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## Vibration of a cracked cantilever beam full reportPosted by: project report tiger Created at: Wednesday 17th of February 2010 07:16:54 AM Last Edited Or Replied at :Wednesday 17th of February 2010 07:16:54 AM | free vibration of cantilever beam ,
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C is in m/N.C0 is the value (1/k0) at the end of the cantilever beam when a/W=0. Thus the Compliance C is given by Or, with the moment of inertia, I=tW3/12 one gets The Compliance can be given in the non dimensional form as Where ÃƒÅ¸=L/W and for a beam without a crack And so, one has the ratio Compliance Ca in the presence of a crack to the Compliance C0 without crack as Taking the spring stiffness k of the cracked beam as the inverse of the Compliance, one gets and the ratio k (a)/k(0) as The relationship between the Compliance and the crack length and between the .................. [:=> Show Contents <=:] | |||

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I want to know how to make a complete analysis of a fiber reinforced composite leaf spring and a
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trical power. Based on Hamilton principle and the assumed mode method, the dyna..................[:=> Show Contents <=:] | |||

## Microcantilever based force tracking with application to high resolution imagingPosted by: seminarsense Created at: Tuesday 16th of November 2010 04:57:16 AM Last Edited Or Replied at :Tuesday 16th of November 2010 04:57:16 AM | microcantilever beams ,
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mployed using a NMC. Piezoresistive NMC is using in this experiment. Aim is to acquire the force trajectory at the NMC’s tip. Mathematical modeling and controller design. Mathematical modelingNanostage can be modelled as a mass spring damper system. Applications Measure forces at nanoscale. Predict the change of spring constant caused by surface stress. Measure DNA hybridization. Study of adsorption of lipoprotein,antigen-antibody binding. Advantages Sensing basedd on NMC is simple,inexpensive and accurate. Instead of bulky laser beam piezore.................. [:=> Show Contents <=:] | |||

## Cantilever Beam SensorsPosted by: rohith.nayanarkn Created at: Thursday 11th of November 2010 11:21:15 PM Last Edited Or Replied at :Thursday 11th of November 2010 11:21:15 PM | seminar topic on cantilever beam,
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## Vibration of a cracked cantilever beam full reportPosted by: project report tiger Created at: Wednesday 17th of February 2010 07:16:54 AM Last Edited Or Replied at :Wednesday 17th of February 2010 07:16:54 AM | free vibration of cantilever beam,
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tation become equal, the condition is called resonance. During resonance the amplitude of vibration
is very large. 3.1 TERMS USED a-crack length Mb- Bending moment A-(1-a/W) P-Force C-Compliance t- Thickness of beam E-Youngâ„¢s Modulus W- Width of beam G- Crack extension force Y- Deflection/amplitude I- Moment of inertia Y0- Static deflection without crack In- Integral Y0 (a)-Deflection /amplitude with crack k-Spring stiffness a-(A-3-A3) K-Stress intensity factor ÃƒÅ¸-L/W L- Length of the beam 0-Fundamental frequency M- Mass of the beam 0 (a) - Fundamental frequency with c.................. [:=> Show Contents <=:] | |||

## UNDAMPED FREE VIBRATIONPosted by: projectsofme Created at: Saturday 27th of November 2010 12:36:33 AM Last Edited Or Replied at :Saturday 27th of November 2010 12:36:33 AM | free undamped vibration pdf ,
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. Spring stiffness is defined as the force required to elongate or compress the spring by unit
length. The differential equation of the spring mass system is set up by considering all the forces and applying D’Alembert’s Principle Spring mass system represents several practical systems Examples: 1. Machine mounted on isolators 2. Mass m attached to the end of a cantilever beam K-Spring stiffness in N/m m-Mass in Kg m xInertia Force Kx = Spring Force, d = Static deflection of spring K d = Force due to static deflection mg = Gravitational pull m x + Kx + K d - mg = 0 m x + K.................. [:=> Show Contents <=:] |

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