The Four Kinetic Regimes of Adsorption from Micellar Surfactant Solutions
|
|
- Linda Kelly
- 5 years ago
- Views:
Transcription
1 The Four Kinetic Regie of Adorption fro Micellar Surfactant Solution P.A. Kralchevky, K.. anov, N.. enkov, N.C. Chritov, K.P. Ananthapadanabhan,* and Alex Lip* Laboratory of Cheical Phyic and Engineering, Faculty of Cheitry, Univerity of Sofia, Bulgaria, and *Unilever R&, Trubull, CT, USA Plenary Lecture at the 59 th iviional Meeting on Colloid and Interface Cheitry, The Cheical Society of Japan Hokkaido Univerity, Sapporo, Japan, Septeber 3-5, 006 Effect of icelle diffuion and diaebly on the dynaic urface tenion
2 ( The interfacial expanion give rie to urfactant adorption and to decreae in the onoer concentration near the interface; ( Thi lead to icelle decopoition and to diffuion of icelle. {Fat icellar proce} {Exchange of onoer between the icelle} (Rate contant k {Slow icellar proce} {ecopoition of a critical-ize icelle to onoer}. (Rate contant k S
3 General Set of Equation (Anianon & Wall, 974 Multi-Step Micellization: k + A + A A ( k,3, 4,... d c dt d c dt + I J 3 J + J J + (,3,4,... I iffuion and Reaction Fluxe: I J c (,,3,... k + c c k c (,3,4,... The proce i theoretically decribed by a yte containing ten of kinetic uation, which i inconvenient for application. For thi reaon, one of the baic proble of icellar kinetic i how to iplify the general et of uation without looing the aduacy and correctne of the theoretical decription.
4 Introduction of a Model (Gauian Micelle Size itribution c C ( exp[ π Anianon & Wall, 974 ] ( n r C C n r c n r c C n r ( c (i (ii (iii Region of the onoer and oligoer, Ω o ( n o Region of the rare aggregate, Ω r (n o < < n r Region of the abundant icelle, Ω ( n r New: ( We do not aue cont. ( We do not ue of the quai-uilibriu approxiation: local cheical uilibriu between icelle and onoer. (3 The derived general uation are nonlinear: applicable to both large and all perturbation.
5 Reduction of the Proble to 4 Equation for 4 Unknown Function Monoer concentr.; Total icelle conc.; Mean aggreg. nuber; Polydiperity c (r,t, C (r,t, (r,t, (r,t d c dt + I n r J J,0 Nonlinear expreion for the fluxe J, J,0, and J, are derived. dc dt d d t ( C + I,0 + I J, n r J + J,0 J J n, J ( r, i J i > n r i 0, d d t [( + C ] + I, n r J J,0 + J, i I, i I ( i n r 0,,
6 Relaxation of a Spatially Unifor Perturbation (C jup; T jup; P jup: bulk relaxation ethod Our purpoe i to ee what are the prediction of the odel for thi type of perturbation. ienionle perturb. in: Total ic. conc.; Mean aggreg. nuber; Polydiperity Linearization of the proble: Syte of three linear uation for ξ c, ξ, and ξ ξ c C C,p, A hoogeneou yte ha a nontrivial olution only if it deterinant i ual to zero characteritic uation I, I, I 3 invariant of the atrix (a ij ; three eigenvalue three relaxation tie: τ c, τ, τ. ; ξ j c,, ( a 3 p ij ; ξ p λδ ξ 0, i c,, λ I λ ij + j I λ I 3 0 λ j ; j c,, τ k t j j
7 The Three Micellar Characteritic Relaxation Tie λ j ; j c,, τ k t j j C tot β CMC CMC ienionle icelle concentration t c k S β β + + β / t c i the characteritic tie of the low proce, that i the relaxation of the total icellar concentration C ; k S rate contant of the low proce (Anianon-Wall + k t β t i the firt characteritic tie of the fat proce, related to the relaxation of the ean icellar aggregation nuber, ; k rate contant of the fat proce (Anianon-Wall t k t i the econd characteritic tie of the fat proce, related to the relaxation of the icellar polydiperity, ; (new! k rate contant of the fat proce. The expreion for t c and t by Anianon & Wall are confired!
8 Nuerical Reult for Typical Paraeter Value: 7 60; 5; ks / k 0 ienionle relax. tie Exact Low icelle concentration: β Approxiate expreion τ c τ τ High icelle concentration: β 00 τ c τ τ ienionle icelle concentration: C tot β CMC CMC Low icelleconcentration τ > : c > τ τ High icelleconcentration : τ > τ > c τ τ c relaxation tie of icelle concentration (of the low proce, Anianon & Wall τ relaxation tie of ean aggreg. nuber (of the fat proce, Anianon & Wall τ relaxation tie of icelle polydiperity (new effect, predicted by preent theory
9 Ayptotic Expreion: The three baic phyical paraeter, C, and, are perturbed. ( The Relaxation of a Perturbation in Micelle Concentration, C, i Governed only by the Slow Micellar Tie, t c ξc ( t Ac exp( t / tc ( tc >> t, t ( A c aplitude of the perturbation in C Hence, if the relaxation of icelle concentration i eaured, only the Slow Micellar Tie, t c, could be deterined. Note, however, that a perturbation in C perturb alo and!
10 The Relaxation of a Perturbation in Micelle Mean Aggregation Nuber i Governed by both the Slow and Fat Tie, t c and t ξ ( t A c τ β exp( t / t c + ( A + A c τ β exp( t / t ( A c and A aplitude of the perturbation in C and Hence, if the relaxation of icelle ean aggregation nuber i eaured, then both the low and fat icellar tie, t c and t, could be deterined. Note that a perturbation in perturb, but doe not affect C
11 The Relaxation of a Perturbation in Micelle Polydiperity i Governed by the two Fat Relaxation Tie, t and t Hence, if the relaxation of icelle polydiperity i eaured, then the two fat icellar tie, t and t, could be deterined. Note that a perturbation in polydiperity doe not affect C and. ] / exp( / [exp( ( / exp( ( β τ ξ t t t t t t t A A t t A t c + +
12 Suary of Part : Micellar Relaxation Procee in the Bulk The theoretical analyi iplie: (A The relaxation of the three baic paraeter, the icelle concentration, C, the ean aggregation nuber,, and the polydiperity,, are characterized by three ditinct relaxation tie: t c, t, and t. (B The firt two of the, t c and t, coincide with the conventional low and fat icellar relaxation tie. (C The third relaxation tie, t, i cloe to t for low icelle concentration, but at high icelle concentration we have t c > t > t..
13 ( The relaxation of C i affected by t c alone. (E The relaxation of i affected by both t and t c. (F The the relaxation of i affected by t and t. Siple, but accurate analytical expreion are available: ( For calculation of the three relaxation tie; ( For decribing the evolution of a icellar yte. [K.. anov, P.A. Kralchevky, et al., Adv. Colloid Interface Sci. 9 (006-6] Next tep: Invetigation of the proble about the kinetic of adorption fro icellar olution, and the repective dynaic urface tenion (Part.
