Numerical Investigation of Heat Transfer and Fluid Flow around the Rectangular Flat Plane Confined by a Cylinder under Pulsating Flow
|
|
- Loraine Armstrong
- 5 years ago
- Views:
Transcription
1 Journal of Alied Fluid Mechanic, Vol. 9, No., , 216. Available online at ISSN , EISSN DOI: /acadub.jafm Numerical Invetigation of Heat Tranfer and Fluid Flow around the Rectangular Flat Plane Confined by a Cylinder under Pulating Flow G. Li, Y. Zheng, H. Yang and Y. Xu Deartment of Energy and Environment Sytem Engineering, Zhejiang Univerity of Science and Technology, Hangzhou, 3123, P. R. China Correonding Author gnlene@163.com (Received October 8, 21; acceted October 1, 215) ABSTRACT Fluid flow around and heat tranfer from a rectangular flat lane with contant uniform heat flux in laminar ulating flow i tudied, and comared with our exerimental data. Quantitatively accurate, econd-order cheme for time, ace, momentum and energy are emloyed, and fine mehe are adoted. The numerical reult agree well with exerimental data. Reult found that the heat tranfer enhancement i caued by the relative low temerature gradient in the thermal boundary layer, and by the lower urface temerature in ulating flow. In addition, the heat tranfer reitance i much lower during revere flow eriod than that during forward flow eriod. The flow reveral eriod i about 18 degree behind the ulating reure wave. Beide, ectrum reult of the imulated averaged urface temerature howed that the temerature fluctuate in multile-eaked mode when the amlitude of the imoed ulation i larger, wherea the temerature fluctuate in a ingle-eaked mode when the amlitude of the imoed ulation i mall. Keyword: Pulating flow; Heat tranfer enhancement; Comutational fluid dynamic. NOMENCLATURE A D c f h H L Nu=hL/λ Nur=Nu/Nu q Re Rh,d Rh,t Rh,ave S h St T T Tw t ulating velocity comonent diameter of the airflow tunnel heat caacity of air ulating frequency convection coefficient height of the airflow tunnel length of the late heater Nuelt number heat tranfer enhancement factor reure amlitude Inut heat flux Reynold number time averaged heat reitance ace averaged heat reitance total averaged heat reitance area of the late heater heat ource Strouhal number tatic temerature inlet temerature averaged urface temerature time u u w y y + zb α λ ρ ε ν σb σ θ Subcrit rad rm intant velocity vector average inlet velocity axial velocity ditance of the firt grid centroid dimenionle ditance ditance along the flat lane abortivity of the heater thermal conductivity of air denity of air emiivity of the heater kinematic vicoity Stefan-Boltzmann cont thermal boundary layer thickne hae angle ulation radiation root mean quare teady
2 G. Li et al. / JAFM, Vol. 9, No., , INTRODUCTION The fluid flow and convective heat tranfer in ulating flow i encountered in many engineering alication, uch a the comact heat exchanger, cooling ytem of nuclear reactor, ule combutor, ule tube dry cooler, electronic cooling ytem and arterial flow inide human body. Therefore, great interet i being attracted to find out in what degree doe the ulation of airflow enhance the heat tranfer roce. Many analytical, exerimental and numerical tudie exit. However, due to it comlicated nature, i.e. many arameter of ulating flow affect the heat tranfer roce, reviou literature continue a to whether the ulation enhance the heat tranfer roce or not. In thoe work concluded in oitive effect by ulation, the exactly hyical mechanim of in what way doe the ulation enhance the heat tranfer roce i till unclear, and need further invetigation. Detail CFD (Comutational Fluid Dynamic) tudie are needed to find out thi mechanim. However, even CFD tudie of heat tranfer in ulating flow are difficult until the large comuter reource could be available in recent year. CFD tudie of heat tranfer need fine comutational grid, the length of which hould be much maller than the thickne of thermal boundary layer. Among thoe imortant ulating arameter affecting the heat tranfer roce, the ulating frequency and reure amlitude are two mot imortant one. However, reviou work how a variety of contradictory reult. In the exerimental tudie, (Habib et al. 22) invetigated the heat tranfer enhancement of a tube with uniform heat flux in laminar ulating flow at variou condition (f= Hz, Re= ). A heat tranfer model Nur = Nur (f, Re) wa develoed with the deviation of about 1% in different range of Reynold number. (Dec et al.1992) tudied the heat tranfer rate in ule combution tail ie in a erie of condition (f=67-11 Hz, Re=375). It concluded that the reure amlitude mut be trong enough to create flow reveral in order to obtain oitive heat tranfer enhancement factor. (Kearney et al. 21) invetigated the time reolved tructure of a thermal boundary layer in laminar ulating channel flow, concluding that the flow reveral i not neceary for heat tranfer enhancement. A few year later, (Moon et al. 25) confirmed Kearney concluion (Kearney et al. 21). Moon work reorted heat tranfer enhancement from a rectangular heated block array in a ulating channel flow at variou condition ( f=1-1 Hz, A=.2-.3). Reult howed that the heat tranfer enhancement factor can be larger than 1.2. Many other valuable exerimental tudie reorted an enhancement in heat tranfer due to the ulation (Zohir et al. 26, Ji et al. 28, Baffigi and Bartoli 21). However, ome tudie uch a Elayed et al. work (Elhafei et al. 28), reorted the ulation would downgrade the heat tranfer comared to that in teady flow. In analytical tudie, (Faghri et al. 1979) reorted that larger heat tranfer enhancement factor could be obtained at higher ulating frequency. However, (Hemida et al. 22) found that the heat tranfer enhancement factor increae with reure amlitude, but decreae with ulating frequency. Some tudie (Chang and Tucker, 2, Chattoadhyay et al. 26) reorted that the ulation ha no effect on the heat tranfer roce. Other work reented valuable analyi about the influence of Prandtl number (Moon et al. 25), hae lag and urface temerature ditribution (Nika et al. 27) on the heat tranfer roce. In numerical tudie, (Thyagewaran 2) develoed a near-wall turbulence model for heat tranfer in ulating flow. (Wang and Zhang 25) found that there i an otimum Womerley number at which heat tranfer i maximally enhanced, which i confirmed by Akdag work (Akdag 21). (Selimefendigil et al. 212) invetigated the nonlinearity of the unteady heat tranfer of a cylinder in ulating cro flow. They develoed an accurate, low-order model for the heat ource dynamic in a Rijke combutor, which i tudied carefully in one of our reviou work (Li et al. 28). The mechanim controlling the heat tranfer enhancement in ulating flow i unclear, and need to be further exlored. Exerimental data i limited, and it i difficult to meaure the velocity/temerature rofile inide the flow/thermal boundary layer. Few CFD tudie exit (Thyagewaran 2, Wang and Zhang 25, Akdag 21, Selimefendigil et al. 212), and more detail analyi i obviou needed, uch a the ulating mode of the temerature field, time evolution of thermal boundary layer and ace ditribution of heat tranfer reitance. In thi work, a detail CFD tudy wa carried out to exlore the mechanim controlling the heat tranfer in ulating flow. Numerical reult were comared with our exerimental data, and detail dicuion were made. 2. NUMERICAL MODEL Thi art reent the detail of the governing equation and the boundary condition. A brief introduction on the exerimental etu and exerimental rocedure i alo reented in order to make the reent tudied roblem more ecified. 2.1 Governing Equation Prediction of the fluid flow and heat tranfer in ulating flow require CFD comutation with a comreible flow model. However, uch comutation demand huge comutational reource, ince the heat tranfer in ulating flow involve variou hyical henomena covering a wide range of length and time cale. Conidering that the ulation wave length are much larger than the characteritic length of the lane heater, the unteady, incomreible Navier-Stoke equation along with the energy equation i olved with ANSYS-FLUENT 13. egregated olver, a follow, 157
