KGCOE MSD Technical Review Agenda Meeting Purpose: To review the detailed design proposal to ensure design adequacy. Materials to be Reviewed: Customer Specifications rev.5 Engineering Analysis rev.2 Risk Analysis rev.2 BOM and Budget rev.1 Meeting Date: February 13, 2009 Meeting Location: 09-4435 Meeting time: 10 a.m. - 12 a.m. Timeline: Meeting Timeline Start Time Topic of Review Required Attendees 10:00 Introductions, Review Agenda Day, Phillips, Wellin 10:02 Design Review 1 Action Items Day, Phillips, Wellin 10:03 System Design and BOM Day, Phillips, Wellin 10:15 Fluids Analysis – Electrical Simulation, Results Day, Phillips, Wellin 10:35 Blood Tank – Bubble Rise Time, Fluid Extraction Day, Phillips, Wellin 10:40 Water Bath – Heat Transfer Day, Phillips, Wellin 10:45 Tubing – Heat Transfer Day, Phillips, Wellin 10:50 Automated Resistance - Linear motor’s force approximation Day, Phillips, Wellin 11:00 Compliance Tank – Arterial Tank Dimensioning, Electrical Equivalent Model Day, Phillips, Wellin 11:15 Custom LVAD Connection Day, Phillips, Wellin 11:20 System Drain – Saline Flush Day, Phillips, Wellin 11:25 Pressure, Flow, and Temperature Sensors and DAQ Day, Phillips, Wellin 11:50 LabView Front Panel Concept Day, Phillips, Wellin 11:55 Wrap-up Day, Phillips, Wellin P09021 Hydraulic VAD Test Loop System Level Design Review Project # Project Name Project Track Project Family P09021 Hydraulic VAD Test Loop Assistive Devices and Bioengineering Artificial Organ Engineering Start Term Team Guide Project Sponsor Doc. Revision 2008-2 Dr. Day Dr. Day 3.0 Expected Project Benefits: Project Description Project Background: The left ventricle is responsible for pumping blood out to the body and for a person with heart disease might not be strong enough. A left ventricular assist device (LVAD) can be surgically implanted to give the heart the boost it needs. RIT is developing a magnetically levitated axial flow LVAD. Past senior design projects have worked on creating a durability tester for the LVAD, and a centering magnet device. Additionally two projects have focused on developing hemodynamic flow simulation systems. Problem Statement: The main goal of this project is to create and construct a flexible system that can be run and operated from a user interface on LabView and allow the creation of flow and pressure curves generated from LVAD devices. The system will be able to test LVAD device both with and without Pulsatile Ventricular Simulator (PVS) with fluids and blood. Objectives/Scope: 1. Collect and process data to generate pressure and flow curves for static system which is automatically adjusted. 3. Capable of extracting fluids while running in order to determine damage to blood caused by LVAD. 3. Collect and process data to generate pressure and flow curve for dynamic system which is a scaled model of the physiological circulatory system working with a PVS. Deliverables: Functional, partially biocompatible Left Ventricular Assist Device test loop. Pressure, Temperature, and Flow characteristic curves for static and dynamic systems. January 16, 2009 Aide in development of magnetically levitated axial flow LVAD by helping to characterize the amount of assistance which is generated, finding the optimal pressure assist, and determining pumps impact on blood. Reinforcing the bioengineering program at RIT. Core Team Members: Jonathan Klein – Project Manager Kyle Menges – Technical Lead Nguyen Dinh Vu – Technical Lead Christine Lowry – Design Engineer (ME) Chris Stein – Design Engineer (ME) Priyadarshini Narasimhan – EE Julie Coggshall – ISE Strategy & Approach Assumptions & Constraints: 1. 