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700r4 fluid flow chart pdf

Algebra 2/Trigonometry - Regents Exams

The following procedures are to be followed for scoring student answer papers for the Regents Examination in Algebra 2/Trigonometry. More detailed information about scoring is provided in the publication Information Booklet for Scoring the Regents Examinations in Mathematics. Do not attempt to correct the student’s work by making insertions or changes of any kind. In scoring the open-ended questions, use check marks to indicate student errors. If the student’s responses for the multiple-choice questions are being hand scored prior to being scanned, the scorer must be careful not to make any stray marks on the answer sheet that might later interfere with the accuracy of the scanning. Unless otherwise specified, mathematically correct variations in the answers will be allowed. Units need not be given when the wording of the questions allows such omissions. Each student’s answer paper is to be scored by a minimum of three mathematics teachers. No one teacher is to score more than approximately one-third of the open-ended questions on a student’s paper. On the student’s separate answer sheet, for each question, record the number of credits earned and the teacher’s assigned rater/scorer letter. Schools are not permitted to rescore any of the open-ended questions on this exam after each question has been rated once, regardless of the final exam score. Schools are required to ensure that the raw scores have been added correctly and that the resulting scale score has been determined accurately. Raters should record the student’s scores for all questions and the total raw score on the student’s separate answer sheet. Then the student’s total raw score should be converted to a scale score by using the conversion chart that will be posted on the Department’s web site at: http://www.p12.nysed.gov/apda/ on Tuesday, June 19, 2012.

Algebra 2/Trigonometry Conversion Chart - Regents Exams

To determine the student’s final examination score, find the student’s total test raw score in the column labeled “Raw Score” and then locate the scale score that corresponds to that raw score. The scale score is the student’s final examination score. Enter this score in the space labeled “Scale Score” on the student’s answer sheet. Schools are not permitted to rescore any of the open-ended questions on this exam after each question has been rated once, regardless of the final exam score. Schools are required to ensure that the raw scores have been added correctly and that the resulting scale score has been determined accurately. Because scale scores corresponding to raw scores in the conversion chart change from one administration to another, it is crucial that for each administration the conversion chart provided for that administration be used to determine the student’s final score. The chart above is usable only for this administration of the Regents Examination in Algebra 2/Trigonometry. Algebra 2/Trigonometry Conversion Chart - June '13

TRANSMISSION REMOVAL & INSTALLATION - A/T ... - LIL EVO

AUTOMATIC FWD MODELS REMOVAL 1) Remove battery and battery tray. On 3000GT, remove undercover(s). On Eclipse turbo, drain and remove intercooler. On all models, remove air cleaner and case. Raise and support vehicle. Remove wheels. Disconnect control cables at transaxle. Drain transaxle fluid. 2) On Mirage 1.6L, disconnect tension rod. On all models, disconnect neutral safety switch connector, oil cooler hoses and electrical connectors from transaxle. Disconnect speedometer cable and throttle control cable (if equipped). Remove starter motor. 3) On Galant models with electronically controlled suspension, remove air compressor and bracket. Disconnect front height sensor rod at lower control arm. 4) On all models, remove upper transaxle-to-engine bolts. Remove engine undercover (if equipped). On all models, remove drive axle shafts. See FWD AXLE SHAFTS article in DRIVE AXLES. Separate lower control arms from struts for access to axle shafts (if necessary). 5) Remove front exhaust pipe (if necessary). On Eclipse 4WD, Galant 4WD and 3000GT, remove right member and gusset. On 4WD models, separate transfer assembly from transaxle. Reference mark transfer assembly-to-drive shaft and remove transfer assembly. 6) On all models, remove transmission inspection (dust) cover. Place index mark on torque converter and drive plate for reassembly reference. Remove torque converter-to-drive plate bolts. Push torque converter away from engine into transaxle. 7) Support transaxle with jack. Remove transaxle mounts bolts, mounting brackets and remaining transaxle-to-engine bolts. Slide transaxle assembly to right and lower to remove. CAUTION: Ensure torque converter is fully seated in transaxle before installation. Always install new snap rings on inner constant velocity joints.