3 G. Li et al. / JAFM, Vol. 9, No., , 216. Continuum equation ui x i Momentum conervation equation 2 u u i iu j 1 u i t x 2 j x i x j Energy conervation equation 2 T u jt k T 2 h t x j c x j (1) (2) (3) where i, j=1,2,3, ρ i the air kinetic vicoity, c i the heat caacity, u i air flow velocity vector, x denote the atial coordinate, tand for tatic reure, T i the tatic temerature. Combining with very fine mehe, the laminar flow method give direct numerical imulation reult. In thi work, relative fine mehe, econd-order cheme for time, ace, momentum and energy, are ued. Such comutation allow week turbulence to be roerly olved under the reent Reynold number of 219. Radiation i taken into conideration, and the P1 model i emloyed. The lane heater i uoed to be a grey obtacle, and the emiivity ε i et to be.68 (Jone et al. 1977). The heat ource in Eq. (3) i a follow (ANSYS Inc. 21), b h T T () c c Where σb i the Stefan-Boltzmann contant, ε and α i the emiivity and abortivity of heater, reectively. 2.2 Boundary Condition The comutational zone and the comutational mehe in the croing ection of the lane heater are hown in Fig. 1, which i conitent with the exerimental tet ection (Li et al. 21). The comutational zone i a circle channel with inner diameter D=68 mm and height H=21 mm. A rectangular lane heater with dimenion of 7 mm 2 mm 1.5 mm i fixed in the middle of the channel. The 7 mm ide of the heater i aligned with channel axi. The Reynold number baed on the averaged channel velocity and the channel diameter i 219. Conidering that the comutation hould cover detail information inide the boundary layer, the length cale of the firt grid around the heater fulfill the following demand (Breuer et al. 23) y<y=.283 mm y+=1 (5) y (u/νzb) -.5 (6) Where y i the ditance to the wall from the adjacent grid centroid, u i the averaged velocity inide the circle channel, and zb denote the ditance along the wall from the tarting oint of the boundary layer. Block artition grid method i emloyed to ave comuter reource and comutation time. The number of comutational mehe i about 2,5, with emhaize around the lane heater. The effect of the y / y + on the numerical reult when rm=75 Pa i hown in Table 1. A hown in Table 1, y / y + =.35 i fine enough ince the temerature difference i le than.5 K for the cae of y / y + =.28. Table 1 Effect of y / y + on the numerical reult y / y + Grow Factor Number of Grow Traniton attern Tw (K) : : : : : Fig. 1. Comutational zone and the meh ditribution in the croing ection. Temerature deended hyical roertie of air (Yang and Tao 1998) including denity, ecific heat caacity, thermal conductivity and vicoity, are ued with everal UDF (Uer Define Function) rogram. At the inlet and outlet, velocity inlet and reure outlet boundary condition are imoed, reectively. The ulation i imoed to the inlet uing a UDF rogram to create reure ocillation (Roux et al. 211), a follow, u(=u(1+ain2πf (7) where A denote the ulating comonent of velocity at the inlet urface. All UDF rogram are written in C language, and interret into the main rogram. The heat flux wall boundary condition i emloyed to decribe the heated lane, in which the wall temerature i calculated with the following equation (ANSYS Inc. 21), T w q q h rad T (8) where Tw i the wall temerature, q i total heat flux from the heated lane, which equal to. W in thi work. qrad i the radiation heat flux, which equal to h in Eq. (). h denote the convection heat tranfer coefficient. In thi work, the ulating frequency i maintained at 15 Hz, and A i modified to roduce different reure amlitude (
4 G. Li et al. / JAFM, Vol. 9, No., , 216. Pa) according to exerimental condition. Time te i et to be 1-3. The global convergence for continuity, momentum and energy reidual are et to be 1 -, 1 -, and 1-7, reectively. Detail of the exerimental etu and the exerimental rocedure can be found in our reviou tudie (Li et al. 21, Li et al. 213). In brevity, the air flow rate i et to be ml/ by a ma flow controller. Two-tage erforated late are intalled to inure the uniformity of inlet airflow. A High Temerature Co-fired Ceramic (HTCC) rectangular lane heater with ame dimenion a Fig. 1 i fixed in the middle of the channel. A loudeaker i intalled utream the inlet to roduce ulating wave. A corrugated vibration-abortive tube i intalled to avoid vibration tranmiion from the loudeaker to the HTCC heater. A reure tranducer i intalled to meaure the reure wave. Then ectrum analyi i carried out to find out the ulating frequency and reure amlitude. The ower of the HTCC heater i ket to be.w, and the ulating frequency i maintained at f=15 Hz, and the reure amlitude, rm, i varied in the range of Pa. All meaured exerimental data have an inaccuracy le than.1% (Li et al. 21). 3. RESULTS AND DISCUSSIONS Verification of the CFD model i reented at firt with the hel of exerimental data. Then the temerature ditribution and the temerature ulating mode are dicued. Finally, the mechanim of heat tranfer enhancement in ulating flow i exlored. 3.1 Verification of CFD Model The imulated averaged urface temerature and the exerimental data i hown in Fig. 2. The heat tranfer enhancement factor Nur can be calculated with above temerature data, which i hown in Fig. 3. The calculation follow the following formula,. q S T T ) h( T T ) (9) b ( hl Nu (1) Nu Nur Nu q q b b A( T A( T T ) ( T T ) ( T T ) T ) (11) where q and T are the conumed ower of the lane heater and the averaged urface temerature of the HTCC heater in ulating airflow, reectively, wherea the q and T are the correonding value in teady airflow, reectively. λ and λ are the heat conductivity of the air in ulating airflow and in teady airflow, reectively. T i the temerature of inlet airflow, and it i maintained at K. A hown in Fig. 2, the imulated temerature agree well with the exerimental data. However, CFD comutation over-redict (about 3. K, le than 1.%) the averaged urface temerature in ulating condition with large reure amlitude (rm 1 Pa). A a reult, the imulated heat tranfer enhancement factor i under-redicted (about 1.%) in thoe cae, hown in Fig. 3. Thi finding reveal that the accurate rediction of temerature field i critical to redict the heat tranfer enhancement factor. Fig. 2. Comarion between imulated averaged urface temerature and exerimental data. Fig. 3. Comarion between imulated heat tranfer enhancement factor and exerimental data. Small dicreancy of temerature field could caue very large difference in rediction of heat tranfer enhancement factor. Therefore, fine comutational mehe, eecially around the heater, hould be adoted. It i exected that the averaged urface temerature i alo time deended. In other word, Fig. 2 reent the averaged value of the averaged urface temerature. The firt average refer to time averaged value, and the econd average refer to atial averaged value. The time evolution of the imulated averaged urface temerature (atial averaged) i hown in Fig.. Single-eaked fluctuation (15 Hz) could be found in ulating condition with low reure amlitude ( rm 5 Pa). However, econd harmonic fluctuation are obviouly excited when the reure amlitude i 1572