2. 3. 4. Understand the pressure, volume, flow rate, and temperature of the physiological circulatory system. Working with an existing steady state VAD closed loop, the team will be able to begin their analysis before designing a loop with the LV Simulator. Proposed Budget: $2,000 - $3,000 Minimize test loop volume and simplistic design due to blood expenses and risk of damage/ clotting. Issues & Risks: o o o Available Resources Functional Pulsatile Ventricular Simulator Blood Issues Certification Purchasing and storage Locations and use Project Understanding by team Bio compatibility Physiological Simulation Electrical Needs 2 P09021 Hydraulic VAD Test Loop System Level Design Review P09021: VAD Test Loop – Customer Needs Importance Need # Needs to (Scale: High, Medium, Low) 1 Able to incorporate LVAD R2 pump into Test Loop High 2 Able to run with and without Pulsatile Ventricular Simulator High 3 Simulate phyiological properties of the human body (i.e., temperature, resistance, compliance) High 4 Consist of Biocompatible components to minimize blood damage High 5 Closed loop system that cannot leak High 6 Generate Pressure and Flow curves at associated temperatures High 7 Operate using multiple fluids (water, water/glycerin mixture, blood) High 8 Extraction of fluid samples cannot interrupt test while running High 9 Within budget High 10 Safe for operators, observers and surrounding environment High 11 Correlate existing pump functionality test with collected data Medium 12 Easy to fill and drain fluids Medium 13 Volume cannot exceed that of blood bag Medium 14 Test device needs to be self contained and portable Medium 15 Easy to maintain and calibrate device Medium 16 Minimal comprehension of the system's functionality is needed to operate (friendly user interface, preferably LabVIEW) Medium January 16, 2009 3 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 4 P09021 Hydraulic VAD Test Loop KGCOE MSD System Level Design Review DR1 Action Items Meeting Purpose: To review the following material in order to gain input based off of attendees’ experience. Materials Reviewed: 26 Page packet included: 1 page summary, needs and specifications, Pugh charts, and sub-system descriptions. PowerPoint Visual Aide. Attendees: Julie Coggshall –IE, Priya- EE, Chris- ME, Kyle- ME, Nguyen- ME, Christine- ME, Jon- IE, Dr. Day- Customer and faculty guide, David Gomez and members of LVAD team- work for Dr. Day, Dr. Doolittle- Professor Head for the School of Life Sciences, Dr. Phillips- EE Professor, Prof. WellinME. Meeting Date: 16 Jan 09 Item # Description Responsible Comments Valve and non-valve connections Calculated bubble rise time A001 Create Quick Connect Design IE-Jon A002 Reservoir Calculations – Air Bubbles ME-Nguyen A003 Temperature Control – Heating Tank, find out what changes are in the human body with regards to temperature? ME-Chris Heating element, water bath A004 Should we use the flow sensors Dr. Day has? EE-Priya Yes EE-Priya Use Bleed port ME - Kyle Automate clamp A005 A006 Pressure Sensor Selection – are resolution, output format and frequency response appropriate? Will sensor trap blood? Select Resistance Generation Method – research automated clamp valve A007 Compliance Tank Analysis – Do we need two tanks? EE-Priya Do not need A008 Compliance Tanks – What are the clinical comparisons for the compliance values, what about different disease states. ME-Christine, Nguyen A009 