using the Analogue Maxwell theoy) T. De Mees - thieydm @ pandoa.be Abstat Blak holes an geneally be defined as stella objets

More information

COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE

COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE To see how the piniple behind the analysis of vaiane method woks, let us onside the following simple expeiment. The means ( 1 and ) of

More information

New Approach to Predict the Micromechanical. Behavior of a Multiphase Composite Material

New Approach to Predict the Micromechanical. Behavior of a Multiphase Composite Material Advanced Studies in Theoetical Physics Vol. 8, 2014, no. 20, 869-873 HIKARI Ltd, www.-hikai.co http://dx.doi.og/10.12988/astp.2014.4677 New Appoach to Pedict the Micoechanical Behavio of a Multiphase oposite

More information

e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e

e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e EN: Continuum Mehanis Homewok : Kinematis Due : noon Fiday Febuay 4th Shool of Engineeing Bown Univesity. To analyze the defomation of a onial membane, it is poposed to use a two-dimensional onial-pola

More information

7.2.1 Basic relations for Torsion of Circular Members

7.2.1 Basic relations for Torsion of Circular Members Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,

More information

In electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface

In electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface Ampee s law n eletostatis, the eleti field E and its soues (hages) ae elated by Gauss s law: EdA i 4πQenl Sufae Why useful? When symmety applies, E an be easily omputed Similaly, in magnetism the magneti

More information

Equivalency of Momentum and Kinetic Energy and Pythagorean Conservation of Mass and Energy

Equivalency of Momentum and Kinetic Energy and Pythagorean Conservation of Mass and Energy Intenational Jounal of Applied Physis and Matheatis, Vol., No. 4, July quivaleny of Moentu and Kineti negy and Pythagoean Consevation of Mass and negy Mohsen Lutey Abstat Aepted equations in the ehanis

More information

Orbital Angular Momentum Eigenfunctions

Orbital Angular Momentum Eigenfunctions Obital Angula Moentu Eigenfunctions Michael Fowle 1/11/08 Intoduction In the last lectue we established that the opeatos J Jz have a coon set of eigenkets j J j = j( j+ 1 ) j Jz j = j whee j ae integes

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods TEAM 2007, Sept. 10-13, 2007,Yokohama, Japan Hydoelastic Analysis of a 1900 TEU Containe Ship Using Finite Element and Bounday Element Methods Ahmet Egin 1)*, Levent Kaydıhan 2) and Bahadı Uğulu 3) 1)

More information

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi ENGI 44 Non-Catesian Coodinates Page 7-7. Conesions between Coodinate Systems In geneal, the conesion of a ecto F F xi Fy j Fzk fom Catesian coodinates x, y, z to anothe othonomal coodinate system u,,

More information

THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS

THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS Abstat THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS V. Bendt, S. Zunft and H. Mülle-Steinhagen Geman Aeospae Cente (DLR), Stuttgat, Gemany This pape desibes the

More information

PHYSICS. Time allowed: 90 minutes. Section A is a set of questions on data analysis. It requires work on graph paper.

PHYSICS. Time allowed: 90 minutes. Section A is a set of questions on data analysis. It requires work on graph paper. PHYSICS EXAMIATIO FOR ETRACE SCHOLARSHIPS JAUARY 7 Tie allowed: 9 inutes Section A is a set of questions on data analysis. It equies wok on gaph pape. Section B consists of nine questions. Attept as any

More information

Macroelement Modelling of Laterally Loaded Piles and Pile-groups

Macroelement Modelling of Laterally Loaded Piles and Pile-groups 1 st Intenational Confeene on Natual Hazads & Infastutue 8-30 June, 016, Chania, Geee Maoelement Modelling of Lateally Loaded Piles and Pile-goups Nikos Geolymos 1 National Tehnial Univesity of Athens

More information