5 G. Li et al. / JAFM, Vol. 9, No., , 216. large ( rm 1Pa). The eak-eak amlitude (about 3. K to 7. K) of the averaged urface temerature decreae firtly, and then increae with the reure amlitude. The correonding ectrum analyzed reult are hown in Fig. 5. The temerature amlitude at 15 Hz decreae firtly, and then increae with reure amlitude. However, the temerature amlitude at 3 Hz i larger than that at 15 Hz when the reure amlitude lie between 1 Pa and 175 Pa. Thi henomenon i accomanied by the dicreancy between imulated averaged urface temerature and the exerimental data. However, there are no evidence to correlate thee two henomena, and thi need to be further tudied. frequency of the CFD comutation i 1-3 and 15 Hz, reectively. Obviou difference can be found in Fig. 6. The temerature level of the averaged temerature field in ulating condition i much lower than that in teady flow condition. Therefore, it worth to robe into the ulation mode of the temerature field in ulating condition. Firtly, a ul-ation cycle wa elected when the reure amlitude equal 75 Pa, which i hown in Fig. 7. Fig. 7 alo reent the time evolution of z-velocity. Secondly, eight intant are elected, which are hown in Fig. 7, marked with mall circle. (a) Steady (b) Pulation Fig.. Time hitory of the imulated averaged urface temerature. Fig. 6. Temerature field of the teady tate and the averaged temerature field of the ulating tate when rm=75 Pa. Fig. 5. Sectrum reult of the imulated averaged urface temerature ulation. 3.2 Temerature Field The averaged temerature field in the lane of x= m i reented in Fig. 6. In the teady flow condition, the temerature increae in the z direction near the wall urface, and the temerature ditribution hae i conitent with thoe in textbook. In the ulating condition, the temerature field i an averaged temerature field from 66 intant temerature field within a ulation cycle, ince the time te and ulating Fig. 7. One ulation cycle for the tudy of temerature field when rm=75 Pa The correonding 8 temerature field are hown in Fig. 8. The local temerature near the wall along the z direction could reach 38 K ( θ=, θ=.96π), however, the averaged local temerature are le than 33 K hown in Fig. 6. The temerature field fluctuate with time, and aear in a ecial mode. In the firt half cycle of reure wave, heated area locate in the utream zone when the flow i in forward, wherea thee area change to locate in 1573
6 G. Li et al. / JAFM, Vol. 9, No., , 216. the downtream zone in the econd half cycle when the flow i in reveral. much larger than that in teady flow condition, which i hown in Fig. 1. Conidering that the heat tranfer reitance i direct roortional with the temerature difference, and i invere roortional with boundary layer thickne. Therefore, the heat tranfer reitance in ulating condition i much le than that in teady flow condition. Fig. 9. Ditribution of the imulated temerature in the line (y=-.75 m, x= m,.7 m z.1 m) in the teady tate and in the ulation tate when rm=75 Pa. Fig. 8. Ocillating temerature field during one cycle in the lane of x= m when rm=75 Pa Thi imlie that the flow reveral occurred in the econd half cycle, in other word, the flow reveral i inconitent with the oitive reure wave. One oible mechanim for the dilacement between the ocillating temerature and the flow reveral may caued by the inconitent between the reure-induced ulating velocity and the ulating reure during one cycle. The highet reure occur when the higher temerature fluid i in the utream zone, acting a a iton to the incoming fluid. Thi i confirmed in Fig According the reviou tudie (Pedley, 1976), the actual ulating velocity amlitude deart from the reure-baed ulating velocity amlitude excited by reure gradient when the Strouhal number St >.3, and lag behind the ulating reure wave. In the reent work, the etimated Strouhal number i larger than 2., therefore, the flow reveral lag behind the ulating reure wave, and cauing the above ocillating temerature mode. The ditribution of imulated temerature near the left ide of lane heater i hown in Fig. 9. In teady flow condition, the temerature increae harly along the heater, and then increaed in a tender way. However, the temerature ditribution i very flat in the ulating condition. In order to find out the mechanim controlling the heat tranfer enhancement in ulating flow, thermal boundary need to be tudied. The averaged thickne of thermal boundary layer in ulating condition i Fig. 1. Ditribution of the imulated thermal boundary layer thickne in the area (y< m, x= m,.7 m z.1 m) in the teady tate and in the ulation tate when rm=75 Pa. 3.3 Heat Tranfer Enhancement Mechanim A hown in Fig. 3, both the exeriment and CFD comutation how that the heat tranfer could be enhanced greatly in ulating flow. However, the mechanim controlling thi enhancement i till unclear. In order to make ome dicuion, everal ecified heat tranfer reitance are defined a follow, R h, d Tw ( z, dt ( z, (12) 157
7 G. Li et al. / JAFM, Vol. 9, No., , 216. R R h, t h, ave Tw ( z, dz ( z, Tw ( z, dzdt ( z, (13) (1) where the temerature of K i the definition of the location of thermal boundary, and equal to 11% of the inlet temerature. Rh,d, Rh,t and Rh,ave are the time averaged heat tranfer reitance, ace averaged heat tranfer reitance and total averaged heat tranfer reitance, reectively. Tw i the urface temerature, and δ i the thickne of thermal boundary layer. Time averaged heat tranfer reitance and ace averaged heat tranfer reitance are hown in Fig. 11 and Fig. 12, reectively. In teady flow condition, the curve in Fig are calculated from Fig. 6(a). In ulating condition, the curve in Fig are calculated from 66 intant cae within a comlete cycle hown in Fig. 7. It hould be reminded that Fig.11 how the atial ditribution of the heat tranfer reitance and Fig.12 how the time evolution of the heat tranfer reitance. time. However, the heat tranfer reitance in anytime i lower than that in teady flow condition. Reult found that the heat tranfer reitance i much lower during revere flow eriod than that during forward flow eriod. The flow reveral eriod i about 18 degree behind the ulating reure wave. Thi finding exand the concluion of reviou work (Dec et al. 1992, Thyagewaran 2, Wang and Zhang 25, Akdag 21, Selimefendigil et al. 212), i.e. the finding in thi work reveal that the heat tranfer i more enhanced in flow reveral eriod during one ulation cycle. Fig. 12. Evolution of the imulated heat reitance in ulation cycle when rm=75 Pa.. CONCLUSION Fig. 11. Ditribution of the imulated heat reitance in the teady tate and in the ulation tate when rm=75 Pa. The heat tranfer reitance hown in Fig. 11 decreae along the lane heater in both teady and ulating flow condition. A hown in Fig. 9-1, the temerature increae along the heater, while the boundary thickne alo increae along the heater, which i invere roortional to the heat tranfer reitance. In other word, the temerature gradient inide the thermal boundary layer i the dominant arameter. The final reult reveal that the temerature gradient in ulating flow i much le than that in teady flow condition. The total averaged heat tranfer reitance i 155 K/m 2 in teady flow condition, while it equal to 552 K/m 2 in ulating flow condition. Thi imlie that the heat tranfer enhancement in ulating flow i generated by larger maller temerature gradient in the thermal boundary layer, and by lower urface temerature. It i worth to find out which time create the lowet heat tranfer reitance during one ulation cycle. A hown in Fig. 12, ace averaged heat tranfer reitance fluctuate with The heat tranfer from a rectangular lane heater in teady and ulating flow i exlored numerically and exerimentally. Fine comutational mehe, econd-order cheme for time, ace, momentum and energy, are emloyed. The numerical reult agree well with exerimental data. Several concluion are drawn a follow, (1) Heat tranfer enhancement in ulating flow i generated by relative low temerature gradient in the thermal boundary layer, and by lower urface temerature. (2) Heat tranfer reitance i much lower during the revere flow eriod than that during forward flow eriod. In addition, the flow reveral eriod i about 18 degree behind the ulating reure wave. (3) The imulated ace averaged urface temerature of the lane heater i time variant, and fluctuate in multile-eaked mode when the amlitude of the imoed ulation wa larger enough. ACKNOWLEDGEMENTS Thi work ha been uorted by the National Natural Science Foundation of China ( , , 51161), the Zhejiang Provincial Natural Science Foundation of China (Z111695), 1575