Blood removal - Look into self healing membrane. ME - Chris Ideal value ~2 mL/mm Hg, range varies for different diseases Disposable syringe, extended connection January 16, 2009 5 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 6 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 7 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 8 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 9 P09021 Hydraulic VAD Test Loop System Level Design Review Electrical Equivalent Simulation Purpose: Analyze the effect of the venous compliance tank (is it really necessary?) Figure 1. – Complete system including both capacitors (compliance tanks) If a resistor represents the resistance in the system, pressure is represented by the voltage in a circuit and the current is the flow rate, a model using electric components can be used to represent the test loop. R1 , R2 , R3 and R4 are the resistors representing the resistance of tubing while R5 is the variable resistor used to vary the resistance in the system so as to achieve desired flow and pressure curves. The 2mF capacitor is the arterial compliance and since it has the units of ml/mmHg the capacitor is in micro farads to follow the units of compliance as opposed to l/mmHg in which case the capacitor value would be 2F. The 50mF capacitor also follows the units of the venous compliance which has the value of 50ml/mmHg. A square wave representing the LVAD and PVS, LVAD is indicated the 1V base voltage and the 100V is the PVS mimicing the left ventricle's pumping. The pulse width is 360ms as it because it best models the duration of a single heart beat and the period was set for 60 beats per minute. Calculation of the total resistance in Figure 1=> 1 1 Frequency of the circuit =T=1 The impedance of capacitor = 1 2𝜋𝑓𝐶 Therefore the total resistance of the above circuit=> 0.51Ω//50mF = 1 1 + 0.51 1 1 𝑗2𝜋50𝑒−3 = (0.4972 - j0.07966) Ω (0.4972 - j0.07966)Ω in series with 0.51Ω, 13 Ω, 0.51 Ω = 0.4972 - j0.07966 + 0.51+0.51+13 = (14.5173 – j0.07966) Ω January 16, 2009 10 P09021 Hydraulic VAD Test Loop (14.5173 – j0.07966) Ω // 2mF= System Level Design Review 1 1 + 0.51 = 1 1 𝑗2𝜋50𝑒−3 (14.5172 - j0.067101) Ω (14.5172-j0.067101) Ω in series with 0.51 Ω = 14.5172-j0.067101 + 0.51 = (15.0272 – j0.067101) Ω 100 (286.957m,96.610) 50 (49.351m,87.605) (286.957m,6.6473) (93.507m,3.0701) 0 (286.957m,3.4120) (9.0909m,9.853) (20.779m,320.801m) -50 0s 0.5s V(R1:2) -I(R2) 1.0s V(C1:1) 1.5s V(V1:+) Time Figure 2.: Figure shows the simulation of figure 1 Figure 3. – System without venous capacitor (compliance tank). The total resistance of Figure 3=> Total impedance in figure 1 – 0.51 Ω //50mF = (15.0272 – j0.06710) Ω - (0.4972 - j0.07966) Ω = (14.53 – j0.01256) Ω January 16, 2009 11 P09021 Hydraulic VAD Test Loop System Level Design Review 100 (256.522m,96.363) (49.351m,87.435) 50 (9.0909m,9.844) 0 (243.478m,7.1310) -50 0s 0.5s V(R1:2) -I(R2) 1.0s 1.5s V(V1:+) Time Figure 4.: Figure shows the simulation of figure 3 Voltage (pres s ure) at the arterial capacitor. (V) With venous capacitor Without venous capacitor Voltage (pres s ure ) at Current(flow the venous rate) in the capacitor (V) loop(A) Ris e time of the arterial capacitor (s ) Ris e time of the venous capacitor (s ) 96.61 3.41 6.64 0.0403 0.0727 96.36 0 7.13 0.0403 0.0000 Table 1: Results to the simulation of figure 1 and 3 showing the voltage at the nodes near each capacitor, the total current and rise times for both arterial and venous. Figure 1 was the schematic used to simulate the test loop with