821 resultados para Submerged biprocess


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As lipases e os biossurfactantes são compostos produzidos por microrganismos através de fermentações em estado sólido (FES) ou sumberso (FSm), os quais são aplicáveis nas indústrias alimentícia e farmacêutica, na bioenergia e na biorremediação, entre outras. O objetivo geral deste trabalho foi otimizar a produção de lipases através de fermentação em estado sólido e fermentação submersa. Os fungos foram selecionados quanto à habilidade de produção de lipases através de FES e FSm e aqueles que apresentaram as maiores atividades lipolíticas foram utilizados na seleção de variáveis significativas e na otimização da produção de lipases nos dois modos de cultivo. Foram empregadas técnicas seqüenciais de planejamento experimental, incluindo planejamentos fracionários, completos e a metodologia de superfície de resposta para a otimização da produção de lipases. As variáveis estudadas na FES foram o pH, o tipo de farelo como fonte de carbono, a fonte de nitrogênio, o indutor, a concentração da fonte de nitrogênio, a concentração do indutor e a cepa do fungo. Na FSm, além das variáveis estudadas na FES, estudaram-se as variáveis concentração inicial de inóculo e agitação. As enzimas produzidas foram caracterizadas quanto à temperatura e pH ótimos e quanto à estabilidade a temperatura e pH. Nas condições otimizadas de produção de lipases, foi avaliada a correlação entre a produção de lipases e bioemulsificantes. Inicialmente foram isolados 28 fungos. Os fungos Aspergillus O- 4 e Aspergillus E-6 foram selecionados como bons produtores de lipases no processo de fermentação em estado sólido e os fungos Penicillium E-3, Trichoderma E-19 e Aspergillus O-8 como bons produtores de lipases através da fermentação submersa. As condições otimizadas para a produção de lipases através de fermentação em estado sólido foram obtidas utilizando-se o fungo Aspergillus O-4, farelo de soja, 2% de nitrato de sódio, 2% de azeite de oliva e pHs inferiores a 5, obtendo-se atividades lipolíticas máximas de 57 U. As condições otimizadas para a produção de lipases na fermentação submersa foram obtidas utilizando-se o fungo Aspergillus O-8, farelo de trigo, 4,5% de extrato de levedura, 2% de óleo de soja e pH 7,15. A máxima atividade obtida durante a etapa de otimização foi 6 U. As lipases obtidas por FES apresentaram atividades máximas a 35ºC e pH 6,0, enquanto que as obtidas por FSm apresentaram ótimos a 37ºC e pH 7,2. A estabilidade térmica das lipases produzidas via FSm foi superior a das lipases obtidas via FES, com atividades residuais de 72% e 26,8% após 1h de exposição a 90ºC e 60ºC, respectivamente. As lipases obtidas via FES foram mais estáveis em pH´s alcalinos, com atividades residuais superiores a 60% após 24 h de exposição, enquanto as lipases produzidas via FSm foram mais estáveis em pH´s ácidos, com 80% de atividade residual na faixa de pH entre 3,5 e 6,5. Na fermentação submersa a correlação entre a produção de lipases e a atividade emulsificante óleo em água (O/A) e água em óleo (A/O) dos extratos foi 95,4% e 86,8%, respectivamente, obtendo-se atividades emulsificantes máximas O/A e A/O de 2,95 UE e 42,7 UE. Embora a maior produção de lipases tenha sido obtida na fermentação em estado sólido, não houve produção concomitante de biossurfactantes. Os extratos da fermentação submersa apresentaram redução da tensão superficial de 50 mN m -1 para 28 mN m -1 e atividade antimicrobiana frente ao microrganismo S. aureus ATCC 25923, com potenciais antimicrobianos de 36 a 43% nos três primeiros dias de fermentação. A fermentação submersa foi a técnica que apresentou os melhores resultados de otimização da produção de lipases, bem como de produção simultânea de biossurfactantes.

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The main focus of this paper is the motion planning problem for a deeply submerged rigid body. The equations of motion are formulated and presented by use of the framework of differential geometry and these equations incorporate external dissipative and restoring forces. We consider a kinematic reduction of the affine connection control system for the rigid body submerged in an ideal fluid, and present an extension of this reduction to the forced affine connection control system for the rigid body submerged in a viscous fluid. The motion planning strategy is based on kinematic motions; the integral curves of rank one kinematic reductions. This method is of particular interest to autonomous underwater vehicles which can not directly control all six degrees of freedom (such as torpedo shaped AUVs) or in case of actuator failure (i.e., under-actuated scenario). A practical example is included to illustrate our technique.

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This paper studies the practical but challenging problem of motion planning for a deeply submerged rigid body. Here, we formulate the dynamic equations of motion of a submerged rigid body under the architecture of differential geometric mechanics and include external dissipative and potential forces. The mechanical system is represented as a forced affine-connection control system on the configuration space SE(3). Solutions to the motion planning problem are computed by concatenating and reparameterizing the integral curves of decoupling vector fields. We provide an extension to this inverse kinematic method to compensate for external potential forces caused by buoyancy and gravity. We present a mission scenario and implement the theoretically computed control strategy onto a test-bed autonomous underwater vehicle. This scenario emphasizes the use of this motion planning technique in the under-actuated situation; the vehicle loses direct control on one or more degrees of freedom. We include experimental results to illustrate our technique and validate our method.