8 G. Li et al. / JAFM, Vol. 9, No., , 216. and the Cro Reearch Foundation of Zhejiang Univerity of Science and Technology (213JC2Z). REFERENCES Akdag, U. (21). Numerical invetigation of ulating flow around a dicrete heater in a channel. International Communication in Heat and Ma Tranfer 37(7), ANSYS Inc. (21). ANSYS FLUENT uer' guide. Baffigi, F. and C. Bartoli (21). Heat tranfer enhancement in natural convection between vertical and down inclined wall and air by ulating jet. Exerimental Thermal and Fluid Science 3(7), Breuer, M., N. Jovičić and K. Mazaev (23). Comarion of DES, RANS and LES for the earated flow around a flat at high incidence. International Journal for Numerical Method in Fluid 1(), Chang, Y. M. and P. G. Tucker (2). Numerical tudie of heat tranfer enhancement in laminar earated flow. International Journal of Heat and Fluid Flow 25(1), Chattoadhyay, H., F. Durt and S. Ray (26). Analyi of heat tranfer in imultaneouly develoing ulating laminar flow in a ie with contant wall temerature. International Communication in Heat and Ma Tranfer 33(), Dec, J. E., J. O. Keller and V. S. Aaci (1992). Heat tranfer enhancement in the ocillating turbulent flow of a ule combutor tail ie. International Journal of Heat and Ma Tranfer 35(9), Elhafei, E. A. M., M. S. Mohamed, H. Manour and M. Sakr (28) Exerimental tudy of heat tranfer in ulating turbulent flow in a ie. International journal of heat and fluid flow 29(), Faghri, M., K. Javadani and A. Faghri (1979). Heat tranfer with laminar ulating flow in a ie. Letter in Heat and Ma Tranfer 6(), Habib, M. A., A. M. Attya, A. I. Eid and A. Z. Aly (22). Convective heat tranfer characteritic of laminar ulating ie air flow. Heat and Ma Tranfer 38(3), Hemida, H. N., M. N. Sabry, A. A. Abel-Rahim and H. Manour (22). Theoretical analyi of heat tranfer in laminar ulating flow. International Journal of Heat and Ma Tranfer 5 (8), Ji, T. H., S. Y. Kim and J. M. Hyun (28). Exeriment on heat tranfer enhancement from a heated quare cylinder in a ulating channel flow. International Journal of Heat and Ma Tranfer 51(5-6), Jone, A. M., I. E. Smith and S. D. Probert (1977). External thermograhy of building and tructure a a mean of determining their heat loe. In Society of Photo Otical Intrumentation Engineer (ed.), Proceeding of a Symoium on Indutrial and Civil Alication of Infrared Technology, Michigan, USA Kearney, S. P., A. M. Jacobi and R. P. Lucht (21). Time-reolved thermal boundary layer tructure in a ulatile revering channel flow. Journal of Heat Tranfer 123(), Li, G. N., H. Zhou and K. F. Cen. (28). Characteritic of acoutic behavior, combution comletene and emiion in a Rijke-tye combutor. Alied Thermal Engineering 28(17-18), Li, G. N., Y. Q. Zheng, G. L. Hu (213). Exerimental invetigation on heat tranfer enhancement from an inclined heated cylinder with contant heat inut ower in infraonic ulating flow. Exerimental Thermal and Fluid Science 9(1), Li, G. N., Y. Q. Zheng, G. L. Hu (21). Heat tranfer enhancement from a rectangular flat late with contant heat flux in ulating flow. Exerimental Heat Tranfer 27(2), Moon, J. W., S. Y. Kim and H. H. Cho (25). Frequency-deendent heat tranfer enhancement from rectangular heated block array. International Journal of Heat and Ma Tranfer 8(23-2), Mochandreou, T. and M. Zamir (1997). Heat tranfer in a tube with ulating flow and contant heat flux. International Journal of Heat and Ma Tranfer (1), Nika, P., Y. Bailly, F. Guermeur (27). Wall and fluid inlet temerature effect on heat tranfer in incomreible laminar ocillating flow. International Journal of Refrigeration 3(6), Pedley, T. J. (1976). Heat tranfer from a hot film in revering hear flow. Journal of Fluid Mechanic 78(3), Roux, S., M. Fénot, G. Lalizel (211). Exerimental invetigation of the flow and heat tranfer of an iminging jet under acoutic excitation. International Journal of Heat and Ma Tranfer 5 (15-16), Selimefendigil, F., S. F. Öller and W. Polifke (212). Nonlinear identification of unteady heat tranfer of a cylinder in ulating cro flow. Comuter and Fluid 53(1), 1-1. Thyagewaran, S. (2). Numerical modeling of ule combutor tail ie heat tranfer. International Journal of Heat and Ma Tranfer 7(12-13), Wang, X. and N. Zhang (25). Numerical analyi of heat tranfer in ulating turbulent flow in a 1576
9 G. Li et al. / JAFM, Vol. 9, No., , 216. ie. International Journal of Heat and Ma Tranfer 8(19-2), Yang, S. M. and W. Q. Tao (1998). Heat tranfer (the 3rd edition). Beijing, China: Higher education re. Zohir, A. E., M. A. Habib, A. M. Atty and A. L. Eid (26). An exerimental invetigation of heat tranfer to ulating ie air flow with different amlitude. Heat and Ma Tranfer 2(7),
ME 3560 Fluid Mechanics
Sring 018 ME 3560 Fluid Mechanic Chater III. Elementary Fluid Dynamic The Bernoulli Equation 1 Sring 018 3.1 Newton Second Law A fluid article can exerience acceleration or deceleration a it move from
More informationFigure 1 Siemens PSSE Web Site
Stability Analyi of Dynamic Sytem. In the lat few lecture we have een how mall ignal Lalace domain model may be contructed of the dynamic erformance of ower ytem. The tability of uch ytem i a matter of
More informationRADIATION THERMOMETRY OF METAL IN HIGH TEMPERATURE FURNACE
XVII IMEKO World Congre Metrology in the 3rd Millennium June 22 27, 2003, Dubrovnik, Croatia RADIATION THERMOMETRY OF METAL IN HIGH TEMPERATURE FURNACE Tohru Iuchi, Tohru Furukawa and Nobuharu Sato Deartment
More informationSolved problems 4 th exercise
Soled roblem th exercie Soled roblem.. On a circular conduit there are different diameter: diameter D = m change into D = m. The elocity in the entrance rofile wa meaured: = m -. Calculate the dicharge
More informationUSE OF INTERNET TO DO EXPERIMENTS IN DYNAMICS AND CONTROL FROM ZACATECAS MEXICO IN THE LABORATORY OF THE UNIVERSITY OF TENNESSEE AT CHATANOOGAA.
USE OF INTERNET TO DO EXPERIMENTS IN DYNAMICS AND CONTROL FROM ZACATECAS MEXICO IN TE LABORATORY OF TE UNIVERSITY OF TENNESSEE AT CATANOOGAA. Jim enry *, Joé Alberto González Guerrero, Benito Serrano Roale..
More informationLecture 10. Erbium-doped fiber amplifier (EDFA) Raman amplifiers Have replaced semiconductor optical amplifiers in the course
ecture 1 Two tye of otical amlifier: Erbium-doed fiber amlifier (EDFA) Raman amlifier Have relaced emiconductor otical amlifier in the coure Fiber Otical Communication ecture 1, Slide 1 Benefit and requirement
More informationVolume IV, Issue IX, September 2015 IJLTEMAS ISSN
Volume IV, Iue IX, Setember 15 IJLEMAS ISSN 78-54 A Comutational Study of A Multi Solid Wall Heat Conduction Made U of Four Different Building Contruction Material Subected to Variou hermal Boundary Condition.