an arterial capacitor and venous capacitor while figure 3 was the schematic used to simulate the test loop without a venous tank. Figure 2 shows the results of the simulation of figure 1 and figure 4 shows the results of the simulation of figure 3. Table 1 shows the results of both simulations in a table form with the voltages at the nodes near the arterial and venous capacitance. It also shows the total current in the loop and also the rise time of both the arterial and venous capacitance. Besides this, the table compares the results obtained with and without the venous capacitor. It shows that by removing the venous capacitor, the voltage at the node near the arterial capacitor decreases slightly since the total current in the loop has increased. The rise time is going to be the same since the capacitor value is not changed. So since there is no drastic change in the voltage at the arterial tank, it will not be required to have the venous. To keep the current, or the rate of flow of the liquid, the variable resistor should be varied. January 16, 2009 12 P09021 Hydraulic VAD Test Loop System Level Design Review Fluids Analysis **Refer to Introduction to Fluid Mechanics by Fox et. Al for all equations, tables and figures referenced for the fluids analysis. Properties: 𝐵𝑙𝑜𝑜𝑑 𝑣𝑖𝑠𝑐𝑜𝑠𝑖𝑡𝑦 = 0.0027 𝑁𝑠⁄𝑚2 𝐵𝑙𝑜𝑜𝑑 𝑑𝑒𝑛𝑠𝑖𝑡𝑦 = 1060 𝑘𝑔⁄𝑚3 𝑅𝑒 = ( 𝜌𝑣̅ 𝐷 𝜇 𝑃1 𝑣̅1 2 𝑃2 𝑣̅2 2 + 𝛼1 + 𝑔𝑧1 ) − ( + 𝛼2 + 𝑔𝑧2 ) = ℎ𝑙𝑇 𝜌 2 𝜌 2 𝑒𝑞 8.29 Assumptions: The assumptions that were chosen for the fluids analysis include: Laminar Flow Incompressible Flow Steady State The fact that blood is a non-Newtonian fluid and that our calculated Reynolds number was 3,936 indicates that there will be some variability between theoretical calculations and the actual pressures and flow measured within the system. Introducing the PVS into the system creates a non-steady condition, and therefore we decided to analyze the system at the maximum desired flow rate for physiological simulation (6 Liters/minute). Under the assumed conditions, the PVS and LVAD both contribute a negative head loss to the system using eq. 8.29, and therefore will benefit the system in terms of pressure loss. Minor Losses: To find friction factor f a VBA code (written by Mr. John Wellin) was used. The code requires an input of the Reynolds number and roughness of the pipe/tubing to perform several iterations in order to determine the friction factor based on the Moody Diagram. January 16, 2009 13 P09021 Hydraulic VAD Test Loop System Level Design Review ℎ𝑙𝑚 𝐿 𝑣̅ 2 =𝑓 𝑒𝑞 8.34 𝐷 2 ℎ𝑙𝑚 = 𝐾 𝑣̅ 2 𝑒𝑞 8.40𝑎 2 For Bend in tube at bottom of loop Table 8.4 was used for 90o elbows (worse case) For all changes in diameter, including the LVAD Reducer, Fig. 8.14 was used to find the appropriate loss coefficients (Kc, Ke). For Quick Connects a loss coefficient of K=0 was used as provided in the data sheet from the manufacturer. The Blood loop and Glycerin water solution loop were analyzed for head losses due to the tubing, connections, tanks and other affects of the system. From our calculations both systems will be able to run and have enough pressure to complete the circuit even with the associated head losses. For the fluids analysis of the Glycerin loop steady state was assumed any variations from this assumption while using the PVS can be accounted for in testing. January 16, 2009 14 P09021 Hydraulic VAD Test Loop System Level Design Review Blood Loop January 16, 2009 15 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 16 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 