14 Part : Theoretical odeling of adorption fro icellar olution at quiecent and expanding urface Main quetion to be anwered: Why in different cae different kinetic regie are oberved? (a diffuion liited kinetic: [ Δ t / ]; (b reaction liited kinetic: [ Δ exp( t /τ ]. Which of the two very different theoretical expreion for the effective diffuivity of a icellar olution i correct? (a by J. Lucaen (975: eff ( + β ( + β / (b by Paul Joo (988: eff ( + β ( + β /
15 Paraeter of the Adorption Proce ζ dienionle ditance; τ dienionle tie; diffuivity of the onoer; k rate contant of the low icellar proce; k rate contant of the fat proce. a S a a a ; ; ; k h K k h K t h z h τ ζ (adorption length ( a c h Γ
16 ienionle Perturbation c C ( exp[ π ] ( n r ξ Γ h p a (0 c,p ; ξ c h β Γ a p C (0,p ; ξ h a c Γ, p (0 p ; ξ h a c Γ, p p (0 ξ dienionle perturbation in the concentration of onoer, c ; ξ c dienionle perturbation in the icelle concentration, C ; ξ dienionle perturbation in the icelle ean aggregation nuber, ; ξ dienionle perturbation in the icelle polydiperity,.
17 General Syte of Kinetic Equation (fro Part S K S K w ϕ β ϕ ζ ξ τ ξ ( c c K B ϕ β ζ ξ τ ξ + K w K B ϕ ϕ β ζ ξ τ ξ + ξ ϕ ϕ β ζ ξ τ ξ ( K K w K B + (urfactant onoer (concentration of icelle (icelle ean aggregation nuber (polydiperity ϕ dienionle reaction flux of the low relaxation proce; ϕ dienionle reaction flux of the fat relaxation proce. CMC ( tot CMC / C β B
18 Reaction fluxe fro the low and fat relaxation procee ϕ ξ ξ For ξ ξ, we obtain ϕ 0 (criterion for uilibriu with repect to the fat icellization proce ϕ ( w ξ ξ + c wξ For ξ ξ c ξ, we obtain ϕ 0 (criterion for uilibriu with repect to the low icellization proce Method of olution of the general yte of linear partial differential uation: Laplace tranfor, olving the uation, and nuerical revere Laplace tranfor
19 Nuerical Reult: Typical Relaxation Curve (Four kinetic regie of adorption: AB, BC, C, and E γ ( t γ γ (0 γ ξ,0 ( τ ξ,0 decribe the relaxation of the urface tenion γ (t. Four different relaxation regie: AB, BC, C, E (B ξ ξ, then ϕ 0 uilibrated fat icellar proce; ( ξ ξ c ξ ϕ ϕ 0 uilibrated fat and low icellar procee.
20 Analytical Expreion for the Relaxation in ifferent Regie τ θ F θ τ C θ c θ c dienionle relaxation tie of the low proce; θ and θ d.le relaxation tie of the fat proce. Two exponential regie (AB and C with relaxation tie τ F and τ C ; Two invere-quare-root regie (BC & E with relaxation tie τ BC and τ E.
21 ( Kinetic Regie AB The fat icellar proce govern the adorption kinetic [exp(t/τ F ] τ / F, F ( + β K θ θ τ F 4 ξ,0 F exp( F F τ + π 0 τ exp[ ( + ττ~ τ F ] ( ~ τ ~ τ + / τ F + ~ τ d ~ τ τ / ξ,0 ( + τ +... (hort π F F ξ,0 exp( τ +... (long F tie ayptotic tie ayptotic τ F F The regie AB(exp wa oberved by P. Joo for Triton X-00, inclined plate ethod. (epending on the urfactant and experient. ethod, different regie are oberved!
22 ( Kinetic Regie BC ξ,0 ξ,0 iffuion control the fat icellar proce i uilibrated, wherea the effect of the low proce i negligible [t / ] τ BC / ξ,0 ( +... π τ (invere-quare-root tie dependence τ BC BC ( + β ( + β (relaxation tie τ BC, & effective diffuivity BC The regie BC wa oberved by u for SS with the axiu bubble preure ethod (MBPM, and by Makievki et al. for Triton X-00, MBPM again. For /, the expreion for BC reduce to that propoed by Joo (988.
23 (3 Kinetic Regie C The low icellar proce govern the adorption kinetic [exp(t/τ S ] γ ( t γ γ (0 γ ξ,0 ( τ ξ,0 τ BC ( π τ / τ exp( τ C (exponential relaxation τ C θ c β 3 K (the relaxation tie, τ C, coincide with the characteritic tie of the low icellar proce
24 (4 Kinetic Regie E iffuion control both the fat and low icellar procee are uilibrated [t / ] τ E / ξ,0 ( +... (invere-quare-root-of-tie dependence; Lucaen 975 π τ τ E + E + ( + β ( + β (Expreion for the Relaxation Tie & iffuivity The Lucaen uation wa unuccefully tried by Joo et al. to fit data for Brij 58 (trip ethod. It turn out that the data by Joo et al. (988 correpond to the regie BC, which ha not been identified at that tie.
25 Cobined Expreion for the whole BCE region Analyzing the baic yte of uation we arrived at the following cobined forula for the whole region BCE: ξ,0 τ E ( π τ / τ BC + ( π τ / τ exp( τ C τ E + + ( + β ( + β τ BC ( + β ( + β 00 >> / τ << τ E BC (eay to ditinguih regie BC fro E [etail in: K.. anov, P.A. Kralchevky, et al., Adv. Colloid Interface Sci, 9 ( ]
26 ifference between the exponential regie AB and C /τ F increae with icelle concentration; /τ C decreae with icelle concentration Exponential regie AB: ξ,0 τ exp( τ + τ F Exponential regie C: τ BC / τ ξ,0 ( exp( π τ τ F C
27 Surfactant v. Method in Relation to the Relaxation Regie Fat urfactant {urfactant that adorb quickly}: Fat ethod {ethod that eaure early urface age}: Regie AB: Can be detected for low urfactant by fat ethod. Exaple: Triton X-00 by inclined plate ethod. Regie C and E: ifficult for detection becaue ξ,0 ha becoe very all for thee regie; in principle, thee regie could be detected for very fat urfactant by very low and enitive ethod. Regie BC: Can be detected for fat urfactant by low ethod. Exaple: SS by MBPM.