More informationEstimating Conditional Mean and Difference Between Conditional Mean and Conditional Median
Etimating Conditional Mean and Difference Between Conditional Mean and Conditional Median Liang Peng Deartment of Ri Management and Inurance Georgia State Univerity and Qiwei Yao Deartment of Statitic,
More informationDesign of Two-Channel Low-Delay FIR Filter Banks Using Constrained Optimization
contrained otimization, CIT Journal of Comuting and Information Technology, vol. 8, no 4,. 34 348, 2. Deign of Two-Channel Low-Delay FIR Filter Bank Uing Contrained Otimization Abtract Robert Bregović
More informationMANUFACTURING TOLERANCES AS A CAUSE FOR AUDIBLE NOISE OF INDUCTION MOTORS
MANUFACTURING TOLERANCES AS A CAUSE FOR AUDIBLE NOISE OF INDUCTION MOTORS Delaere K., Franen J., Hameyer K., Belman R. Katholieke Univeriteit Leuven, De. EE (ESAT) Div. ELEN, Kardinaal Mercierlaan 94,
More informationME 315 Exam 3 8:00-9:00 PM Thursday, April 16, 2009 CIRCLE YOUR DIVISION
ME 315 Exam 3 8:00-9:00 PM Thurday, Aril 16, 009 Thi i a cloed-book, cloed-note examination. There i a formula heet at the back. You mut turn off all communication device before tarting thi exam, and leave
More informationTemperature Sensitive Paint Heat Flux Measurements in Hypersonic Tunnels
Temerature Senitive Paint Heat Flux Meaurement in Hyeronic Tunnel Tianhu Liu, Z. Cai, B. Wang Wetern Michigan Univerity, Kalamazoo, MI 49008 J. Rubal, J. P. Sullivan, S. Schneider Purdue Univerity, Wet
More informationComputational fluid dynamics simulation of a very dense liquid-solid flow using a Eulerian model
Comutational Method in Multihae Flow III 305 Comutational fluid dynamic imulation of a very dene liuid-olid flow uing a Eulerian model J. Yang & R. J. Chalaturnyk Deartment of Civil and Environmental Engineering,
More informationInvestigation on thermal effects in high power Yb-doped fiber laser. Usha Chakravarty,* B. N. Upadhyaya, A. Kuruvilla, S. M. Oak
Invetigation on thermal effect in high ower Yb-doed fiber laer Uha Chakravarty,* B. N. Uadhyaya, A. Kuruvilla, S. M. Oak Solid State Laer Diviion, Raja Ramanna Centre for Advanced Technology, Indore-452013
More informationROOT LOCUS. Poles and Zeros
Automatic Control Sytem, 343 Deartment of Mechatronic Engineering, German Jordanian Univerity ROOT LOCUS The Root Locu i the ath of the root of the characteritic equation traced out in the - lane a a ytem
More informationFluids Lab 1 Lecture Notes
Fluid Lab Lecture Note. Bernoulli Equation. Pitot-Static Tube 3. Aireed Meaurement 4. Preure Nondimenionalization Reference: Anderon 3.-3.5, Denker 3.4 ( htt://www.av8n.com/how/ ) Bernoulli Equation Definition
More informationFluid-structure coupling analysis and simulation of viscosity effect. on Coriolis mass flowmeter
APCOM & ISCM 11-14 th December, 2013, Singapore luid-tructure coupling analyi and imulation of vicoity effect on Corioli ma flowmeter *Luo Rongmo, and Wu Jian National Metrology Centre, A*STAR, 1 Science
More informationOperational transconductance amplifier based voltage-mode universal filter
Indian Journal of Pure & Alied Phyic ol. 4, etember 005,. 74-79 Oerational tranconductance amlifier baed voltage-mode univeral filter Naeem Ahmad & M R Khan Deartment of Electronic and Communication Engineering,
More informationNumerical Simulation of Triaxial Compression Stress Paths Tests for Unsaturated Soil
Numerical Simulation of Triaxial Comreion Stre Path Tet for Unaturated Soil Dong Jian-jun Key Laboratory Of Mechanical Reliability For Heavy Equiment And Large Structure of Hebei Province, Yanhan Univerity,
More informationExternal Flow: Flow over Bluff Objects (Cylinders, Spheres, Packed Beds) and Impinging Jets
External Flow: Flow over Bluff Object (Cylinder, Sphere, Packed Bed) and Impinging Jet he Cylinder in Cro Flow - Condition depend on pecial feature of boundary layer development, including onet at a tagnation
More informationUSEFUL TECHNIQUES FOR FIELD ANALYSTS IN THE DESIGN AND OPTIMIZATION OF LINEAR INDUCTION MOTORS
USEFUL TECHNIQUES FOR FIELD ANALYSTS IN THE DESIGN AND OPTIMIZATION OF LINEAR INDUCTION MOTORS By: K.R. Davey R.C. Zowarka Twelfth Biennial IEEE Conference on Electromagnetic Field Comutation (CEFC 006),
More informationModeling of Transport and Reaction in a Catalytic Bed Using a Catalyst Particle Model.
Excerpt from the Proceeding of the COMSOL Conference 2010 Boton Modeling of Tranport and Reaction in a Catalytic Bed Uing a Catalyt Particle Model. F. Allain *,1, A.G. Dixon 1 1 Worceter Polytechnic Intitute
More informationDiscovery Mass Reach for Excited Quarks at Hadron Colliders
Dicovery Ma Reach for Excited Quark at Hadron Collider Robert M. Harri Fermilab, Batavia, IL 60510 ABSTRACT If quark are comoite article then excited tate are exected. We etimate the dicovery ma reach
More informationSimulation of Wound Rotor Synchronous Machine under Voltage Sags
Simulation of Wound Rotor Synchronou Machine under oltage Sag D. Aguilar, G. azquez, Student Member, IEEE, A. Rolan, Student Member, IEEE, J. Rocabert, Student Member, IEEE, F. Córcole, Member, IEEE, and
More informationMAE 101A. Homework 3 Solutions 2/5/2018
MAE 101A Homework 3 Solution /5/018 Munon 3.6: What preure gradient along the treamline, /d, i required to accelerate water upward in a vertical pipe at a rate of 30 ft/? What i the anwer if the flow i
More informationFluid Detection in Tight Gas Sand from the Seismic Data
Fluid Detection in Tight Ga Sand from the Seimic Data Jiang Ren, Zeng Qingcai, Ouyang Yonglin, Huang Jiaqiang, Heei, Hu Xinhai Reearch Intitute of Petroleum Exloration and Develoment-LangFang, Lang Fang
More informationSimulation model of Heat Transfer through the Wall
Proceeding of the International Conference on Alied Mathematic and Comutational Method Simulation model of Heat Tranfer through the Wall Jana Mižáková Stella Hrehová Aleander Hošovký Deartment of Mathematic
More informationRadiation Heat Transfer
CM30 ranport I Part II: Heat ranfer Radiation Heat ranfer Profeor Faith Morrion Department of Chemical Engineering Michigan echnological Univerity CM30 ranport Procee and Unit Operation I Part : Heat ranfer
More informationUncertainty Analysis in Potential Transformer Calibration Using a High Voltage Capacitance Bridge
Journal of Electrical Engineering & Technology, ol., No. 3,. 4~47, 4 Uncertainty Analyi in Potential Tranformer Caliration Uing a High oltage Caacitance Bridge Jae Ka Jung, Sang Hwa Lee*, Jeon Hong Kang*,
More informationp and transverse momentum p BF
Strangene roduction at high Q with the H detector Julia E. Ruiz abaco Centro de Invetigacione y Etio Avanzado del Intituto Politécnico Nacional Antigua carretera a Progreo Km. 6 97, Mérida, Yucatán, México