17 P09021 Hydraulic VAD Test Loop System Level Design Review Physiological Loop January 16, 2009 18 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 19 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 20 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 21 P09021 Hydraulic VAD Test Loop System Level Design Review Bubble Rise Time Abstract: this is an analysis to figure out how much time needed for a bubble to reach the surface of liquid. It can be applied for dimensioning the blood tank. Scheme / given information: Fb 2R mg - blood viscosity µ=0.0027 at 100°F blood density ρblood=1060 kg/m3 air density ρair=1.177 kg/m3 at 100°F - bubble volume 𝑉𝑜𝑙 = 3 𝜋𝑅 3 - buoyancy force 𝐹𝑏 = 𝜌𝑏𝑙𝑜𝑜𝑑 𝑔𝑉𝑜𝑙 drag force 𝐹𝑑 = 6𝜋𝜇𝑏𝑙𝑜𝑜𝑑 𝑅𝑉 gravity force mg velocity of fluid inside the tubing Vfluid=0.79 m/s 4 Fd Assumption: bubbles is sphere-shape, temperature is constant at 100˚F, the bubble rises vertically. Analysis: 𝑚𝑎 = 𝐹𝑏 − 𝐹𝑑 − 𝑚𝑔 4 𝑑𝑉 4 4 ⇒ 𝜌𝑎𝑖𝑟 𝜋𝑅 3 = 𝜌𝑏𝑙𝑜𝑜𝑑 𝑔 𝜋𝑅 3 − 6𝜋𝜇𝑏𝑙𝑜𝑜𝑑 𝑅𝑉 − 𝜌𝑎𝑖𝑟 𝜋𝑅 3 g 3 𝑑𝑡 3 3 𝑑𝑉 𝜌𝑏𝑙𝑜𝑜𝑑 − 𝜌𝑎𝑖𝑟 9𝜇𝑏𝑙𝑜𝑜𝑑 ⇒ =𝑔 − 𝑉 𝑑𝑡 𝜌𝑎𝑖𝑟 2𝜌𝑎𝑖𝑟 𝑅 2 The bubble will reach its maximum velocity when the acceleration is zero: 2 𝜌𝑏𝑙𝑜𝑜𝑑 − 𝜌𝑎𝑖𝑟 𝑉𝑚𝑎𝑥 = 𝜋𝑔𝑅2 9 𝜋𝜇𝑏𝑙𝑜𝑜𝑑 We calculated for a bubble of 0.5mm in radius. All the bubble with smaller size will take more time to rise. After calculation in Maple, we found that the time and distance for that the bubble reach its maximum velocity are negligible. So we can assume that the velocity of the bubble is constant with the value V=Vmax=0.213m/s. As a result, the traveled distance is represented as below: January 16, 2009 22 P09021 Hydraulic VAD Test Loop System Level Design Review Figure 1. Distance traveled by the bubbled in function of time If we assume that the velocity of liquid inside the tank is two times less than the velocity in the tubing. So the time needed for a fluid element pass through the tank is: 𝑡= 𝐷𝑖𝑠𝑡𝑎𝑛𝑐𝑒 𝑖𝑛𝑝𝑢𝑡/𝑜𝑢𝑡𝑝𝑢𝑡 0.5 × 𝑉𝑓𝑙𝑢𝑖𝑑 With this time, the distance that a bubble raises is: 𝐻 = 𝑉𝑚𝑎𝑥 × 𝑡 = 𝑉𝑚𝑎𝑥 × 𝐷𝑖𝑠𝑡𝑎𝑛𝑐𝑒 0.5 × 𝑉𝑓𝑙𝑢𝑖𝑑 So, in the case of the blood tank, the distance between input and output is ID=4.75 in, so H=2.5 in. In the case of the arterial tank, the distance is IDxcos45o, so H=3.0 in. In the two cases, the bubble gets far enough. Maple code: > restart; > mju_blood:=0.0027: rho_blood:=1060: rho_air:=1.177: g:=9.81: > R:=0.5e-3: > eqn:=diff(V(t),t) = g*(rho_blood-rho_air)/rho_air (6*mju_blood)/(rho_air*(4/3*R^2))*V(t); eqn := d V ( t ) = 8825.024325 K 41291.41887 V ( t ) dt > V:=rhs(dsolve({eqn,V(0)=0},V(t))); January 16, 2009 23 P09021 Hydraulic VAD Test Loop System Level Design Review 45256535 45256535 0K V := K e 211750866 211750866 1 4129141887 t 100000 > V_max:=4/3*Pi*R^3*g*(rho_blood-rho_air)/(6*Pi*mju_blood*R); V_max := 0.2137253834 > t_max:=Re(solve(V=V_max,t)); t_max := 0.0005203217489 The distance made from 0 to t_max > int(V,t=0..t_max); 0 .0001060299410 The distance made from t_max > Distance:=int(V,t=0..t_max)+V_max*(t-t_max); Distance := K 0.0000051760243 C 0.2137253834 t > plot(Distance,t=t_max..1,x=0..0.25, labels=["time(s)", "distance(m)"]); If we change the size of the bubble, we obtain: - R=0.1mm January 16, 2009 24 P09021 Hydraulic VAD Test Loop - System Level Design Review R=1mm January 16, 2009 25 P09021 Hydraulic VAD Test Loop System Level Design Review Heat Transfer of Tanks Tank Dimensions: Ø = 4.875” x 5.5” Tw = 98oF = 310.15K Tw Tb = 70oF (room temperature) = 294.26K Tb Attempt w/ LCM (Lumped Capacitance Method) ∙ 𝑢𝑠𝑒 𝑖𝑓 𝐵𝑖 # 𝑖𝑠 < 0.1 𝐵𝑖 = ℎ𝐿𝑐 ⁄𝐾 𝐿𝑐 = 𝑉⁄𝐴 = 𝑟⁄2 = 2.4375⁄2 = 1.21875 𝐾302 𝑆𝑡𝑎𝑖𝑛𝑙𝑒𝑠𝑠 = 15.1 𝑤⁄𝑚𝑘 𝑡𝑎𝑏𝑙𝑒 𝐴. 1 𝑉𝑜𝑙𝑢𝑚𝑒 𝑏𝑙𝑜𝑜𝑑 = 1.9𝐿 = .0019𝑚3 ℎ= 𝜌𝑣𝐶𝑝 𝜏𝐴𝑠 𝑇∞ = 98.2℉ r2 r1 Ti 𝑇∞ Ti q” ln(𝑟2 ⁄𝑟1 ) 2𝜋𝐾𝑇 𝐿 1 2𝜋𝑟2 ℎ𝐿 𝐿 = 6.756" = .1714𝑚 𝐾𝑔𝑙𝑦𝑐𝑒𝑟𝑖𝑛 = .286 𝑊⁄𝑚𝐾 ℎ = .1714𝑚 = 6.75 𝑖𝑛 𝐾𝑠𝑡𝑎𝑖𝑛𝑙𝑒𝑠𝑠 = 15.1 𝑊⁄𝑚𝐾 𝑟1 = .062 𝑚 = 2.4375 𝑖𝑛 𝑟1 = .060 𝑚 = 2.375 𝑖𝑛 January 16, 2009 26 P09021 Hydraulic VAD Test Loop System Level Design Review 𝑅𝑇𝑜𝑡 = 𝑅𝑇𝑜𝑡 = ln(𝑟2 ⁄𝑟1 ) 1 + 2𝜋𝐾𝑇 𝐿 2𝜋𝑟2 ℎ𝐿 ln(. 