28 Rudientary Kinetic iagra at Low Micelle Concentration (β and/or at Saller ifference between the Rate of the Fat and Slow Micellization Procee (aller K /K The three icellar relaxation tie, θ c, θ and θ, are cloe to each other. Point A, B, and C coincide. τ / ξ,0 ( + τ +... π (hort tie ayptotic (the ae a in regie AB The effect of the fat relaxation proce diappear at low urfactant concentration (β ξ,0 τ exp( τ + τ C The long-tie ayptotic i the ae a in regie AB but τ F τ C C
29 Method with Stationary Interfacial Expanion: Micellar Kinetic d A dα ( t α& ( t A d t d t cont. The kinetic regie are: (AB θ /(K AB + θ / kinetic regie governed by the fat icellization proce; (BC θ / diffuion-liited regie at uilibrated fat proce but negligible low proce; (C θ /(K C + θ / kinetic regie governed by the low icellization proce; θ a h & α θ dienionle expanion rate (E θ / diffuion-liited regie at uilibrated both the fat and low icellization procee. [etail in: K.. anov, P.A. Kralchevky, et al., Colloid & Surface A, 8-83 ( ]
30 Coparion of Theory and Experient Exaple : ynaic urface tenion of Brij 58 eaured by the trip ethod (Paul Joo Theory: ΓkT π & α / ( CMC BC CMC ol/c 3 ifferent curve correpond to different icelle concentration, β Γ ol/c (at CMC Fro the lope of the plot α& / v. at fixed β, one deterine the apparent diffuivity BC (β.
31 Coparion of Theory and Experient (Continued Exaple : ynaic urface tenion of Brij 58 eaured by the trip ethod (Paul Joo 00 Brij 58, Strip ethod u.06, B BC + uβ ( + uβb ( BC / B / 0.43 (reaonable value β (C tot CMC/CMC Fro the fit of the data, one deterine: u For Brij 58, 70 ; hence the polydiperity of the icelle i 8.6 The obtained reaonable value confir that the kinetic regie i BC /.06
32 The Overflowing Cylinder Method Another ethod with tationary interfacial expanion d A α& ( t cont. A d t Adorption (rather than urface tenion i detected by ellipoetry or neutron reflection The Overflowing Cylinder Method (OFC C.. Bain et al. Languir 004, 0,
33 Exaple : ynaic urface tenion of C 4 TAB by the Overflowing Cylinder Method (Colin Bain et al.; the adorption Γ i directly eaured by ellipoetry The data point are not for the ae β! Theory: Y Γ Γ Y 0 (i.e. 0, give the uilibriu adorption at CMC, Γ. / τ dif ( Γ Y { π & α /[( + uβ ( + uβb ]} α& / Adorption, Γ (μol/ Γ C 4 TAB + 00 M NaBr Overflowing cylinder u.; B 0.3 The bet fit Γ v. Y correpond to B / 0.3 and u / Y ( / 80; fro u. we deterine that the polydiperity of the C 4 TAB icelle i 9.8. The obtained value of Γ. B and are reaonable. Thi confir that the kinetic regie i BC. [τ dif h a / i the characteritic diffuion tie]
34 Part 3: Application of the Maxiu Bubble Preure Method Proble: ifferent tenioeter - different reult for the dynaic urface tenion. Thi i difference i deontrated with our data for two apparatue. The data are plotted a ST v. t / : ynaic urface tenion, N/ M SS, 8 M NaCl t / ( / Kru BP Setup - Horozov Explanation: ifferent tie-dependence, A(t, of the bubble urface area for different apparatue.
35 Solution of the Proble Suggeted by the Experient The experient indicate that A(t d i independent of:. Bubbling period, t age. Surfactant concentration 3. Surfactant type (General validity? The theory indicate that in ot cae γ(t depend on a contant paraeter, λ integral of A(t, rather than on the function A(t. A(t (the apparatu function can be deterined only by cineatography; λ (the apparatu contant can be deterined alo by MBPM (uch eaier! Below we check whether λ i independent of t age, urfactant type and concentration.
36 Expanding Surface v. Iobile Surface γ γ,0λ γ γ + γ / + γ / + ( t ( t ( t age age u γ,0 / γ kt Γ λ γ, 0 λ, t / u tage / ( π c λ ( τ τ t d τ 0 0 A d A0 (ˆ t dˆ t / d, d dt d A( t [ A d 0 ]dt τ τ ( t d d λ ( The whole effect of the interfacial expanion i incorporated in λ ; ( t u (univeral urface age, i the age of an (initially clean iobile urface with the ae γ a that regitered by the MBPM tenioeter. c bulk urfactant concentration; Γ uilibriu adorption; γ uilibriu urface tenion; urfactant diffuivity; γ,0 the value of γ for an iobile interface.
37 Exaple : Coparion of data obtained by MBPM (expanding bubble with data for iobile bubble (IB for SS + 00 M NaCl. For MBPM λ i deterined by integration of the experiental A(t curve (for our apparatu; For IB we have λ (no expanion t u t age /λ i ued to plot the MBPM data in (b (λ 37
38 70.5 M NaCG + 00 M NaCl Exaple : Surface tenion, γ (N/ MBPM Wilhely plate Coparion of data obtained by MBPM (expanding bubble with data fro Wilhely plate ethod for Na N-Cocoylglycinate Noinal urface age, t age / ( / For Wilhely plate (iobile urface: t u t age (λ For MBPM (expanding urface: t u t age /λ (λ The excellent fit with the theoretical dependence evidence diffuion-liited adorption kinetic. Surface tenion, γ (N/ 70.5 M NaCG + 00 M NaCl 60 MBPM 50 γ γ γ γ,0 / γ,0 + tu 4.43 ± 0.0 N/ Wilhely plate / / Univeral urface age, t u ( + a
39 Two way to deterine the apparatu contant, λ: ( By integration of the experiental A(t curve; ( By MBPM experient, λ γ / γ,0. γ,0 kt (π Γ / c (Copare the value of λ obtained in the two way! Procedure: ( γ (t age curve are obtained by MBPM and fitted with the dependence: γ γ + a + (t age / Thu γ i deterined. ( Next, γ,0 i calculated fro fit of uilibriu urface tenion iother. γ (3 λ γ / γ,0
40 C SS (M Γ (μol/ γ,0 (N.. / γ (N.. / λ γ / γ,0 SS + 0 M NaCl SS + 00 M NaCl Theory: λ Average: λ 6.07 ± 0.0
41 C TAB (M Γ (μol/ γ,0 (N.. / γ (N.. / λ γ / γ,0 TAB + 5 M NaBr TAB + 00 M NaBr Theory: λ Average: λ 6.07 ± 0.0
42 Concluion: The reult confir the concept about the apparatu contant: ( λ i the ae for all concentration of a given urfactant and electrolyte; ( λ i the ae for SS and TAB; (3 λ i calculated fro γ deterined of the data fit for 0 < t age < 40 t u t age /λ λ ( Hence, in ter of t u the MBP ethod i uch (37 tie fater. t u t age /λ, account for the urface expanion, and for thi reaon t u give the phyically correct urface age. etail in: Chritov et al., Languir (
43 Plot of the dienionle effective diffuivity of icellar olution, eff /, v. β Maxiu Bubble Preure Method (MBPM eff γ,cmc γ diffuivity of urfactant onoer. The data for γ(t are fitted well with the expreion for diffuion-liited adorption: γ γ + a + (t γ age / eff BC ( + β ( + β Hence, the kinetic regie i either BC or E. The data coplie with BC!
