Undergraduate Research (AE 4699) Final Report Wagner, Killian C 12-11-2015 Introduction: This semester was spent on the research, design, and development of sapphire windows which would be used to transmit infrared beams onto a high-temperature, high-pressure burner in order to perform spectroscopic analysis. The selection of the material for the lens of this material was sapphire due to its ability to transmit efficiently at the required wavelength and its resistance to stresses and scratches. A portion of this semester was spent determining how to thick the window is required to be in order to withstand the pressure that it will undergo during the course of experiments. This involved doing research to see what equations needed to be set-up and then implementing the parameters relevant to the experiment at hand. The current window that needed to be replaced had dimensions of the following: D = 3 inches = 7.62 cm And the objective was to develop a designed window configuration and determine the dimensions of the lens that would be associated with it as these had to be based on cost-effective. Following this, companies were contacted and quotes were requested for lenses within a dimension range as the window base would be developed to match the dimensions of whichever window lens was deemed most cost effective. Lastly, another portion of this semester was spent developing the model of the window and its frame in SolidWorks so that the drawings for each of the components with dimensions could be developed and sent to in-house manufacturing in order to reduce cost of development. Development of above Plot: D = Diameter of Window (measured) T = Required Thickness of Window to sustain max pressure To obtain this plot and solve for the required material thickness, we use the following equation for the maximum stress in a loaded uniform, circular plate: ππππ₯ = πΎπ· 2 π 4π 2 Where ππππ₯ = πΉπ ππ Sf: the safety factor of the window, a selected parameter Fa is the common apparent elastic limit for Al2O3 (sapphire) so that no permanent deformation results in the window. It is a material property πΉπ πΎπ· 2 π = ππ 4π 2 Rearranging to solve for thickness, T ππ πΎπ π = π·β 4πΉπ Sf: the safety factor for the window (selected value of 4 for many laboratory applications) K: a factor that depends on the support method for the window. In this case, it is unclamped so K=Ku=1.1125 Once these values are substituted into T expression: π π = 1.06066 π·β πΉπ Consulting a material properties table gives us Fa πΉπ = 276 πππ = 45000 ππ π ππππ₯ ππππ₯ = (1.06066)π·β 45000 Pmax = 25 atm = 367.3975 psi Current laboratory window has D = 3 in = 7.62 cm ππππ₯ = 0.7303 ππ This thickness represents the minimum required thickness of the window at this selected diameter to withstand the maximum pressure that will occur during the course of the experiment without any permanent deformation. For a sample MATLAB script to create the above plots, the code attached to end of the report. For the clamped case: The only variation compared to the unclamped case is that the value of K is now Kc, rather than Ku: πΎ = πΎπ = .75 The expression for the thickness, T, becomes: ππ πΎπ π π = π·β 4πΉπ and the value of Sf stays the same as previously π π = 0.866 π· β πΉπ And since we are still examining sapphire, Fa retains its value of 45,000 psi. The expression for Tmax that can be written is: ππππ₯,πππππππ = (0.866)π·β ππππ₯ 45000 Or as expressed in millimeters, the thickness vs. diameter plot becomes: A window of 25.0 mm diameter with a thickness of 2.3 mm would be put in the region above this curve meaning that the material properties of the window would be sufficient for the experiment at hand. The safety factor for a window of these dimensions could be calculated by rearranging the thickness formula as follows: ππ πΎπ π π = π·β 4πΉπ ππ = 4πΉπ π 2 πΎπ ππ· 2 When substituting the specific values in: ππ = 4(45000 ππ π)(2.3 ππ)2 (0.75)(367.40)(25 ππ)2 ππΉ = 5.5 This value was rounded down in order to generate a conservative estimate, but it is still well above the selected value of 4, which is a common value in laboratory experiments. SF: Safety Factor of the Window Selection of Material: The material that was selected as the lens for this window configuration was sapphire due to its ability to resist wear, withstand high pressures, and transmit a large range of light wavelengths. In the experiments to be performed, it was important that the material transmits at about 5 micrometers with a high efficiency and the ability of sapphire to perform to this standard is given in the following plot: An example of a graduate student performing a similar experiment and the means by which they selected their lens material is given in the following link: http://openscholarship.wustl.edu/cgi/viewcontent.cgi?article=1502&context=etd Purchase Options: Another portion of this semester was spent collecting data on the sapphire lens optics that are available on the market. This would allow us to size the metallic pieces and develop the SolidWorks representation of each of the pieces. This stage of the design process involved going online and collecting as much information for these lenses as possible from multiple companies. For each possible lens, the safety factor was calculated in order to determine whether the piece would meet lab safety requirements (in many cases it did not). Below is the majority of the collected data as it was inputted into an Excel spreadsheet: Purchase Options from Edmund Optics: Purchase Options from Esco Optics: Purchase Options from Newport: Complete data: In this table, the Design column represents whether the configuration is clamped or unclamped as this affects the safety factor calculation. Final Window Design: The window design is composed of two primary steel pieces and then the lens itself. The smaller piece is what attaches to the experiment set-up itself. It is anchored to the larger metal piece by screws which can be seen in the following image: The larger holes in the big metallic circular section are for bolts that will lock the configuration onto the burner set-up. The circular incisions in each of the metal frames is where an O-ring will be placed in order to ensure that there is no contact between the metal surfaces. There is also a small divot in each of metal pieces which is half the thickness of the lens (half of 3 mm) and this will ensure that the lens is locked into place once the bolts are in place. The location of the lens is off center so that it can capture the entire experimental area. Final Requested Sapphire Window Lens: Diameter: 1.5 inches Thickness: 0.11811 inches = 3 mm SF exceeds 4 experiment requirement Code:
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