062𝑚⁄. 060𝑚) 1 + 𝑊 𝑊 2𝜋(15.1 ⁄𝑚𝐾 )(.1714𝑚) 2𝜋(. 062𝑚)( ⁄𝑚𝐾 )(.1714𝑚) 𝑅𝑇𝑜𝑡 = .002 𝐾⁄𝑤 + 52.37 𝐾⁄𝑤 = 52.37 𝐾⁄𝑤 𝑅𝑇𝑜𝑡 = 52.37 𝐾⁄𝑤 𝑞= 𝑇∞ − 𝑇𝑖 310.05𝐾 − 294.26𝐾 = = .02 𝑤 𝑅𝑇𝑜𝑡 52.37 𝐾⁄𝑤 𝑤= 𝐵𝑖 = ℎ𝐿𝑐 ℎℎ2 𝑜 𝐿𝑐 ℎℎ2 𝑜 (𝑟⁄2) = = 𝑘 𝑘𝑏𝑙𝑜𝑜𝑑 𝑘𝑏𝑙𝑜𝑜𝑑 ℎ= ℎℎ2 𝑜 = 𝐽 𝑆 𝜌𝑣𝑐𝑝 𝜏𝐴𝑠 15.1 𝑊⁄𝑚𝐾 2𝜋𝐾𝑇 𝐿 𝐾𝑇 = = = 7427.6 𝑊⁄ 2 𝑚 𝐾 2𝜋𝑟2 𝐿 ln(𝑟2 ⁄𝑟1 ) 𝑟2 ln(𝑟2 ⁄𝑟1 ) . 062𝑚 (ln(. 062 )) . 060 𝐵𝑖 = 𝜉 = 2.3455 7427.6 𝑊⁄ 2 (3114𝑚⁄2) 𝑚 𝐾 = 42.16 15.1 𝑊⁄𝑚𝐾 𝐶1 = 1.5993 𝛼𝑠𝑡𝑎𝑖𝑛𝑙𝑒𝑠𝑠 = 3.91 × 10−6 𝑚2 ⁄𝑠 In order to find the approximate time for the blood in the tank to heat as well as the time it took for the water bath tank to heat to temperature the Lumped Capacitance method was used. We inputted these equations and values into excel and found that the time for the blood loop to heat would be less than 2 hours. These numbers indicate a show temperature rise that will be less likely to damage the blood. January 16, 2009 27 P09021 Hydraulic VAD Test Loop System Level Design Review Heat Loss in Tubes 𝑻∞= 𝟕𝟎℉ Ti=98oF Tm=? y x |<-------------------L=50in------------->| Blood Properties 70℉ @ µ = .00345 𝑁𝑠/𝑚2 98℉ @ µ = .0027 𝑁𝑠/𝑚2 𝛲 = 1060 𝑘𝑔/𝑚3 𝑣̅ = .789 𝑚⁄𝑠 𝐷 = .5𝑖𝑛 = 1.27 × 10−2 𝑚 𝐴𝑐𝑟𝑜𝑠𝑠 = 1.267 × 10−4 𝑚2 𝐶𝑝 𝑔𝑙𝑦𝑐𝑒𝑟𝑖𝑛 = 2.49 × 103 𝐽⁄𝑘𝑔𝐾 310𝐾 @ 𝐾𝑔𝑙𝑦𝑐𝑒𝑟𝑖𝑛 = 286 × 10−2 𝑊 ⁄𝑚𝐾 𝑁𝑢𝐷 = 0.027𝑅𝑒𝑑 4⁄5 𝑃𝑟 1⁄3 (𝜇⁄𝜇𝑠 )0.14 Equations 𝑅𝑒𝑑 = 𝑒𝑣̅ 𝐷⁄𝜇 ℎ = 𝑁𝑈𝐷 𝐾 ⁄𝐷 𝑑𝑇𝑚 𝑑𝑥 = 𝑃 ℎ(𝑇𝑠 𝑚̇𝐶𝑝 − 𝑇𝑚 ) Pg. 498 equation 8.37 Properties and Equation from Fundamentals of Heat and Mass Transfer 6th editions Solution 𝑑𝑇𝑚 𝑃ℎ 𝑃ℎ = 𝑇𝑠 − 𝑇 𝑑𝑥 𝑚̇𝐶𝑝 𝑚̇𝐶𝑝 𝑚 January 16, 2009 28 P09021 Hydraulic VAD Test Loop System Level Design Review 𝑑𝑇𝑚 𝑃ℎ 𝑃ℎ + 𝑇𝑠 = 𝑇 𝑑𝑥 𝑚̇𝐶𝑝 𝑚̇𝐶𝑝 𝑚 𝐶= 𝑃ℎ 𝑚̇𝐶𝑝 Homogenous 𝑇𝑚 1 + Assume solution: 𝑃ℎ 𝑇 =0 𝑚̇𝐶𝑝 𝑚 𝑇𝑚 1 = 𝑟𝑒 𝑟𝑥 𝑇𝑚 = 𝑒 𝑟𝑥 𝑟+ 𝑃ℎ =0 𝑚̇𝐶𝑝 𝑟= −𝑃ℎ 𝑚̇𝐶𝑝 Particular Solution Assume Solution: 𝑇𝑚 = 𝐴𝑥 + 𝑏 , 𝑇𝑚 1 = 𝐴 𝐴+ 𝑃ℎ 𝑃ℎ 𝐴𝑥 + 𝑏 = 𝐶𝑇𝑠 𝑚̇𝐶𝑝 𝑚̇𝐶𝑝 𝑃ℎ 𝐴𝑥 = 0 → 𝐴 = 0 𝑚̇𝐶𝑝 𝑃ℎ 𝑏 = 𝐶𝑇𝑠 → 𝑏 = 𝑇𝑠 𝑚̇𝐶𝑝 𝑃ℎ Now: 𝑇𝑚 = 𝑒 ( ̇ )𝑥 𝑚𝐶𝑝 + 𝑇𝑠 These calculations required the solution of a first order ordinary differential equation. The solution to this ODE led us to a find the final temperature of the tubes after a certain distance. The solution to this final equation was graphed in excel. The data shows that there is less than 1 degree change in temperature over 50 in of tubing. From this calculation it is clear that the heating system that we have chosen will heat and maintain the blood at the appropriate temperature to model the human circulatory system. January 16, 2009 29 P09021 Hydraulic VAD Test Loop System Level Design Review Linear motor’s force approximation Abstract: this is an analysis to approximate the force needed by the linear motor. Scheme / given information: Fmotor Pfluid Constants: - Fluid maximum pressure: Pfluid=2 psi - Outer diameter of the tubing: OD=11/16 in - Width of clamp: W=1 in Assumption: The resistance of the tubing has been neglected Analysis: OD Fmotor When the tubing is totally clamped, the length of clamp area is: Circumference 𝜋𝑂𝐷 𝜋 11⁄16 𝐿= = = = 1.1 𝑖𝑛 2 2 2 So the force can be approximated as: 𝐹𝑚𝑜𝑡𝑜𝑟 = 𝑃𝑓𝑙𝑢𝑖𝑑 × 𝐿 × 𝑊 = 2𝑝𝑠𝑖 × 1.1𝑖𝑛 × 1𝑖𝑛 = 2.2 𝑝𝑜𝑢𝑛𝑑𝑠 So if we neglect the resistance of the tubing, the force needed is 2.2 pounds. January 16, 