44 Plot of Plot of v. β calculated fro the data for eff / (MBPM Rudientary kinetic regie icelle ean aggregation nuber; icelle polydiperity Kinetic regie BC Reaonable paraeter value the kinetic regie i BC Value / < are reaonable. For exaple, for β 0 and 70 we obtain: 7. (SS 9.5 (TAB
45 Suary and Concluion The theory indicate the preence of four different kinetic regie of adorption fro icellar urfactant olution: ( Regie AB: the fat icellar proce govern the adorption kinetic [exp(t/τ F ] ( Regie BC: diffuion control the fat icellar proce i uilibrated, wherea the effect of the low proce i negligible [t / ]. (3 Regie C: the low icellar proce govern the adorption kinetic [exp(t/τ S ] (4 Regie E: diffuion control both the fat and low icellar procee are uilibrated [t / ]. (5 MBPM: The deterination of the apparatu contant, λ, for a given tenioeter allow one to characterize a given urfactant olution with a univeral dynaic urface tenion curve, γ(t.
46 The reult are publihed in the following paper:. K.. anov, P.A. Kralchevky, N.. enkov, K.P. Ananthapadanabhan, and A. Lip, Ma Tranport in Micellar Surfactant Solution:. Relaxation of Micelle Concentration, Aggregation Nuber and Polydiperity, Adv. Colloid Interface Sci. 9 ( K.. anov, P.A. Kralchevky, N.. enkov, K.P. Ananthapadanabhan, and A. Lip, Ma Tranport in Micellar Surfactant Solution:. Theoretical Modeling of Adorption at a Quiecent Interface, Adv. Colloid Interface Sci. 9 ( K.. anov, P.A. Kralchevky, K.P. Ananthapadanabhan, and A. Lip, Micellar Surfactant Solution: ynaic of Adorption at Fluid Interface Subjected to Stationary Expanion, Colloid & Surface A, 8-83 ( N.C. Chritov, K.. anov, P.A. Kralchevky, K.P. Ananthapadanabhan, and A. Lip, The Maxiu Bubble Preure Method: Univeral Surface Age and Tranport Mechani in Surfactant Solution, Languir ( K.. anov, P.A. Kralchevky, K.P. Ananthapadanabhan, and A. Lip, Influence of Electrolyte on the ynaic Surface Tenion of Ionic Surfactant Solution: Expanding and Iobile Interface, J. Colloid Interface Sci. (006 in pre.
Moisture transport in concrete during wetting/drying cycles
Cheitry and Material Reearch Vol.5 03 Special Iue for International Congre on Material & Structural Stability Rabat Morocco 7-30 Noveber 03 Moiture tranport in concrete during wetting/drying cycle A. Taher
More informationMicellar surfactant solutions: Dynamics of adsorption at fluid interfaces subjected to stationary expansion
Colloids and Surfaces A: Physicoche. Eng. Aspects 8 83 (006) 143 161 Micellar surfactant solutions: Dynaics of adsorption at fluid interfaces subjected to stationary expansion Krassiir D. Danov a, Peter
More informationAn Exact Solution for the Deflection of a Clamped Rectangular Plate under Uniform Load
Applied Matheatical Science, Vol. 1, 007, no. 3, 19-137 An Exact Solution for the Deflection of a Claped Rectangular Plate under Unifor Load C.E. İrak and İ. Gerdeeli Itanbul Technical Univerity Faculty
More informationThe Extended Balanced Truncation Algorithm
International Journal of Coputing and Optiization Vol. 3, 2016, no. 1, 71-82 HIKARI Ltd, www.-hikari.co http://dx.doi.org/10.12988/ijco.2016.635 The Extended Balanced Truncation Algorith Cong Huu Nguyen
More informationLecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes
ecture Phy 798S Spring 6 Steven Anlage The heart and oul of uperconductivity i the Meiner Effect. Thi feature uniquely ditinguihe uperconductivity fro any other tate of atter. Here we dicu oe iple phenoenological
More informationA novel protocol for linearization of the Poisson-Boltzmann equation
Ann. Univ. Sofia, Fac. Chem. Pharm. 16 (14) 59-64 [arxiv 141.118] A novel protocol for linearization of the Poion-Boltzmann equation Roumen Tekov Department of Phyical Chemitry, Univerity of Sofia, 1164
More informationThe Features For Dark Matter And Dark Flow Found.
The Feature For Dark Matter And Dark Flow Found. Author: Dan Vier, Alere, the Netherland Date: January 04 Abtract. Fly-By- and GPS-atellite reveal an earth-dark atter-halo i affecting the orbit-velocitie
More information4.5 Evaporation and Diffusion Evaporation and Diffusion through Quiescent Air (page 286) bulk motion of air and j. y a,2, y j,2 or P a,2, P j,2
4.5 Evaporation and Diffuion 4.5.4 Evaporation and Diffuion through Quiecent Air (page 86) z bul otion of air and j z diffuion of air (a) diffuion of containant (j) y a,, y j, or P a,, P j, z 1 volatile
More informationPHYSICS 211 MIDTERM II 12 May 2004
PHYSIS IDTER II ay 004 Exa i cloed boo, cloed note. Ue only your forula heet. Write all wor and anwer in exa boolet. The bac of page will not be graded unle you o requet on the front of the page. Show
More informationConservation of Energy
Add Iportant Conervation of Energy Page: 340 Note/Cue Here NGSS Standard: HS-PS3- Conervation of Energy MA Curriculu Fraework (006):.,.,.3 AP Phyic Learning Objective: 3.E.., 3.E.., 3.E..3, 3.E..4, 4.C..,
More informations s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr
Flipping Phyic Lecture Note: Introduction to Acceleration with Priu Brake Slaing Exaple Proble a Δv a Δv v f v i & a t f t i Acceleration: & flip the guy and ultiply! Acceleration, jut like Diplaceent
More informationChapter 7. Principles of Unsteady - State and Convective Mass Transfer
Suppleental Material for Tranport Proce and Separation Proce Principle hapter 7 Principle of Unteady - State and onvective Ma Tranfer Thi chapter cover different ituation where a tranfer i taking place,
More informationAnswer keys. EAS 1600 Lab 1 (Clicker) Math and Science Tune-up. Note: Students can receive partial credit for the graphs/dimensional analysis.
Anwer key EAS 1600 Lab 1 (Clicker) Math and Science Tune-up Note: Student can receive partial credit for the graph/dienional analyi. For quetion 1-7, atch the correct forula (fro the lit A-I below) to
More information15 N 5 N. Chapter 4 Forces and Newton s Laws of Motion. The net force on an object is the vector sum of all forces acting on that object.