More informationResearch on DC resistivity for an arbitrarily anisotropic earth using circular scanning measurement
Reearch on DC reitivity for an arbitrarily aniotroic earth uing circular canning meaurement Zhilong Yang* Changchun Yin Xiuyan Ren Changkai Qiu Xiaoyue Cao Jilin Univerity Jilin Univerity Jilin/RMIT Univerity
More informationBandwidth expansion of a pressure control system for pneumatic anti-vibration apparatuses in presence of dead time
23456789 Bulletin of the JSME Journal of Advanced Mechanical Deign, Sytem, and Manufacturing Vol.9, No.3, 25 Bandwidth exanion of a reure control ytem for neumatic anti-vibration aaratue in reence of dead
More informationMicrowave magnetoelectric fields: An analytical study of topological characteristics
Microwave magnetoelectric field: An analytical tudy of toological characteritic R. Joffe 1,, R. Shavit 1, and E. O. Kamenetkii 1, 1 Microwave Magnetic Laboratory, Deartment of Electrical and Comuter Engineering,
More informationCHAPTER 4 COMPARISON OF PUSH-OUT TEST RESULTS WITH EXISTING STRENGTH PREDICTION METHODS
CHAPTER 4 COMPARISON OF PUSH-OUT TEST RESULTS WITH EXISTING STRENGTH PREDICTION METHODS 4.1 General Several tud trength rediction method have been develoed ince the 1970. Three o thee method are art o
More informationPractical issues of reverse time migration: true-amplitude gathers, noise removal and harmonic-source encoding
Submiion number: 3784 Practical iue of revere time migration: true-amlitude gather, noie removal and harmonic-ource encoding Yu Zhang, CGGVerita, Houton Jame Sun, CGGVerita, Singaore Summary We analyze
More informationSystems Analysis. Prof. Cesar de Prada ISA-UVA
Sytem Analyi Prof. Cear de Prada ISAUVA rada@autom.uva.e Aim Learn how to infer the dynamic behaviour of a cloed loo ytem from it model. Learn how to infer the change in the dynamic of a cloed loo ytem
More informationImproved Adaptive Time Delay Estimation Algorithm Based on Fourth-order Cumulants
Available online www.jocr.com Journal of hemical and Pharmaceutical Reearch, 016, 8(5):889-894 Reearch Article ISSN : 0975-784 ODEN(USA) : JPR5 Imroved Adative Time Delay Etimation Algorithm Baed on Fourth-order
More informationEstimating floor acceleration in nonlinear multi-story moment-resisting frames
Etimating floor acceleration in nonlinear multi-tory moment-reiting frame R. Karami Mohammadi Aitant Profeor, Civil Engineering Department, K.N.Tooi Univerity M. Mohammadi M.Sc. Student, Civil Engineering
More informationPerformance analysis of heat exchanger with different types of fins
1. www.ierjournal.org International Engineering Reearch Journal (IERJ) Special Iue 3 Page 3-370, 201, ISSN 2395-121 ISSN 2395-121 Performance analyi of heat exchanger with different type of fin #1 Mi.
More informationA Mathematical Model of Two Layered Pulsatile Blood Flow through Stenosed Arteries
A Mathematical Model of Two Layered Pulatile lood Flow through Stenoed Arterie S. U. Siddiqui, S.. Shah, Geeta Deartment of Mathematic, Harcourt utler Technological Intitute, Kanur-8, India Email: geeta5_hbti@rediffmail.com
More informationLecture 3. Dispersion and waves in cold plasma. Review and extension of the previous lecture. Basic ideas. Kramers-Kronig relations
Lecture 3 Dierion and wave in cold lama Review and extenion of the reviou lecture Baic idea At the reviou lecture, we dicued how to roerly earch for eigenmode (or quai-eigenmode) of a dierive medium. In
More informationDetermination of Flow Resistance Coefficients Due to Shrubs and Woody Vegetation
ERDC/CL CETN-VIII-3 December 000 Determination of Flow Reitance Coefficient Due to hrub and Woody Vegetation by Ronald R. Copeland PURPOE: The purpoe of thi Technical Note i to tranmit reult of an experimental
More informationPOWER SYSTEM SMALL SIGNAL STABILITY ANALYSIS BASED ON TEST SIGNAL
POWE YEM MALL INAL ABILIY ANALYI BAE ON E INAL Zheng Xu, Wei hao, Changchun Zhou Zheang Univerity, Hangzhou, 37 PChina Email: hvdc@ceezueducn Abtract - In thi paper, a method baed on ome tet ignal (et
More informationHeat Transfer Modeling using ANSYS FLUENT
Lecture 7 Heat raner in Porou Media 14.5 Releae Heat raner Modeling uing ANSYS FLUEN 2013 ANSYS, Inc. March 28, 2013 1 Releae 14.5 Agenda Introduction Porou Media Characterization he Rereentative Elementary
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 informationDESIGN AND ANALYSIS OF FLEXIBLE STRUCTURES WITH PARAMETRIC UNCERTAINTIES FOR ACTIVE VIBRATION CONTROL USING ANSYS
INTERNATIONAL JOURNAL OF R&D IN ENGINEERING, SCIENCE AND MANAGEMENT Vol.1, Iue I, AUG.14 ISSN 9-85X Reearch Paer DESIGN AND ANALYSIS OF FLEXIBLE STRUCTURES WITH PARAMETRIC UNCERTAINTIES FOR ACTIVE VIBRATION
More informationSimulation Study on the Shock Properties of the Double-Degree-of-Freedom Cushioning Packaging System
Proceeding of the 7th IAPRI World Conference on Packaging Simulation Study on the Shock Propertie of the Double-Degree-of-Freedom Cuhioning Packaging Sytem Xia Zhu, Qiaoqiao Yan, Xiaoling Yao, Junbin Chen,
More informationEfficiency Optimal of Inductive Power Transfer System Using the Genetic Algorithms Jikun Zhou *, Rong Zhang, Yi Zhang
International Conference on echanical Science and Engineering (ICSE5 Efficiency Otimal of Inductive Power Tranfer Sytem Uing the Genetic Algorithm Jikun Zhou *, ong Zhang, Yi Zhang Intitute of ytem engineering,
More informationAMS 212B Perturbation Methods Lecture 20 Part 1 Copyright by Hongyun Wang, UCSC. is the kinematic viscosity and ˆp = p ρ 0
Lecture Part 1 Copyright by Hongyun Wang, UCSC Prandtl boundary layer Navier-Stoke equation: Conervation of ma: ρ t + ( ρ u) = Balance of momentum: u ρ t + u = p+ µδ u + ( λ + µ ) u where µ i the firt
More informationMathematical and Intelligent Modeling of Electropneumatic Servo Actuator Systems
Autralian Journal of Baic and Alied Science, 3(4): 3663-3671, 2009 ISSN 1991-8178 Mathematical and Intelligent Modeling of Electroneumatic Servo Actuator Sytem Hazem I. Ali, Samul Bahari B Mohd Noor, S.M.
More informationOVERSHOOT FREE PI CONTROLLER TUNING BASED ON POLE ASSIGNMENT
OVERSHOO FREE PI CONROER UNING BASED ON POE ASSIGNMEN Nevra Bayhan * Mehmet uran Söylemez ** uğba Botan ** e-mail: nevra@itanbul.edu.tr e-mail: oylemez@el.itu.edu.tr e-mail: botan@itu.edu.tr * Itanbul
More informationChapter 7: 17, 20, 24, 25, 32, 35, 37, 40, 47, 66 and 79.
hapter 7: 17, 0,, 5,, 5, 7, 0, 7, 66 and 79. 77 A power tranitor mounted on the wall diipate 0.18 W. he urface temperature of the tranitor i to be determined. Aumption 1 Steady operating condition exit.