2009 30 P09021 Hydraulic VAD Test Loop System Level Design Review Arterial tank dimensioning Abstract: this is an analysis to dimension the arterial tank, and calculate its properties. Scheme / given information: Constants from the physiological mocking system: - Compliance Cv=2.2 mL/mmHg=1.65e-8 m3/Pa - Fluid pressure at the output (absolute) Pf=860 mmHg =1.147e5 Pa - Density of glycerin ρ=1060km/m3 ID Pair h Constants from material constraints: hf - Inner diameter of the tank ID=7.75 in=0.197 m - Height of the tank h=0.6 ft=0.183 m Other constant: gravity g=9.81 m/s2 Assumption: ideal gas, small change in fluid height Analysis: From the equation: 𝐶𝑣 = 𝑉𝑎𝑖𝑟 𝑉𝑡𝑎𝑛𝑘 − 𝐴𝑡𝑎𝑛𝑘 ℎ𝑓 = 𝑃𝑎𝑖𝑟 𝑃𝑓 − 𝜌𝑔ℎ𝑓 We come up to the expression: ℎ𝑓 = 𝐶𝑣 𝑃𝑓 − 𝐴𝑡𝑎𝑛𝑘 ℎ = 0.121𝑚 = 4.78 𝑖𝑛 𝐶𝑣 𝜌𝑔 − 𝐴𝑡𝑎𝑛𝑘 And: 𝑃𝑎𝑖𝑟 = 𝑉𝑎𝑖𝑟 = 1.13𝑒5 (𝑎𝑏𝑠𝑜𝑙𝑢𝑡𝑒) 𝐶𝑣 So we find that we need to fill in 4.78 inch-height liquid, and the pressure of the air in the tank must be 1.75psi to have a pressure of 100mmHg at the output of the tank. Reference: Yingjie Liu, Paul Allaire, Yi Wu, Houston Wood, Don Olsen. Construction of an artificial heart pump performance test system. Springer Science + Business Media. 11/30/2006 January 16, 2009 31 P09021 Hydraulic VAD Test Loop January 16, 2009 System Level Design Review 32 P09021 Hydraulic VAD Test Loop System Level Design Review Saline Flush In search for a solution to flush out LVAD test loop post- blood testing, Drugs.com (a Drug Information Online source) suggested the use of Sodium Chloride Irrigation, which is commonly used in Clinical Pharmacology. 0.9% Sodium Chloride Irrigation USP is used for a variety of clinical indications such as sterile irrigation of body cavities, tissues or wounds, indwelling urethral catheters, surgical drainage tubes, and for washing, rinsing or soaking surgical dressings, instruments and laboratory specimens. It also serves as a diluent or vehicle for drugs used for irrigation or other pharmaceutical preparations. 0.9% Sodium Chloride Irrigation USP provides an isotonic saline irrigation identical in composition with 0.9% Sodium Chloride Injection USP (normal saline).1 Many vendors of biocompatible tubing or valves, which we will likely purchase materials, such as Cole-Parmer.com, suggest sterilization by autoclave, radiation, or ethylene oxide. An autoclave is a pressurized machine that heats aqueous solutions above their boiling point at normal atmospheric pressure to make objects sterilized.2 Autoclaves can cost anywhere between $1,756 and $3,958, and are out of the price range of this project. 3 Radiation is also an option not suited for this project, and would divert too much focus away from the scope. Ethylene oxide is the organic compound with the formula C2H4O. This colorless flammable gas with a faintly sweet odor is the simplest epoxide, a three-member ring consisting of two carbons and one oxygen atom, and is also used for medical sterilization.4 This chemical is used in a chamber sterilization method, which a chamber is flooded with a mixture of ethylene oxide and other gases that are later aerated. Because of this, and the fact that it is toxic to inhale, we are choosing not to use ethylene oxide (nor radiation or autoclave) to sterilize the LVAD test loop, but rather normal saline. 