Printable (PDF) version - Innovate Motorsports

www.tuneyourengine.com. 1994 - 1997 Mitsubishi 3000GT VR4 ECU Diagram. Connector A. Connector B Connector C. Connector D. Pin #. Name. Signal Type. Connector B Name Injector 1 Injector 3 Injector 5 Injector 2 Injector 4 Injector 6 Power Ground Air Intake Temperature Sensor O2 Sensor # 1 (Right Bank) O2 Sensor # 2 (Left Bank) Engine Coolant Temperature Sensor Throttle Position Sensor Atmospheric Pressure Sensor Vehicle Speed Sensor Volume Air Flow Sensor Power Ground Sensor Ground Connector C Connector D Signal Type Speed Speed Speed Speed Speed Speed Ground Analog Analog Analog Analog Analog Analog Speed Analog Ground GroundConnector B Name Injector 1 Injector 3 Injector 5 Injector 2 Injector 4 Injector 6 Power Ground Air Intake Temperature Sensor O2 Sensor # 1 (Right Bank) O2 Sensor # 2 (Left Bank) Engine Coolant Temperature Sensor Throttle Position Sensor Atmospheric Pressure Sensor Vehicle Speed Sensor Volume Air Flow Sensor Power Ground Sensor Ground Connector C Connector D Signal Type Speed Speed Speed Speed Speed Speed Ground Analog Analog Analog Analog Analog Analog Speed Analog Ground GroundConnector B Name Injector 1 Injector 3 Injector 5 Injector 2 Injector 4 Injector 6 Power Ground Air Intake Temperature Sensor O2 Sensor # 1 (Right Bank) O2 Sensor # 2 (Left Bank) Engine Coolant Temperature Sensor Throttle Position Sensor Atmospheric Pressure Sensor Vehicle Speed Sensor Volume Air Flow Sensor Power Ground Sensor Ground Connector C Connector D Signal Type Speed Speed Speed Speed Speed Speed Ground Analog Analog Analog Analog Analog Analog Speed Analog Ground Ground

Transflow S3™ Vacuum Phthalate-Free Flexible Tubing - Process ...

The only choice for phthalate-free f lexible tubing Dairy and Vacuum Applications Transflow S3™ Vacuum from Saint-Gobain Performance Plastics is now phthalate-free. Saint-Gobain is proud to be among the first companies to offer sustainable flexible tubing products. The bio-based Transflow S3™ line combines the high performance standards customers demand with an eco-friendly tubing design. Reduced Maintenance and Inspection Concerns Transflow S3™ Vacuum tubing is ideally suited for supply air transport. The smooth inner surface is less susceptible to particle entrapment, which can restrict air flow, while crystal clarity permits detection of equipment deficiencies such as backflow of milk into the air lines. Transflow S3™ Vacuum tubing is designed to work in tandem with Transflow S3™ M-34-R to provide a vacuum tube and easy fluid flow within the milking process. The Mark of Quality Every foot of Transflow S3™ Vacuum Tubing has been embedded with a trademark blue stripe within the tubing walls. The embedded blue stripe is your assurance of receiving genuine Transflow ® tubing, the world's finest raw milk tubing produced specifically for the dairy industry.

Fluid structure interaction in flexible vessels

The thesis is concerned with the study of fluid-structure interaction in flexible tubes both from the modelling as well as the experimental point of view. More specifically, it presents the first stage of development and testing of a novel unified solution method suitable for fluid-structure interaction problems. In the conventional approach for modelling such problems, the fluid and solid components are treated separately, information is exchanged at their interface and different solution algorithms are used for the two components. The equations for solids are solved for displacement and stress and, the ones for fluids are solved for velocity and pressure. The exchange of information between two solution methods that solve for different quantities is not a trivial task and has also known drawbacks such as high computational cost and potential numerical instabilities, especially for very flexible structures. In the new method presented in the thesis, a single set of equations is used to describe both fluid and solid, while the interface between them is contained within the solution domain itself. This is achieved by reformulating the solid equations to contain the same primitive variables used in fluids i.e. velocity and pressure. The PISO algorithm is used to handle the velocity-pressure coupling. The method proposed is fully tested for solids on a structural dynamic problem (beam bending) and the results compared successfully with the classical structural analysis. In order to quantify the dissipation characteristics of the numerical integration technique, a stability eigenvalue analysis of the proposed time marching and spatial discretisation scheme is performed in one dimension but the conclusions of this analysis were also in agreement with the results of the beam bending.

Analysis of Flow Fields in a Flexible Tube with Periodic Constriction

Numerical techniques based on pressure-velocity formulation have been adopted to solve approximately, the governing equations for viscous flows through a tube (simulating an artery) with a periodic constriction. The effect of the constriction as well as the rigid of the tube, on the flow characteristics, and its consequences for arterial disease is the focus of this investigation. The unsteady incompressible Navier-Stokes equations are solved by using the finite-difference technique in staggered grid distribution. The haemodynamic factors like wall shear stress, pressure and velocity are analyzed through their graphical representations. Maximum resistance is attained in case of rigid stenosed tube rather than the flexible one. The main result is to contribute that the recirculating region is larger in case of a rigid tube than that of flexible one. Key words: Periodic constriction, pressure-velocity approach, complaint wall, finite difference scheme MSC 2010 No.: 76D, 74S20 2045

Stability of fluid flow in a flexible tube to non-axisymmetric ...