More informationTypes of Heat Transfer
Type of Heat Tranfer Dv Dt x = k dt dx v T S 2 * * ( v GrT * z = + z H vap lat uject in the coure conduction (Fourier Law forced convection (due to flow ource term free convection (fluid motion due to
More informationLiang Peng, Qiwei Yao Estimating conditional means with heavy tails
Liang Peng, Qiwei Yao Etimating conditional mean with heavy tail Article (Acceted verion) (Refereed) Original citation: Peng, Liang and Yao, Qiwei (217) Etimating conditional mean with heavy tail. Statitic
More informationA NEW YIELD CRITERION FOR ORTHOTROPIC SHEET METALS UNDER PLANE-STRESS CONDITIONS
In: Proc. of 7 th COLD METAL FORMING Conference ( Ed. D. Banaic) May -1 Cluj Naoca Romania ag. 17-4. (htt://www.utcluj.ro/conf/tr) A NEW IELD CRITERION FOR ORTHOTROPIC SHEET METALS UNDER PLANE-STRESS CONDITIONS
More informationA Numerical Model of an Electrostatic Precipitator
16 th Autralaian Fluid Mechanic Conference Crowne Plaza, Gold Coat, Autralia -7 December 7 A Numerical Model of an Electrotatic Preciitator Shah M E Haque 1*, M G Raul, M M K Khan, A V Deev 1, and N Subachandar
More informationDynamic Behavior of Local Solids Concentration in Fluidized Beds: Experimental Validation of an Eulerian-Eulerian Model
Dynamic Behavior of Local Solid Concentration in Fluidized Bed: Exerimental Validation of an Eulerian-Eulerian Model Clay R. Sutton and John C. Chen Deartment of Chemical Engineering Lehigh Univerity Bethlehem,
More informationTypes of Heat Transfer
ype of Heat ranfer * Dvz Dt x k d dx v S * * v Gr z HH vap lat uject in the coure conduction (Fourier Law) forced convection (due to flow) ource term free convection (fluid motion due to denity variation
More informationModelling of straitened sedimentation process in bidisperse suspension with inter-fractional coagulation
American Journal of Chemical Engineering 04; (): 4-0 Publihed online June 0 04 (htt://www.cienceublihinggrou.com/j/ajche) doi: 0.648/j.ajche.0400. Modelling of traitened edimentation roce in bidiere uenion
More informationINVESTIGATION OF THE TURBULENT MASS TRANSPORT DURING THE MIXING OF A STABLE STRATIFICATION WITH A FREE JET USING CFD-METHODS
INVESTIGATION OF THE TURBULENT MASS TRANSPORT DURING THE MIXING OF A STABLE STRATIFICATION WITH A FREE JET USING CFD-METHODS I1. Armin Zirkel, I2. Eckart Laurien Intitute of Nuclear Technology and Energy
More informationNONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor
NONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor T o T T o T F o, Q o F T m,q m T m T m T mo Aumption: 1. Homogeneou Sytem 2. Single Reaction 3. Steady State Two type of problem: 1. Given deired
More informationAnalysis the Transient Process of Wind Power Resources when there are Voltage Sags in Distribution Grid
Analyi the Tranient Proce of Wind Power Reource when there are Voltage Sag in Ditribution Grid Do Nhu Y 1,* 1 Hanoi Univerity of ining and Geology, Deartment of Electrification, Electromechanic Faculty,
More informationEffect of Directional Spreading and Spectral Bandwidth on the Nonlinearity of the Irregular Waves
Proceeding of the Eighth (1998 International Offhore and Polar Engineering Conference Montréal, Canada, May -9, 1998 Coyright 1998 by The International Society of Offhore and Polar Engineer ISBN 1-8853-3-
More informationRELIABILITY ANALYSIS OF A COMPLEX REPAIRABLE SYSTEM COMPOSED OF TWO 2-OUT-OF-3: G SUBSYSTEMS CONNECTED IN PARALLEL
Journal of Reliability and Statitical Studie; ISSN (Print: 97-8, (Online:9-5666 Vol. 7, Iue Secial (: 89- RELIILITY NLYSIS OF COMPLEX REPIRLE SYSTEM COMPOSE OF TWO -OUT-OF-: G SUSYSTEMS CONNECTE IN PRLLEL
More informationMidterm 3 Review Solutions by CC
Midterm Review Solution by CC Problem Set u (but do not evaluate) the iterated integral to rereent each of the following. (a) The volume of the olid encloed by the arabaloid z x + y and the lane z, x :
More informationBernoulli s equation may be developed as a special form of the momentum or energy equation.
BERNOULLI S EQUATION Bernoulli equation may be developed a a pecial form of the momentum or energy equation. Here, we will develop it a pecial cae of momentum equation. Conider a teady incompreible flow
More informationGeometric optimization of micro-thermoacoustic cooler for heat management in electronics
Geometric otimization of micro-thermoacoutic cooler for heat management in electronic K.artibu, B.Sun and M.A.E. Kaunda Deartment of Mechanical Engineering Cae Peninula Univerity of echnology Box 65 Cae
More informationLecture 6. Erbium-doped fiber amplifier (EDFA) Raman amplifiers Have replaced semiconductor optical amplifiers in the course
Lecture 6 wo tye of otical amlifier: Erbium-doed fiber amlifier (EDFA) Raman amlifier Have relaced emiconductor otical amlifier in the coure Fiber Otical Communication Lecture 6, Slide 1 Benefit and requirement
More informationHybrid Projective Dislocated Synchronization of Liu Chaotic System Based on Parameters Identification
www.ccenet.org/ma Modern Applied Science Vol. 6, No. ; February Hybrid Projective Dilocated Synchronization of Liu Chaotic Sytem Baed on Parameter Identification Yanfei Chen College of Science, Guilin
More informationNarasimha Marakala 1, Appu Kuttan K K 2 and Ravikiran Kadoli 2
IOSR Journal o Mechanical and Civil Engineering (IOSR-JMCE) ISSN: 78-1684, PP: 63-68 www.iorjournal.org Exerimental and Theoretical Invetigation o Combined Eect o Fluid and Thermal Induced Vibration on
More informationMassachusetts Institute of Technology Dynamics and Control II
I E Maachuett Intitute of Technology Department of Mechanical Engineering 2.004 Dynamic and Control II Laboratory Seion 5: Elimination of Steady-State Error Uing Integral Control Action 1 Laboratory Objective:
More informationTheoretical Research on the Calculation of Bending Moment at Arc Vault in Steel Corrugated Plate
Theoretical Reearch on the Calculation of Bending oment at Arc Vault in Steel Corrugated Plate Baijian Li, Liangheng Zhu, Xinha Fu, Xu Luo. School of Civil Engineering,Tranortation, South China Univerity
More informationLoad-deformation Analysis of a Pile in Expansive Soil upon Infiltration
Proceeding of the 2 nd World Congre on Civil, Structural, and Environmental Engineering (CSEE 17) Barcelona, Sain Aril 2 4, 2017 Paer No. ICGRE 157 ISSN: 2371-5294 DOI: 10.11159/icgre17.157 Load-deformation
More informationAdvanced Workshop on Anderson Localization, Nonlinearity and Turbulence: a Cross-Fertilization. 23 August - 3 September, 2010
16-7 dvanced Workho on nderon Localization, Nonlinearity and Turbulence: a Cro-Fertilization 3 ugut - 3 Setember, 010 Four-wave Mixing Induced Turbulent Sectral Broadening in CW Fiber Laer Dmitry CHURKIN
More informationINVESTIGATIONS OF HEAT TRANSFER AND PRESSURE LOSS IN AN ENGINE-SIMILAR TWO-PASS INTERNAL BLADE COOLING CONFIGURATION
INVESTIGATIONS OF HEAT TRANSFER AND PRESSURE LOSS IN AN ENGINE-SIMILAR TWO-PASS INTERNAL BLADE COOLING CONFIGURATION C. Waidmann* - R. Poer* - J. von Wolferdorf* M. Foi** - K. Semmler** * Intitut of Aeropace