Chapter 4 orce and ewton Law of Motion Goal for Chapter 4 to undertand what i force to tudy and apply ewton irt Law to tudy and apply the concept of a and acceleration a coponent of ewton Second Law to
More informationScale Efficiency in DEA and DEA-R with Weight Restrictions
Available online at http://ijdea.rbiau.ac.ir Int. J. Data Envelopent Analyi (ISSN 2345-458X) Vol.2, No.2, Year 2014 Article ID IJDEA-00226, 5 page Reearch Article International Journal of Data Envelopent
More informationPOSTER PRESENTATION OF A PAPER BY: Alex Shved, Mark Logillo, Spencer Studley AAPT MEETING, JANUARY, 2002, PHILADELPHIA
POSTER PRESETATIO OF A PAPER BY: Ale Shved, Mar Logillo, Spencer Studley AAPT MEETIG, JAUARY, 00, PHILADELPHIA Daped Haronic Ocillation Uing Air a Drag Force Spencer Studley Ale Shveyd Mar Loguillo Santa
More informationImage Denoising Based on Non-Local Low-Rank Dictionary Learning
Advanced cience and Technology Letter Vol.11 (AT 16) pp.85-89 http://dx.doi.org/1.1457/atl.16. Iage Denoiing Baed on Non-Local Low-Rank Dictionary Learning Zhang Bo 1 1 Electronic and Inforation Engineering
More informationName: Answer Key Date: Regents Physics. Energy
Nae: Anwer Key Date: Regent Phyic Tet # 9 Review Energy 1. Ue GUESS ethod and indicate all vector direction.. Ter to know: work, power, energy, conervation of energy, work-energy theore, elatic potential
More information4 Conservation of Momentum
hapter 4 oneration of oentu 4 oneration of oentu A coon itake inoling coneration of oentu crop up in the cae of totally inelatic colliion of two object, the kind of colliion in which the two colliding
More informationDIFFERENTIAL EQUATIONS
Matheatic Reviion Guide Introduction to Differential Equation Page of Author: Mark Kudlowki MK HOME TUITION Matheatic Reviion Guide Level: A-Level Year DIFFERENTIAL EQUATIONS Verion : Date: 3-4-3 Matheatic
More informationTopic 7 Fuzzy expert systems: Fuzzy inference
Topic 7 Fuzzy expert yte: Fuzzy inference adani fuzzy inference ugeno fuzzy inference Cae tudy uary Fuzzy inference The ot coonly ued fuzzy inference technique i the o-called adani ethod. In 975, Profeor
More informationMarkov Processes. Fundamentals (1) State graph. Fundamentals (2) IEA Automation 2018
Fundaental () Markov Procee Dr Ulf Jeppon Div of Indutrial Electrical Engineering and Autoation (IEA) Dept of Bioedical Engineering (BME) Faculty of Engineering (LTH), Lund Univerity Ulf.Jeppon@iea.lth.e
More informationPhysics 20 Lesson 28 Simple Harmonic Motion Dynamics & Energy
Phyic 0 Leon 8 Siple Haronic Motion Dynaic & Energy Now that we hae learned about work and the Law of Coneration of Energy, we are able to look at how thee can be applied to the ae phenoena. In general,
More informationm 0 are described by two-component relativistic equations. Accordingly, the noncharged
Generalized Relativitic Equation of Arbitrary Ma and Spin and Bai Set of Spinor Function for It Solution in Poition, Moentu and Four-Dienional Space Abtract I.I.Gueinov Departent of Phyic, Faculty of Art
More informationRanking DEA Efficient Units with the Most Compromising Common Weights
The Sixth International Sypoiu on Operation Reearch and It Application ISORA 06 Xiniang, China, Augut 8 12, 2006 Copyright 2006 ORSC & APORC pp. 219 234 Ranking DEA Efficient Unit with the Mot Coproiing
More informationInvestigation of application of extractive distillation method in chloroform manufacture
Invetigation of application of etractive ditillation ethod in chlorofor anufacture Proceeding of uropean Congre of Cheical ngineering (CC-6) Copenhagen, 16-20 Septeber 2007 Invetigation of application
More informationResearch Article An Extension of Cross Redundancy of Interval Scale Outputs and Inputs in DEA
Hindawi Publihing Corporation pplied Matheatic Volue 2013, rticle ID 658635, 7 page http://dx.doi.org/10.1155/2013/658635 Reearch rticle n Extenion of Cro Redundancy of Interval Scale Output and Input
More informationTIME-AVERAGED TURBULENT MIXING AND VERTICAL CONCENTRATION DISTRIBUTION OF HIGH-DENSITY SUSPENSIONS FORMED UNDER WAVES
TIME-AVERAGED TURBULENT MIXING AND VERTICAL CONCENTRATION DISTRIBUTION OF HIGH-DENSITY SUSPENSIONS FORMED UNDER WAVES Bing Yan, Qing-He Zhang, Michael P. Lab 3 We analyzed ocillating flo data fro U-tube
More informationCIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh
Nae: CIRCLE YOUR DIVISION: Div. 1 (9:30 a) Div. (11:30 a) Div. 3 (:30 p) Prof. Ruan Prof. Nai Mr. Singh School of Mechanical Engineering Purdue Univerity ME315 Heat and Ma Tranfer Exa # edneday, October
More informationConcept of Reynolds Number, Re
Concept of Reynold Nuber, Re Ignore Corioli and Buoyancy and forcing Acceleration Advection Preure Gradient Friction I II III IV u u 1 p i i u ( f u ) b + u t x x x j i i i i i i U U U? U L L If IV <
More informationSIMM Method Based on Acceleration Extraction for Nonlinear Maneuvering Target Tracking
Journal of Electrical Engineering & Technology Vol. 7, o. 2, pp. 255~263, 202 255 http://dx.doi.org/0.5370/jeet.202.7.2.255 SIMM Method Baed on Acceleration Extraction for onlinear Maneuvering Target Tracking
More informationSTRUCTURE AND MAGNETIC PROPERTIES OF NANOCOMPOSITES ON THE BASIS PE+Fe 3 O 4 и PVDF+ Fe 3 O 4
Diget Journal of Nanoaterial and Biotructure Vol. 5, No 3, July-Septeber 21, p. 727-733 STRUCTURE AND MAGNETIC PROPERTIES OF NANOCOMPOSITES ON THE BASIS PE+Fe 3 O 4 и PVDF+ Fe 3 O 4 М. А. RAMAZANOV *,
More information1-D SEDIMENT NUMERICAL MODEL AND ITS APPLICATION. Weimin Wu 1 and Guolu Yang 2
U-CHINA WORKHOP ON ADVANCED COMPUTATIONAL MODELLING IN HYDROCIENCE & ENGINEERING epteber 9-, Oxford, Miiippi, UA -D EDIMENT NUMERICAL MODEL AND IT APPLICATION Weiin Wu and Guolu Yang ABTRACT A one dienional
More informationCh. 6 Single Variable Control ES159/259
Ch. 6 Single Variable Control Single variable control How o we eterine the otor/actuator inut o a to coan the en effector in a eire otion? In general, the inut voltage/current oe not create intantaneou
More informationAP Physics Momentum AP Wrapup
