STRESS is \({\sigma _c} = \frac{{Pd}}{{2t}}\;\) andLongitudinal stress will be half of the circumferential stress i.E. \({\sigma _l} = \frac{{Pd}}{{4t}}\).where P is the pressure, t is the thickness of cylinder, d is the diameter of the cylinderCalculation:Given:p = 20 MPa, t = 2.5 mm and d = 50 mm.Longitudinal stress\({\sigma _l} = \frac{{Pd}}{{4t}}\)\({\sigma _l} = \frac{{20\times 50}}{{4\times 2.5}} =100~MPa\)Hoop stress\({\sigma _h} = \frac{{Pd}}{{2t}} = {\sigma _1}\)Hoop strain\({\epsilon_h} = \frac{{Pd}}{{4tE}}\left( {2 - \MU } \right)\)Longitudinal stress\({\sigma _L} = \frac{{Pd}}{{4t}} = {\sigma _2} = \frac{{{\sigma _1}}}{2}\)Longitudinal strain\({\epsilon_L} = \frac{{Pd}}{{4tE}}\left( {1 - 2\mu } \right) = \frac{{{\sigma _2}}}{E}\left( {1 - 2\mu } \right)\)

"> STRESS is \({\sigma _c} = \frac{{Pd}}{{2t}}\;\) andLongitudinal stress will be half of the circumferential stress i.E. \({\sigma _l} = \frac{{Pd}}{{4t}}\).where P is the pressure, t is the thickness of cylinder, d is the diameter of the cylinderCalculation:Given:p = 20 MPa, t = 2.5 mm and d = 50 mm.Longitudinal stress\({\sigma _l} = \frac{{Pd}}{{4t}}\)\({\sigma _l} = \frac{{20\times 50}}{{4\times 2.5}} =100~MPa\)Hoop stress\({\sigma _h} = \frac{{Pd}}{{2t}} = {\sigma _1}\)Hoop strain\({\epsilon_h} = \frac{{Pd}}{{4tE}}\left( {2 - \MU } \right)\)Longitudinal stress\({\sigma _L} = \frac{{Pd}}{{4t}} = {\sigma _2} = \frac{{{\sigma _1}}}{2}\)Longitudinal strain\({\epsilon_L} = \frac{{Pd}}{{4tE}}\left( {1 - 2\mu } \right) = \frac{{{\sigma _2}}}{E}\left( {1 - 2\mu } \right)\)

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Oxygen gas at a pressure of 20 MPa is stored in a thin cylinder of thickness 2.5 mm and a mean diameter of 50 mm. The longitudinal stress in the cylinder is

Machine Design Cylinder Pressure Vessels in Machine Design 9 months ago

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Concept:By thin-walled cylinder, we mean that the thickness ‘t' is very much smaller than the radius Ri and we may quantify this by stating that the ratio t / Ri of the thickness of radius should be less than 0.1.In a thin shell circumferential STRESS is \({\sigma _c} = \frac{{Pd}}{{2t}}\;\) andLongitudinal stress will be half of the circumferential stress i.E. \({\sigma _l} = \frac{{Pd}}{{4t}}\).where P is the pressure, t is the thickness of cylinder, d is the diameter of the cylinderCalculation:Given:p = 20 MPa, t = 2.5 mm and d = 50 mm.Longitudinal stress\({\sigma _l} = \frac{{Pd}}{{4t}}\)\({\sigma _l} = \frac{{20\times 50}}{{4\times 2.5}} =100~MPa\)Hoop stress\({\sigma _h} = \frac{{Pd}}{{2t}} = {\sigma _1}\)Hoop strain\({\epsilon_h} = \frac{{Pd}}{{4tE}}\left( {2 - \MU } \right)\)Longitudinal stress\({\sigma _L} = \frac{{Pd}}{{4t}} = {\sigma _2} = \frac{{{\sigma _1}}}{2}\)Longitudinal strain\({\epsilon_L} = \frac{{Pd}}{{4tE}}\left( {1 - 2\mu } \right) = \frac{{{\sigma _2}}}{E}\left( {1 - 2\mu } \right)\)

Posted on 22 Nov 2024, this text provides information on Machine Design related to Cylinder Pressure Vessels in Machine Design. Please note that while accuracy is prioritized, the data presented might not be entirely correct or up-to-date. This information is offered for general knowledge and informational purposes only, and should not be considered as a substitute for professional advice.

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