Department of Chemical Engineering, Indian Institute of Science, Bangalore 560 012, India (Received 17 June 1998 and in revised form 25 October 1999) The stability of fluid flow in a flexible tube to non-axisymmetric perturbations is analysed in this paper. In the first part of the paper, the equivalents of classical theorems of hydrodynamic stability are derived for inviscid flow in a flexible tube subjected to arbitrary non-axisymmetric disturbances. Perturbations of the form vi = ˜i exp [ik(x − ct) + inθ] are imposed on a steady axisymmetric mean flow U(r) in v a flexible tube, and the stability of mean flow velocity profiles and bounds for the phase velocity of the unstable modes are determined for arbitrary values of azimuthal wavenumber n. Here r, θ and x are respectively the radial, azimuthal and axial coordinates, and k and c are the axial wavenumber and phase velocity of disturbances. The flexible wall is represented by a standard constitutive relation which contains inertial, elastic and dissipative terms. The general results indicate that the fluid flow in a flexible tube is stable in the inviscid limit if the quantity UdG/dr > 0, and could be unstable for UdG/dr < 0, where G ≡ rU /(n2 + k 2 r2 ). For the case of Hagen–Poiseuille flow, the general result implies that the flow is stable to axisymmetric disturbances (n = 0), but could be unstable to non-axisymmetric disturbances with any non-zero azimuthal wavenumber (n = 0). This is in marked contrast to plane parallel flows where two-dimensional disturbances are always more unstable than three-dimensional ones (Squire theorem).

Power Brake Booster, Replacing.wps - volvoXC.com

Power Brake Booster, Replacing Power Brake Booster, Replacing Preparation Disconnect the battery lead Removal Preparations for removing the power brake booster Switch off the ignition. Remove the cross member. (On 5 cylinder engines): Remove the screws and nuts from the engine mounting. Lift out the cross member. Remove the air cleaner (ACL) housing. Remove the plastic cap and the cable holder. Remove the integrated relay/fusebox. Preparations for removing the ABS unit Clean the brake pipes terminals at the master cylinder and ABS unit. Place paper under the master cylinder to avoid brake fluid spillage. Remove all the brake pipes from the master cylinder and the ABS unit. Plug the master cylinder socket for the brake pipes. Remove the ABS unit and bracket from the side member The unit is secured with three screws. NOTE: Store the ABS unit in such a way that no dirt can get into the pipe couplings. Preparations for removing the master cylinder NOTE: On cars with 6-cylinder engines: Disconnect the connectors from the master cylinder. Mark up a connector. Disconnect the connectors on the power brake booster. NOTE: If the car has hydraulic clutch: Block the hose to the clutch cylinder. Use hose pliers. Remove the master cylinder Avoid brake fluid spillage when removing. NOTE: Ensure that the gasket between the power brake booster and the master cylinder stays in place on the master cylinder. Remove the soundproofing panel and the power brake booster Transfer the components to the new power brake booster Transfer: ...

BRAKE BOOSTER
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BRAKE BOOSTER REMOVAL OF BRAKE BOOSTER 1. REMOVE MASTER CYLINDER (See page BR–10) 2. DISCONNECT VACUUM HOSE FROM BRAKE BOOSTER 3. REMOVE PEDAL RETURN SPRING 4. REMOVE CLIP AND CLEVIS PIN 5. REMOVE BRAKE BOOSTER, GASKET AND CLEVIS BR–17 BRAKE SYSTEM – Brake Booster INSTALLATION OF BRAKE BOOSTER (See page BR–16) 1. ADJUST LENGTH OF BOOSTER PUSH ROD (a) Install the gasket on the master cylinder. (b) Set the SST on the gasket, and lower the pin until its tip slightly touches the piston. SST 09737–00010 (c) Turn the SST upside down, and set it on the booster. SST 09737–00010 (d) Measure the clearance between the booster push rod and pin head (SST). Clearance: 0 mm (0 in.) (e) Adjust the booster push rod length until the push rod lightly touches the pin head. 2. INSTALL BRAKE BOOSTER, GASKET AND CLEVIS (a) Install the booster and gasket. (b) Install the clevis. (c) Install and torque the booster mounting nuts. Torque: 13 N–m (130 kgf–cm, 9 ft–lbf ) 3. CONNECT CLEVIS TO BRAKE PEDAL Insert the clevis pin into the clevis and brake pedal and install the clip to the clevis pin. 4. INSTALL PEDAL RETURN SPRING 5. INSTALL MASTER CYLINDER (See page BR–15) 6. CONNECT HOSE TO BRAKE BOOSTER 7. FILL BRAKE RESERVOIR WITH BRAKE FLUID AND BLEED BRAKE SYSTEM (See page BR–8) 8. CHECK FOR FLUID LEAKAGE 9. CHECK AND ADJUST BRAKE PEDAL (See page BR–6) 10. PERFORM OPERATIONAL CHECK (See page BR–7)

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