AP Phyic Moentu AP Wrapup There are two, and only two, equation that you get to play with: p Thi i the equation or oentu. J Ft p Thi i the equation or ipule. The equation heet ue, or oe reaon, the ybol
More informationinto a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get
Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}
More informationA New Model and Calculation of Available Transfer Capability With Wind Generation *
The Eighth International Sypoiu on Operation Reearch and It Application (ISORA 09) Zhangjiajie, China, Septeber 0, 009 Copyright 009 ORSC & APORC, pp. 70 79 A New Model and Calculation of Available Tranfer
More informationUnified Model for Short-Channel Poly-Si TFTs
Unified Model for Short-Channel Poly-Si TFT Benjaín Iñiguez, 1 Zheng Xu, 1 Tor A. Fjeldly 1, and Michael. S. Shur 1 1 Departent of Electrical, Coputer, and Syte Engineering, Renelaer Polytechnic Intitute,
More informationChemistry I Unit 3 Review Guide: Energy and Electrons
Cheitry I Unit 3 Review Guide: Energy and Electron Practice Quetion and Proble 1. Energy i the capacity to do work. With reference to thi definition, decribe how you would deontrate that each of the following
More informationINVERSE ESTIMATE OF SOIL PARAMETERS AND SURFACE ENERGY BUDGET FROM IN SITU MEASUREMENTS
INVERSE ESTIMATE OF SOIL PARAMETERS AND SURFACE ENERGY BUDGET FROM IN SITU MEASUREMENTS KUN YANG, TOSHIO KOIKE Departent of Civil Engineering, Univerity of Toyo, Hongo 7-3-, Bunyo-u, Toyo 3-8656, Japan
More informationPHYSICS 151 Notes for Online Lecture 2.3
PHYSICS 151 Note for Online Lecture.3 riction: The baic fact of acrocopic (everda) friction are: 1) rictional force depend on the two aterial that are liding pat each other. bo liding over a waed floor
More information4. ENZYME KINETICS. Enzyme kinetics
4. ENZYME INETIC Enzye inetic Invetigation of enzyatic reaction rate, identification of paraeter. E + E + P For toichioetric calculation all coponent hould be given in ole or gra. But: enzye are not pure
More informationTHE BICYCLE RACE ALBERT SCHUELLER
THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The
More information2.7 Aerosols and coagulation
1 Note on 1.63 Advanced Environmental Fluid Mechanic Intructor: C. C. Mei, 1 ccmei@mit.edu, 1 617 53 994 December 1,.7 Aerool and coagulation [Ref]: Preent, Kinetic Theory of Gae Fuch, Mechanic of Aerool
More informationFLists. F.1 Nomenclature
FLit Appendix F F.1 Noenclature In the following ubection the ybol ued in thi thei are given, with their dienion if applicable, followed by a hort decription. F.1.1 A A B c x d D D c D D T E F g g n G
More informationHybrid technique based on chirp effect and phase shifts for spectral Talbot effect in sampled fiber Bragg gratings (FBGs)
Optica Applicata, Vol. XLI, No. 1, 011 Hybrid technique baed on chirp effect and phae hift for pectral Talbot effect in apled fiber Bragg grating (FBG) GUO DENG *, WEI PAN Center for Inforation Photonic
More information3.185 Problem Set 6. Radiation, Intro to Fluid Flow. Solutions
3.85 Proble Set 6 Radiation, Intro to Fluid Flow Solution. Radiation in Zirconia Phyical Vapor Depoition (5 (a To calculate thi viewfactor, we ll let S be the liquid zicronia dic and S the inner urface
More informationLecture 17: Frequency Response of Amplifiers
ecture 7: Frequency epone of Aplifier Gu-Yeon Wei Diiion of Engineering and Applied Science Harard Unierity guyeon@eec.harard.edu Wei Oeriew eading S&S: Chapter 7 Ski ection ince otly decribed uing BJT
More informationThe continuous time random walk (CTRW) was introduced by Montroll and Weiss 1.
1 I. CONTINUOUS TIME RANDOM WALK The continuou time random walk (CTRW) wa introduced by Montroll and Wei 1. Unlike dicrete time random walk treated o far, in the CTRW the number of jump n made by the walker
More informationA First Digit Theorem for Square-Free Integer Powers
Pure Matheatical Science, Vol. 3, 014, no. 3, 19-139 HIKARI Ltd, www.-hikari.co http://dx.doi.org/10.1988/p.014.4615 A Firt Digit Theore or Square-Free Integer Power Werner Hürliann Feldtrae 145, CH-8004
More informationStudy of a Freely Falling Ellipse with a Variety of Aspect Ratios and Initial Angles
Study of a Freely Falling Ellipe with a Variety of Apect Ratio and Initial Angle Dedy Zulhidayat Noor*, Ming-Jyh Chern*, Tzyy-Leng Horng** *Department of Mechanical Engineering, National Taiwan Univerity
More informationMATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.:
MATEMATIK Datum: 20-08-25 Tid: eftermiddag GU, Chalmer Hjälpmedel: inga A.Heintz Telefonvakt: Ander Martinon Tel.: 073-07926. Löningar till tenta i ODE och matematik modellering, MMG5, MVE6. Define what
More informationPulsed Magnet Crimping
Puled Magnet Crimping Fred Niell 4/5/00 1 Magnetic Crimping Magnetoforming i a metal fabrication technique that ha been in ue for everal decade. A large capacitor bank i ued to tore energy that i ued to
More information24P 2, where W (measuring tape weight per meter) = 0.32 N m
Ue of a 1W Laer to Verify the Speed of Light David M Verillion PHYS 375 North Carolina Agricultural and Technical State Univerity February 3, 2018 Abtract The lab wa et up to verify the accepted value
More information1.3.3 Statistical (or precision) uncertainty Due to transient variations, spatial variations 100%
1.1 Why eaure, and why tudy eaureent? 1. Introductory Exaple Exaple: Meauring your weight: The eaureent i not the thing. 1.3 Practical Source o Meaureent Uncertainty Exaple: Meauring T o roo. 1.3.1 Reading
More informationBogoliubov Transformation in Classical Mechanics
Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How
More informationConvergence of a Fixed-Point Minimum Error Entropy Algorithm
Entropy 05, 7, 5549-5560; doi:0.3390/e7085549 Article OPE ACCESS entropy ISS 099-4300 www.dpi.co/journal/entropy Convergence of a Fixed-Point Miniu Error Entropy Algorith Yu Zhang, Badong Chen, *, Xi Liu,
More informationOne Class of Splitting Iterative Schemes
One Cla of Splitting Iterative Scheme v Ciegi and V. Pakalnytė Vilniu Gedimina Technical Univerity Saulėtekio al. 11, 2054, Vilniu, Lithuania rc@fm.vtu.lt Abtract. Thi paper deal with the tability analyi
