Reducing Sound Intensity of an Aerodynamic Vehicle Ryan Gohlke – SHHS Alex Henry – WMHS Wouldn’t It be Great for a Car Gohlke-Henry 2 Background • Old Time vents (1950s) – Produced more drag = more $ – No vents on modern cars – Vortices shedding around window posts http://upload.wikimedia.org/wikipedia/commons/thumb/c/cd/1965_AMC_Ambassador_detail_ of_vent_window.jpg/330px-1965_AMC_Ambassador_detail_of_vent_window.jpg Gohlke-Henry 3 Applications • Automotive design • Engineering • Everyday drivers Gohlke-Henry 4 Purpose • To reduce sound intensity in a vehicle driving at high velocities while keeping drag force consistent Gohlke-Henry 5 Aerodynamics • Drag • Lift http://www.motiva.fi/myllarin_tuulivoima/windpower%20web/en/tour/wtrb/aeroforc.htm Gohlke-Henry 6 Open and Closed Pipe Resonance • Resonance • Speed of sound = 343 m/s ± depending on temperature http://hyperphysics.phy-astr.gsu.edu/hbase/waves/imgwav/ccyl.gif Gohlke-Henry 7 Node and Antinode • Standing wave • Node – resting point • Antinode – farthest displaced point http://www.antonine-education.co.uk/Image_library/Physics_2/Waves/Superposition/wav_26.gif Gohlke-Henry 8 Interference • Intersecting points create beats • Beats = thump Gohlke-Henry 9 Damping • Displace wave molecules to assure standing wave is harder to form http://www.splung.com/kinematics/images/damped_oscillations/damped_oscillations.gif Gohlke-Henry 10 Invention…Is Conceived! Gohlke-Henry 11 Invention is Officially Born Gohlke-Henry 12 Deresonator • Printed at different angles to destruct the formation of standing waves Gohlke-Henry 13 Hypothesis • If the deresonator is manufactured at 45°, then intensity will decrease and drag force will remain the same as if the windows were not open. Gohlke-Henry 14 PROCEDURES Gohlke-Henry 15 Sound Intensity Materials Air Supply Model SF-9216 Logger Pro Vernier Microphone Round Bottom Flask Gohlke-Henry 17 Procedure Gohlke-Henry 18 Take the Maximum! Gohlke-Henry 19 Data Sound Intensity 16 Trials No Angle 30º 45º 60º 17 1 3.563 2.807 2.890 2.761 18 2 3.596 2.795 2.787 2.783 19 3 3.618 2.846 2.799 2.756 20 4 3.606 2.797 2.800 2.767 21 5 3.581 2.803 2.779 2.767 22 6 3.586 2.821 2.865 2.762 23 7 3.505 2.785 2.787 2.757 8 3.535 2.818 2.792 2.744 24 gap between numbers 9 3.517 2.781Significant 2.840 2.753 25 10 3.586 2.812 2.829 2.734 26 11 3.607 2.845 2.785 2.767 27 12 3.642 2.817 2.812 2.769 28 13 3.547 2.785 2.843 2.744 29 14 3.534 2.793 2.818 2.752 30 15 3.557 2.804 2.807 2.745 Gohlke-Henry 3.573 2.852 2.841 2.773 3.597 2.834 2.863 2.773 3.558 2.804 2.831 2.738 3.580 2.821 2.840 2.762 3.540 2.840 2.846 2.773 3.543 2.831 2.811 2.757 3.597 2.812 2.830 2.746 3.583 2.837 2.835 2.762 3.617 2.780 2.857 2.742 3.614 2.810 2.846 2.766 3.579 2.803 2.820 2.752 3.579 2.797 2.804 2.743 3.549 2.802 2.807 2.759 3.590 2.801 2.809 2.781 3.623 2.818 2.843 2.756 20 Observations Observations Trial Sound Intensity Observations: Used duct tape to secure flask, will do so from now on De-resonator was not fully secured and fell into flask De-resonator was not fully secured and fell into flask De-resonator was not fully secured and fell into flask Gohlke-Henry No Angle: Trial 7 30°: Trial 15 30°: Trial 22 60°: Trial 3 21 Analysis • H0: µno angle = µ30° =µ45° =µ60° • Ha: Not all µno angle, µ30°, µ45°, µ60° are equal • Most assumptions are met for Sound Intensity – S.R.S., Distribution normal by C.L.T. – Deviation Rule of Thumb is not met Gohlke-Henry 22 Intensity Box Plots Sound Intensity (dB) Gohlke-Henry 23 Possible Overlap Sound Intensity (dB) Gohlke-Henry 24 Intensity Stats Sound Intensity (dB) x̄i Sxi ni No Angle 3.577 0.03315 30 30° 2.812 0.01986 30 45° 2.823 0.02719 30 60° 2.758 0.01257 30 Gohlke-Henry 25 ANOVA Test Results • Reject H0 • p-value of 0.0000 is less than the alpha level of 0.05 • Means are different and sound intensity has decreased • There is a 0% chance of getting results this extreme based on chance alone assuming H0is true • Standard deviation rule of thumb not met Gohlke-Henry 26 Overlap Results • • • • • H0: µ30° = µ45° Ha: µ30° ≠ µ45° Assumptions met Fail to reject H0 The two deresonators could produce a sound intensity at the same level • 5.39% chance of getting results this extreme based on chance alone assuming H0 is true Gohlke-Henry 27 Drag Force Materials Round Bottom Flask Light String Frictionless Pulley Vernier Dual Range Force Sensor Gohlke-Henry 29 Procedure Gohlke-Henry 30 Take the Mean! Gohlke-Henry 31 Data 14 15 30º 45º 60º 16 0.054 0.052 0.048 17 0.053 0.049 0.048 18 0.056 0.049 0.052 19 0.055 0.053 0.045 20 0.057 0.054 0.051 21 22 0.054 0.054 0.050 23 0.054 0.050 0.055 Insignificant gap between numbers 24 0.055 0.047 0.052 25 0.055 0.048 0.053 26 0.056 0.051 0.053 27 0.056 0.048 0.052 28 0.053 0.051 0.055 29 0.058 0.052 0.053 30 Drag Force (N) Trials No Angle 1 0.045 2 0.048 3 0.051 4 0.047 5 0.049 6 0.048 7 0.050 8 0.050 9 0.048 10 0.049 11 0.049 12 0.046 13 0.050 Gohlke-Henry 0.050 0.049 0.047 0.046 0.050 0.052 0.049 0.048 0.049 0.049 0.051 0.050 0.048 0.050 0.051 0.050 0.040 0.055 0.059 0.059 0.055 0.059 0.056 0.057 0.057 0.057 0.056 0.060 0.061 0.059 0.058 0.055 0.061 0.059 0.050 0.051 0.052 0.051 0.051 0.052 0.051 0.049 0.052 0.051 0.051 0.051 0.052 0.050 0.050 0.051 0.053 0.056 0.053 0.054 0.055 0.053 0.058 0.057 0.054 0.056 0.054 0.056 0.056 0.057 0.055 0.057 0.055 0.056 32 Observations Observations Trial Drag Force Observations: Force Sensor was moved during trial, experiment was reset LabQuest recorded inaccurate data, flask was repositioned LabQuest recorded inaccurate data, flask was repositioned LabQuest recorded inaccurate data, flask was repositioned Gohlke-Henry 45°: Trial 22 30°: Trial 9 No Angle: Trial 26 60°: Trial 17 33 Analysis • H0: µno angle = µ30° =µ45° =µ60° • Ha: Not all µno angle, µ30°, µ45°, µ60° are equal • Assumptions are met for drag force – S.R.S., Deviation Rule of Thumb, Distribution normal by C.L.T. Gohlke-Henry 34 Drag Force Box Plots Drag Force (N) Gohlke-Henry 35 Possible Overlap Drag Force (N) Gohlke-Henry 36 Drag Force Stats x̄i Sxi No Angle 0.049 0.00230 30 30° 0.057 0.00225 30 45° 0.051 0.00168 30 60° 0.054 0.00299 30 Drag Force (N) Gohlke-Henry ni 37 Drag Force Test Results • Reject H0 • p-value of 0.0000 is less than the alpha level of 0.05 • Means are different and drag force has varied in the positive direction • There is a 0% chance of getting results this extreme based on chance alone assuming H0 is true Gohlke-Henry 38 Overlap Results • • • • • H0: µ30° = µ60° Ha: µ30° ≠ µ60° Assumptions met Reject H0 The two deresonators cannot have the same drag force • 0.01% chance of getting results this extreme based on chance alone assuming H0 is true Gohlke-Henry 39 Conclusion • Sound Intensity • Drag Force – 60° followed by 30°, then 45° – 45° followed by 60°, then 30° Overall hypothesis was rejected 60° was deemed Gohlke-Henry 40 Force Diagram Lift Drag Gohlke-Henry 41 Further Research • Varying wind velocities and shape • Full-scale testing, apply fit deresonator to window of a car Gohlke-Henry 42 Acknowledgements • Chris Oesterling • Thomas J. Benson – Printed deresonators – Mentor Gohlke-Henry 43 Works Cited Aerodynamic Forces: Definitions of Lift and Drag. Digital image. n.p., n.d. Web. 03 Nov. 2014. <http://www.motiva.fi/myllarin_tuulivoima/windpower web/en/tour/wtrb/aeroforc.htm>. Aerodynamic Forces: Definitions of Lift and Drag." WindPower. Danish Wind Industry Association, 29 Sept. 2002. Web. 17 Sept. 2014. <http://www.motiva.fi/myllarin_tuulivoima/windpower%20web/en/tour/wtrb/aeroforc.htm >. Benson, Tom. "What Is Drag?" National Aeronautics and Space Administration.NASA. gov., 16 July 2014. Web. 17 Sept. 2014. <http://www.grc.nasa.gov/WWW/k-12/airplane/drag1.html>. Buscarello, Ralph T. "Mechanical Resonance - Detuning Resonant Part versus Reducing Vibration at the Source." Update International, 2013. Web. 22 Sept. 2014. <http://www.updateintl.com/VibrationBook2i.htm>. Closed-End Resonance. Digital image. Resonance. n.p., n.d. Web. 22 Sept. 2014. <http://www.physicsclassroom.com/Class/sound/u11l4b4.gif>. 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