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In this paper we analyze the equations of motion of a submerged rigid body. Our motivation is based on recent developments done in trajectory design for this problem. Our goal is to relate some properties of singular extremals to the existence of decoupling vector fields. The ideas displayed in this paper can be viewed as a starting point to a geometric formulation of the trajectory design problem for mechanical systems with potential and external forces.

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The classical problem of surface water-wave scattering by two identical thin vertical barriers submerged in deep water and extending infinitely downwards from the same depth below the mean free surface, is reinvestigated here by an approach leading to the problem of solving a system of Abel integral equations. The reflection and transmission coefficients are obtained in terms of computable integrals. Known results for a single barrier are recovered as a limiting case as the separation distance between the two barriers tends to zero. The coefficients are depicted graphically in a number of figures which are identical with the corresponding figures given by Jarvis (J Inst Math Appl 7:207-215, 1971) who employed a completely different approach involving a Schwarz-Christoffel transformation of complex-variable theory to solve the problem.

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A formulation in terms of a Fredholm integral equation of the first kind is given for the axisymmetric problem of a disk oscillating harmonically in a viscous fluid whose surface is contaminated with a surfactant film. The equation of the first kind is converted to a pair of coupled integral equations of the second kind, which are solved numerically. The resistive torque on the disk is evaluated and surface velocity profiles are computed for varying values of the ratio of the coefficient of surface shear viscosity to the coefficient of viscosity of the substrate fluid, and the depth of the disk below the surface.

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A new microcycle microconidiating strain (mcm) ofNeurospora crassa was derived by successive backcrosses of a soil isolate to a laboratory wild-type strain. Surface grown cultures show normal wild-type vegetative morphology. However, under continuous agitation in liquid cultures at 22°C, macroconidial germlings bypass the usual mycelial phase and produce abundant numbers of uninucleate microconidia within 24 h. Temperature and culture media affect the production of microconidia.

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Wave propagation in fluid?filled/submerged tubes is of interest in large HVAC ducts, and also in understanding and interpreting the experimental results obtained from fluid?filled impedance tubes. Based on the closed form analytical solution of the coupled wave equations, an eigenequation, which is the determinant of an 8×8 matrix, is derived and solved to obtain the axial wave number of the lowest?order longitudinal modes for cylindrical ducts of various diameter and wall thickness. The dispersion behavior of the wave motion is analyzed. It is observed that the larger the diameter of the duct and/or the smaller its wall thickness, the more flexible the impedance tube leading to more coupling between the waves in the elastic media. Also, it is shown that the wave motion in water?filled ducts submerged in water exhibits anomalous dispersion behavior. The axial attenuation characteristics of plane waves along water?filled tubes submerged in water or air are also investigated. Finally, investigations on the sound intensity level difference characteristics of the wall of the air?filled tubes are reported.

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Scattering of water waves by a sphere in a two-layer fluid, where the upper layer has an ice-cover modelled as an elastic plate of very small thickness, while the lower one has a rigid horizontal bottom surface, is investigated within the framework of linearized water wave theory. The effects of surface tension at the surface of separation is neglected. There exist two modes of time-harmonic waves - the one with lower wave number propagating along the ice-cover and the one with higher wave number along the interface. Method of multipole expansions is used to find the particular solution for the problem of wave scattering by a submerged sphere placed in either of the layers. The exciting forces for vertical and horizontal directions are derived and plotted against different values of the wave number for different submersion depths of the sphere and flexural rigidity of the ice-cover. When the flexural rigidity and the density of the ice-cover are taken to be zero, the numerical results for the exciting forces for the problem with free surface are recovered as particular cases. (C) 2011 Elsevier Ltd. All rights reserved.

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This paper deals with the study of a submerged jet for the suction of unwanted fluid. This submerged jet is caused by the fluid coming out from a source. The presence of a sink in front of this source facilitates the suction of the fluid depending upon the source and sink flow rates, the axial and lateral separations of the source and sink, and the angle between the axes of the source and sink. The main purpose is the determination of the sink flow rate for 100% removal of the source fluid as a function of these parameters. The experiments have been carried using a source nozzle 6 mm in diameter and two sizes for the sink pipe diameter: 10 mm and 20 mm. The main diagnostics used are flow visualization using dye and particle image velocimetry (PIV). The dependence of the required suction flow rate to obtain 100% effectiveness on the suction tube diameter and angle is relatively weak compared to the lateral separation. DOI: 10.1115/1.4007266]

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In several chemical and space industries, small bubbles are desired for efficient interaction between the liquid and gas phases. In the present study, we show that non-uniform electric field with appropriate electrode configurations can reduce the volume of the bubbles forming at submerged needles by up to three orders of magnitude. We show that localized high electric stresses at the base of the bubbles result in slipping of the contact line on the inner surface of the needle and subsequent bubble formation occurs with contact line inside the needle. We also show that for bubble formation in the presence of highly non-uniform electric field, due to high detachment frequency, the bubbles go through multiple coalescences and thus increase the apparent volume of the detached bubbles. (C) 2013 AIP Publishing LLC.