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ME3221: Fundamentals of Design & Manufacturing
Lab: Fluctuating Stresses in a Bicycle Crankshaft
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Lab Problem & Content Describe stress state in bicycle crankshaft
Measure stresses – Electrical resistance strain gages Stress analysis - Mechanical analysis of system
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Sensing elements Load Cells - examples Hydraulic Capacitive
Piezoelectric
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Load Cells - examples Electrical resistance strain gages Most common, by far Sensitive to strain along gage longitudinal direction
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So, we’ve decided to measure bending stress and shear stress at an accessible location.
How to do this? Measurement concept – Use electrical resistance strain gages on crankshaft System Design - Specify number and orientation of gages
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Strain gages – “easy-to-use” – how do they work?
Measure strain, egage, then use, stress – strain relations esurface esurface = egage => DR a meander pattern foil resistor bonded to the test surface loading applied to test structure deforming structure deforms gage => resistance change measure DR calibration of gage to give strain in terms of resistance change gages designed to be sensitive only to axial strain
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Measure Strains Gage responds to strain
Lead tabs Gage Physical process in gage is DR due to e Advance alloy Calibrate gage: DR as function of e => Gage factor, Sg
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Measure Stresses – Surface of Part
Measure DR and calculate e (Valid for uniaxial tension only!) DR, and so e, more usefully measured as DV using a “bridge circuit”
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Gaging of Bicycle Crankshaft Strain gage rosettes
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The Instrumented Bicycle Crankshaft
Strain gage rosettes 90o apart
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Strain Gage Measurement – Bending stress
Gages are sensitive to strain along length of gage x y z F M about z M x y e Use Gage 2, which is aligned with the x-axis: x z
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Sir Charles Wheatstone
DR Measured DV Samuel Christie Sir Charles Wheatstone Vout Vin A D B C R2 R3 R1 R4 SG Rosette Gage 2 “Dummy gage” for temperature compensation (on “dummy” crank shaft taped to down tube) R3 & R4 are “bridge completion resistors” included on strain gage amp circuit board Note: DVout is amplified by a factor of ≈ 3500! (Any noise in the “slip ring” can cause jitters in your data.)
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How to measure txy? Wire in gages 1&3 as bridge resistances 1&2: 45○
Vout Vin A D B C R2 R3 R1 R4 SG Rosette Gage 3 Gage 1 Wire in gages 1&3 as bridge resistances 1&2: x y 45○ x’ y’ Bridge will measure a function of sx’ – sy’
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Now apply Mohr’s Circle:
2 sx txy sx’ sy’ q (90○– q) r sx txy y x x y’ txy’ sx’ sy’ x’ 45○ sx’ = sx /2 + r cos(90 ○– q) sy’ = sx /2 - r cos(90 ○– q) sx’ - sy’ = 2 r cos(90 ○– q)= 2 r sinq But sinq = txy / r So: sx’ - sy’ = 2txy (The 2X factor is included in the final V->s scale factor)
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Typical Results What to do with them? - In lab writeup
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