1Drugs.com. Sodium Chloride Irrigation. http://www.drugs.com/pro/sodium-chlorideirrigation.html 2Wikipedia- Autoclave. http://en.wikipedia.org/wiki/Autoclave 3 MedSupplier.com. http://www.medsupplier.com/autoclaves-andsterilizers.aspx?gclid=CMiLl92otZgCFROgnAod4hT5bA 4 Wikipedia- Ethylene Oxide. http://en.wikipedia.org/wiki/Ethylene_oxide January 16, 2009 33 P09021 Hydraulic VAD Test Loop System Level Design Review Sensor and DAQ analysis This report looks at the resolution and sensitivity of the sensors and also the resolution of the DAQ. Besides is also looks at output voltage of then sensors so it is possible to compare DAQ and a sensor to figure out if they will be compatible with each other. Sensitivity = 50𝑚 5 = 10mV/psi If using accuracy of measurement for pressure is 0.1 in H20 Resolution = 10mV/psi × (0.1inches of water × 0.0361) psi = 36.1µV Pressure Sensor (Omega PX26-005DV ) Specs Model's specs Output format (@10V) 50mV Price $36.00 Sensitivity= 10 = 64 0.156V/liter Resolution= 0.156V/liter × 0.05liter =7.8mV Flow sensor (Transducer+board digiflow-ext1 ) Specs Model's specs Resolution 1ml/min Output format -5V to 5V Max measurement ±32 𝑙/𝑚𝑖𝑛 Frequency 15kHz to 18MHz (transmitter frequency) Price Don’t need to purchase January 16, 2009 34 P09021 Hydraulic VAD Test Loop System Level Design Review Thermocouple. (Omega - KMQSS-020G-12) Specs Model's specs Type Ungrounded Price $28.65 Resolution in volts = 𝑓𝑢𝑙𝑙 𝑠𝑐𝑎𝑙𝑒 𝑟𝑎𝑛𝑔𝑒 2𝑀 = 160𝑚 224 = 9.54nV/code Thermocouple DAQ (NI 9211A) Specs Model's specs Resolution 24bit Number input pins 4 Voltage range -80mV to 80mV Sampling rate 15 S/s (samples per secs) Price $521 January 16, 2009 35 P09021 Hydraulic VAD Test Loop System Level Design Review Resolution in volts = 5−(−5) 10 =222 2𝑀 Resolution in volts = 62𝑚−(−62𝑚) 124𝑚 = 222 2𝑀 = 2.384µV/code = .2956nV/code DAQ (OMB-DAQ-54) Specs Model's specs Resolution 22 bits Number input pins 10 single ended Voltage range 31mV to 20V Sampling rate 80 S/sec Price $649 Looking at the results for what was obtained from the calculations to figure out the sensitivity of the sensor and resolution of both the DAQ and sensor, it was found that if the PX2300 was purchased it can be coupled with the flow sensor and the USB 6009 DAQ. If instead the PX26 was purchased it is possible to couple it with the NI9211A DAQ and thermocouple. But if the OMB-DAQ-54 was bought it is possible to incorporate all the sensors including the flow sensor as it has a total of 10 single ended analog inputs. Since the NI9211 has the a range of ±80𝑚𝑉 along with the thermocouple, this makes it possible to use the PX26 pressure sensor, besides this it has a resolution of about 10nV/bit showing that it will be able to resolve the minute fluctuation of the sensors. The sensor is shown to output 10mV per psi of change. Assuming that required accuracy of the pressure reading is 0.1inches of water, it was found that the resolution of the sensor to be 36.1µV, meaning that the when the sensor detects 36.1µV then it indicates a change in pressure. For the flow sensor, it has a sensitivity of about 0.156V/liter and a resolution of 7.8mV if it is assumed that the accuracy of the reading needs to be a 0.05 liter change. The output voltage range also corresponds of the OMB-DAQ-54 so they can be used together. January 16, 2009 36 P09021 Hydraulic VAD Test Loop System Level Design Review LabVIEW Front Panel Prototype Controls: Indicators: LVAD Speed (rpm) Desired Flow ( L/m) Desired Pressure Decrease (mm Hg) PVS Speed (rpm) PVS upper/ lower (bpm) Resistance Valve control (in) January 16, 2009 Real time/ Summary of pressure/ flow graphs PVS Change in Pressure and Flow with max/ min indicators Temperatures in tank and at LVAD Boolean Warning lights if temperature is out of range 2 Pressure Sensors 2 Flow Sensors 37