More informationPhysics 20 Lesson 16 Friction
Phyic 0 Leon 16 riction In the previou leon we learned that a rictional orce i any orce that reit, retard or ipede the otion o an object. In thi leon we will dicu how riction reult ro the contact between
More informationMODE SHAPE EXPANSION FROM DATA-BASED SYSTEM IDENTIFICATION PROCEDURES
Mecánica Coputacional Vol XXV, pp. 1593-1602 Alberto Cardona, Norberto Nigro, Victorio Sonzogni, Mario Storti. (Ed.) Santa Fe, Argentina, Noviebre 2006 MODE SHAPE EXPANSION FROM DATA-BASED SYSTEM IDENTIFICATION
More informationLEARNING DISCRIMINATIVE BASIS COEFFICIENTS FOR EIGENSPACE MLLR UNSUPERVISED ADAPTATION. Yajie Miao, Florian Metze, Alex Waibel
LEARNING DISCRIMINATIVE BASIS COEFFICIENTS FOR EIGENSPACE MLLR UNSUPERVISED ADAPTATION Yajie Miao, Florian Metze, Alex Waibel Language Technologie Intitute, Carnegie Mellon Univerity, Pittburgh, PA, USA
More informationLaplace Transformation
Univerity of Technology Electromechanical Department Energy Branch Advance Mathematic Laplace Tranformation nd Cla Lecture 6 Page of 7 Laplace Tranformation Definition Suppoe that f(t) i a piecewie continuou
More informationBayesian Reliability Estimation of Inverted Exponential Distribution under Progressive Type-II Censored Data
J. Stat. Appl. Pro. 3, No. 3, 317-333 (2014) 317 Journal of Statitic Application & Probability An International Journal http://dx.doi.org/10.12785/jap/030303 Bayeian Reliability Etiation of Inverted Exponential
More informationOn the Use of High-Order Moment Matching to Approximate the Generalized-K Distribution by a Gamma Distribution
On the Ue of High-Order Moent Matching to Approxiate the Generalized- Ditribution by a Gaa Ditribution Saad Al-Ahadi Departent of Syte & Coputer Engineering Carleton Univerity Ottawa Canada aahadi@ce.carleton.ca
More informationRelated Rates section 3.9
Related Rate ection 3.9 Iportant Note: In olving the related rate proble, the rate of change of a quantity i given and the rate of change of another quantity i aked for. You need to find a relationhip
More information7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281
72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition
More informationPrivacy-Preserving Point-to-Point Transportation Traffic Measurement through Bit Array Masking in Intelligent Cyber-Physical Road Systems
Privacy-Preerving Point-to-Point Tranportation Traffic Meaureent through Bit Array Making in Intelligent Cyber-Phyical Road Syte Yian Zhou Qingjun Xiao Zhen Mo Shigang Chen Yafeng Yin Departent of Coputer
More informationBUBBLES RISING IN AN INCLINED TWO-DIMENSIONAL TUBE AND JETS FALLING ALONG A WALL
J. Autral. Math. Soc. Ser. B 4(999), 332 349 BUBBLES RISING IN AN INCLINED TWO-DIMENSIONAL TUBE AND JETS FALLING ALONG A WALL J. LEE and J.-M. VANDEN-BROECK 2 (Received 22 April 995; revied 23 April 996)
More informationPPP AND UNIT ROOTS: LEARNING ACROSS REGIMES
PPP AND UNIT ROOTS: LEARNING ACROSS REGIMES GERALD P. DYWER, MARK FISHER, THOMAS J. FLAVIN, AND JAMES R. LOTHIAN Preliinary and incoplete Abtract. Taking a Bayeian approach, we focu on the inforation content
More informationSEISMIC GUIDELINES FOR TUNNELS ON ROCK
October 1-17, 008, Beijing, hina SEISMI GUIDELINES FOR TUNNELS ON ROK Nava-Tritán O. E. 1, Ulie Mena Hernández 1, Enrique Mena Sandoval and Elia Andrade 1 Reearcher, Gerencia de Ingeniería ivil, Intituto
More informationResearch Article Numerical and Analytical Study for Fourth-Order Integro-Differential Equations Using a Pseudospectral Method
Matheatical Proble in Engineering Volue 213, Article ID 43473, 7 page http://d.doi.org/1.11/213/43473 Reearch Article Nuerical and Analytical Study for Fourth-Order Integro-Differential Equation Uing a
More informationIntroduction to Laplace Transform Techniques in Circuit Analysis
Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found
More informationAN EASY INTRODUCTION TO THE CIRCLE METHOD
AN EASY INTRODUCTION TO THE CIRCLE METHOD EVAN WARNER Thi talk will try to ketch out oe of the ajor idea involved in the Hardy- Littlewood circle ethod in the context of Waring proble.. Setup Firt, let
More information_10_EE394J_2_Spring12_Inertia_Calculation.doc. Procedure for Estimating Grid Inertia H from Frequency Droop Measurements
Procedure or Etiating Grid Inertia ro Frequency Droop Meaureent While the exion or inertia and requency droop are well known, it i prudent to rederive the here. Treating all the grid generator a one large
More informationPractice Problems Solutions. 1. Frame the Problem - Sketch and label a diagram of the motion. Use the equation for acceleration.
Chapter 3 Motion in a Plane Practice Proble Solution Student Textbook page 80 1. Frae the Proble - Sketch and label a diagra of the otion. 40 v(/) 30 0 10 0 4 t () - The equation of otion apply to the
More information( ) Zp THE VIBRATION ABSORBER. Preamble - A NEED arises: lbf in. sec. X p () t = Z p. cos Ω t. Z p () r. ω np. F o. cos Ω t. X p. δ s.
THE VIBRATION ABSORBER Preable - A NEED arie: Lui San Andre (c) 8 MEEN 363-617 Conider the periodic forced repone of a yte (Kp-Mp) defined by : 1 1 5 lbf in : 1 3 lb (t) It natural frequency i: : ec F(t)
More informationResearch Article Efficient Recursive Methods for Partial Fraction Expansion of General Rational Functions
Journal of Applied atheatic Volue 24, Article ID 89536, 8 page http://dx.doi.org/.55/24/89536 Reearch Article Efficient Recurive ethod for Partial Fraction Expanion of General Rational Function Youneng
More informationMath 273 Solutions to Review Problems for Exam 1
Math 7 Solution to Review Problem for Exam True or Fale? Circle ONE anwer for each Hint: For effective tudy, explain why if true and give a counterexample if fale (a) T or F : If a b and b c, then a c
More informationLOAD AND RESISTANCE FACTOR DESIGN APPROACH FOR FATIGUE OF MARINE STRUCTURES
8 th ACE pecialty Conference on Probabilitic Mechanic and tructural Reliability PMC2000-169 LOAD AND REITANCE FACTOR DEIGN APPROACH FOR FATIGUE OF MARINE TRUCTURE Abtract I.A. Aakkaf, G. ACE, and B.M.
More informationADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR
ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR SAEED ABAZARI MOHSEN HEIDARI NAVID REZA ABJADI Key word: Adaptive control Lyapunov tability Tranient tability Mechanical power. The operating point of
More informationV = 4 3 πr3. d dt V = d ( 4 dv dt. = 4 3 π d dt r3 dv π 3r2 dv. dt = 4πr 2 dr
0.1 Related Rate In many phyical ituation we have a relationhip between multiple quantitie, and we know the rate at which one of the quantitie i changing. Oftentime we can ue thi relationhip a a convenient
More informationPractice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4.
Chapter 5 Newton Law Practice Proble Solution Student Textbook page 163 1. Frae the Proble - Draw a free body diagra of the proble. - The downward force of gravity i balanced by the upward noral force.
More informationPractice Midterm #1 Solutions. Physics 6A
Practice Midter # Solution Phyic 6A . You drie your car at a peed of 4 k/ for hour, then low down to k/ for the next k. How far did you drie, and what wa your aerage peed? We can draw a iple diagra with
More informationFrequency Response Analysis of Linear Active Disturbance Rejection Control
Senor & Tranducer, Vol. 57, Iue, October 3, pp. 346-354 Senor & Tranducer 3 by IFSA http://www.enorportal.co Freuency Repone Analyi of Linear Active Diturbance Reection Control Congzhi HUANG, Qing ZHENG
More informationFundamental Physics of Force and Energy/Work:
Fundamental Phyic of Force and Energy/Work: Energy and Work: o In general: o The work i given by: dw = F dr (5) (One can argue that Eqn. 4 and 5 are really one in the ame.) o Work or Energy are calar potential
More informatione st t u(t 2) dt = lim t dt = T 2 2 e st = T e st lim + e st
Math 46, Profeor David Levermore Anwer to Quetion for Dicuion Friday, 7 October 7 Firt Set of Quetion ( Ue the definition of the Laplace tranform to compute Lf]( for the function f(t = u(t t, where u i
More informationSecond Law of Motion. Force mass. Increasing mass. (Neglect air resistance in this example)
Newton Law of Motion Moentu and Energy Chapter -3 Second Law of Motion The acceleration of an object i directly proportional to the net force acting on the object, i in the direction of the net force,
More informationPHY 211: General Physics I 1 CH 10 Worksheet: Rotation
PHY : General Phyic CH 0 Workheet: Rotation Rotational Variable ) Write out the expreion for the average angular (ω avg ), in ter of the angular diplaceent (θ) and elaped tie ( t). ) Write out the expreion
More informationPHY 171 Practice Test 3 Solutions Fall 2013
PHY 171 Practice et 3 Solution Fall 013 Q1: [4] In a rare eparatene, And a peculiar quietne, hing One and hing wo Lie at ret, relative to the ground And their wacky hairdo. If hing One freeze in Oxford,
More informationLecture 7: Testing Distributions
CSE 5: Sublinear (and Streaming) Algorithm Spring 014 Lecture 7: Teting Ditribution April 1, 014 Lecturer: Paul Beame Scribe: Paul Beame 1 Teting Uniformity of Ditribution We return today to property teting
More information( 7) ( 9) ( 8) Applying Thermo: an Example of Kinetics - Diffusion. Applying Thermo: an Example of Kinetics - Diffusion. dw = F dr = dr (6) r
Fundamental Phyic of Force and Energy/Work: Energy and Work: o In general: o The work i given by: dw = F dr (5) (One can argue that Eqn. 4 and 5 are really one in the ame.) o Work or Energy are calar potential
More informationin a circular cylindrical cavity K. Kakazu Department of Physics, University of the Ryukyus, Okinawa , Japan Y. S. Kim
Quantization of electromagnetic eld in a circular cylindrical cavity K. Kakazu Department of Phyic, Univerity of the Ryukyu, Okinawa 903-0, Japan Y. S. Kim Department of Phyic, Univerity of Maryland, College
More informationSeat: PHYS 1500 (Fall 2006) Exam #2, V1. After : p y = m 1 v 1y + m 2 v 2y = 20 kg m/s + 2 kg v 2y. v 2x = 1 m/s v 2y = 9 m/s (V 1)
Seat: PHYS 1500 (Fall 006) Exa #, V1 Nae: 5 pt 1. Two object are oving horizontally with no external force on the. The 1 kg object ove to the right with a peed of 1 /. The kg object ove to the left with
More informationOptics. Measuring the velocity of light Geometrical Optics. What you need:
Geoetrical Optic Optic Meauring the velocity of light -01 What you can learn about Refractive index Wavelength Frequency Phae Modulation Electric field contant Magnetic field contant Principle: The intenity
More informationA Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems
A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement
More informationCONSOLIDATION ANALYSIS OF SOFT CLAY AT LARGE STRAIN
Proceeding of Softoil 04, October, -3 rd 04 CONSOLIDATION ANALYSIS OF SOFT CLAY AT LARGE STRAIN Yakin, Y. A., Djayaputra, A. A. and Rahardjo, P. P. 3 ABSTRACT: Settleent of oft oil caued by external load
More informationCalculation of the temperature of boundary layer beside wall with time-dependent heat transfer coefficient
Ŕ periodica polytechnica Mechanical Engineering 54/1 21 15 2 doi: 1.3311/pp.me.21-1.3 web: http:// www.pp.bme.hu/ me c Periodica Polytechnica 21 RESERCH RTICLE Calculation of the temperature of boundary
More informationOn the Pre-Exponential Factor Comparing in Thermoluminescence (TL) Theory
Open Acce Library Journal On the Pre-xponential Factor Comparing in hermoluminecence (L) heory ugenio Chiaravalle 1, ichele angiacotti 1, Claudio Furetta 2, Giuliana archeani 1, ichele omaiulo 1 1 Centro
More informationProperties of Amphoteric Surfactants Studied by ζ-potential Measurements with Latex Particles
1996 Langmuir 1998, 14, 1996-23 Propertie of Amphoteric Surfactant Studied by ζ-potential Meaurement with Latex Particle R. G. Alargova, I. Y. Vakarelky, V. N. Paunov, S. D. Stoyanov, P. A. Kralchevky,*,
More informationHOMEWORK ASSIGNMENT #2
Texa A&M Univerity Electrical Engineering Department ELEN Integrated Active Filter Deign Methodologie Alberto Valde-Garcia TAMU ID# 000 17 September 0, 001 HOMEWORK ASSIGNMENT # PROBLEM 1 Obtain at leat
More information