More informationLecture #5: Introduction to Continuum Mechanics Three-dimensional Rate-independent Plasticity. by Dirk Mohr
Lecture #5: 5-0735: Dynamic behavior of material and tructure Introduction to Continuum Mechanic Three-dimenional Rate-indeendent Platicity by Dirk Mohr ETH Zurich, Deartment of Mechanical and Proce Engineering,
More information84 ZHANG Jing-Shang Vol. 39 of which would emit 5 He rather than 3 He. 5 He i untable and eparated into n + pontaneouly, which can alo be treated a if
Commun. Theor. Phy. (Beijing, China) 39 (003) pp. 83{88 c International Academic Publiher Vol. 39, No. 1, January 15, 003 Theoretical Analyi of Neutron Double-Dierential Cro Section of n+ 11 B at 14. MeV
More informationStability analysis of the ideal internal kink mode in a toroidally rotating tokamak plasma with ultra flat q profile
Stability analyi of the ideal internal kink mode in a toroidally rotating tokamak lama with ultra flat q rofile hriter Wahlberg To cite thi verion: hriter Wahlberg. Stability analyi of the ideal internal
More informationGEOMETRIC OPTIMISATION OF CONJUGATE COOLING CHANNELS WITH DIFFERENT CROSS-SECTIONAL SHAPES
GEOMETRIC OPTIMISATION OF CONJUGATE COOING CHANNES WITH DIFFERENT CROSS-SECTIONA SHAPES By Olabode Thoma OAKOYEJO Prof. T. Bello Ochende, Prof. J. P. Meyer Department of Mechanical and Aeronautical Engineering,
More informationFinite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization
Finite Element Analyi of a Fiber Bragg Grating Accelerometer for Performance Optimization N. Baumallick*, P. Biwa, K. Dagupta and S. Bandyopadhyay Fiber Optic Laboratory, Central Gla and Ceramic Reearch
More informationFuzzy Model of Human s Performance for Guarding a Territory in an Air Combat
Fuzzy Model of Human Performance for Guarding a Territory in an Air Combat ABSTRACT R. Ghaemi i *, S.K.Y. Nikraveh ii, M.B. Menhaj iii and S. Akbari iv Received 1 October 9; received in revied 5 May 1;
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 informationHybrid models for hardware-in-the-loop simulation of hydraulic systems Part 2: experiments
1 Hybrid model for hardware-in-the-loo imulation of hydraulic ytem Part 2: exeriment J A Ferreira1*, F Gome Almeida2, M R Quinta2 and J P Etima de Oliveira3 1Deartment of Mechanical Engineering, Univerity
More informationA Comparison of Correlations for Heat Transfer from Inclined Pipes
A Comparion of Correlation for Heat Tranfer from Inclined Pipe Krihperad Manohar Department of Mechanical and Manufacturing Engineering The Univerity of the Wet Indie St. Augutine, Trinidad and Tobago
More informationRecent progress in fire-structure analysis
EJSE Special Iue: Selected Key Note paper from MDCMS 1 1t International Conference on Modern Deign, Contruction and Maintenance of Structure - Hanoi, Vietnam, December 2007 Recent progre in fire-tructure
More informationJ.P. Holman: 3.09) T sur := Use table 3-1 to determine the shape factor for this problem. 4π r S := T sphere := 30K r 1. S = m k := 1.
.P. Holman:.09) T ur : 0 Ue table - to determine the hape factor for thi problem. D :.m r : 0.5m π r S : T phere : 0 r D S 7.0 m :.7 m Ue eq. - to calculate the heat lo. q : S T phere T ur q 57.70 .P.
More informationMULTISCALE MODELING OF EQUAL CHANNEL ANGULAR EXTRUDED ALUMINIUM WITH STRAIN GRADIENT CRYSTAL PLASTICITY AND PHENOMENOLOGICAL MODELS
MULTISCALE MODELING OF EQUAL CHANNEL ANGULAR EXTRUDED ALUMINIUM WITH STRAIN GRADIENT CRYSTAL PLASTICITY AND PHENOMENOLOGICAL MODELS L. Duchêne, M.G.D. Geer, W.A.M. Brekelman, E. Chen, B. Verlinden and
More informationRupro, breach model used by Cemagref during Impact project
PAQUIER 1 Rupro, breach model ued by Cemagref during Impact project A PAQUIER Cemagref, France andre.paquier@cemagref.fr SUMMARY For embankment dam, piping and overtopping failure are the mot frequent
More informationECSE 4440 Control System Engineering. Project 1. Controller Design of a Second Order System TA
ECSE 4440 Control Sytem Enineerin Project 1 Controller Dein of a Secon Orer Sytem TA Content 1. Abtract. Introuction 3. Controller Dein for a Sinle Penulum 4. Concluion 1. Abtract The uroe of thi roject
More informationPolarization Invariants and Retrieval of Surface. Parameters Using Polarization Measurements in. Remote Sensing Applications
Thi i a rerint coy of an article ublihed in Alied Otic (Shetoaloff Yu. K. Polarization Invariant and Retrieval of Surface Parameter Uing Polarization Meaurement in Remote Sening Alication, Alied Otic,
More informationarxiv:hep-ph/ Nov 1995
DESY 95-6 ISSN 048-9833 he-h/95405 November 995 Incluive Dijet Production at HERA: Direct Photon Cro Section in Next-To-Leading Order QCD arxiv:he-h/95405 4 Nov 995 M. Klaen, G. Kramer II. Intitut für
More informationNONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH
International Journal of Electrical, Electronic and Data Communication, ISSN: 232-284 Volume-3, Iue-8, Aug.-25 NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH
More informationNumerical analysis of heating characteristics of a slab in a bench scale reheating furnace
International Journal of Heat and Ma Tranfer 5 (27) 219 223 Technical Note Numerical analyi of heating characteritic of a lab in a bench cale reheating furnace Sang Heon Han a, *, Seung Wook Baek a, Sang
More information1. Basic introduction to electromagnetic field. wave properties and particulate properties.
Lecture Baic Radiometric Quantitie. The Beer-Bouguer-Lambert law. Concept of extinction cattering plu aborption and emiion. Schwarzchild equation. Objective:. Baic introduction to electromagnetic field:
More informationLatest CMS results on low x physics and di raction
Latet CMS reult on low x hyic and di raction Benoit Roland (DESY) On behalf of the CMS Collaboration eracale Workho 04-3 December 04 DESY, Hamburg Benoit Roland (DESY) Latet CMS reult low x and di raction
More informationGain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays
Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,
More informationDEVELOPMENT OF A STRUCTURED THERMOCLINE THERMAL ENERGY STORAGE SYSTEM
DEVELOPMENT OF A STRUCTURED THERMOCLINE THERMAL ENERGY STORAGE SYSTEM Brad M. Brown Matt N. Straer R. Paneer Selvam Univerity of Arkana Department of Civil Engineering 4190 Bell Engineering Center Fayetteville,
More informationReliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay
International Journal of Applied Science and Engineering 3., 4: 449-47 Reliability Analyi of Embedded Sytem with Different Mode of Failure Emphaizing Reboot Delay Deepak Kumar* and S. B. Singh Department
More informationCHAPTER 3 LITERATURE REVIEW ON LIQUEFACTION ANALYSIS OF GROUND REINFORCEMENT SYSTEM
CHAPTER 3 LITERATURE REVIEW ON LIQUEFACTION ANALYSIS OF GROUND REINFORCEMENT SYSTEM 3.1 The Simplified Procedure for Liquefaction Evaluation The Simplified Procedure wa firt propoed by Seed and Idri (1971).
More informationLiquid cooling
SKiiPPACK no. 3 4 [ 1- exp (-t/ τ )] + [( P + P )/P ] R [ 1- exp (-t/ τ )] Z tha tot3 = R ν ν tot1 tot tot3 thaa-3 aa 3 ν= 1 3.3.6. Liquid cooling The following table contain the characteritic R ν and
More information