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Vibration of a cracked cantilever beam full report


Posted 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
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sity factor is given by

4. ANALYSIS OF VIBRATION OF THE BEAM
From figure .1 it can be seen that when the length of the crack increases, the force required to cause the same deflection is reduced. Thus the main consequence of this crack is to alter the stiffness of the beam leading to changes in fundamental frequency. In the absence of the crack the fundamental frequency of the cantilever beam is given by
0 = 2.04 (K/M) 1/2 (4.1)
The spring stiffness decreases with an increase in crack length Ëœaâ„¢. As a result of this, the fundamental frequency also decreases. Thus vibration..................[:=> Show Contents <=:]



ansys tutorial for leaf spring contact analisys


Posted by:
Created at: Saturday 27th of October 2012 01:18:06 PM
Last Edited Or Replied at :Saturday 27th of October 2012 01:18:06 PM
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I want to know how to make a complete analysis of a fiber reinforced composite leaf spring a..................[:=> Show Contents <=:]



vibration spectrum analysis book free download


Posted by:
Created at: Thursday 25th of October 2012 12:22:38 PM
Last Edited Or Replied at :Saturday 10th of November 2012 06:55:45 AM
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requesting vibra..................[:=> Show Contents <=:]



piezoelectric laminate transducer


Posted by: seminar addict
Created at: Thursday 02nd of February 2012 03:21:27 AM
Last Edited Or Replied at :Thursday 02nd of February 2012 03:21:27 AM
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ter is attached to a host structure rotating around a horizon axis, the alternation of the gravity component causes the beam to vibrate along its transverse direction. The vibration induces an alternating magnetic field applied on the transducer, which causes the ME transducer to generate electrical power. Based on Hamilton principle and the assumed mode method, the dynamic equation is derived to study the influences of the nonlinear dynamic behavior of the harvester on the energy harvesting. A prototype is fabricated and tested. The experimental results are in agreement with the analytical re..................[:=> Show Contents <=:]



Microcantilever based force tracking with application to high resolution imaging


Posted 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, microcantilever force resolution ,
real time implementation of robust nonlinear control frame work for piezoresistive NMC based force tracking.
Utilizing MRC PE controller could result in smoother control when compared to commercially avaliable PID controllers.
It significantly enhance the imaging resolution and manipulation accuracy.

References
“nanotechnology”. IEEE Transactions on nanotechnology Vol. 5, No 6, november 2006.
“Microassemblyexperiments under optical vision based control”.IEEE transaction of industrual electronics.Vol 52.No.4,Aug 2005
“Study of data retention of nanocrystal Flash memorie..................[:=> Show Contents <=:]



Cantilever Beam Sensors


Posted 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
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Vibration of a cracked cantilever beam full report


Posted 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
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e fixed end can be given in terms of the static deflection Y0 (a) as
(4.14)
The variation of the amplitude Y (a) with the exciting frequency /0is shown in figure 8 for a/W=0.4 and ß=8.
CRACK AT MID SPAN
With the crack at the mid span, the vibrations of the cantilever beam can be analysed as two spring mass system. With the force ËœF0 sin tâ„¢ , acting at the free end of the beam , the amplitudes ËœY1â„¢ and ËœY2â„¢at the mid span and at the free end, respectively can be written as
(4.15)
and
(4.16)
Where Yst= F0/k1.As a particular case with a/W=0.2, a..................[:=> Show Contents <=:]



UNDAMPED FREE VIBRATION


Posted 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
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own as undamped vibration. The first step in solving a vibration problem is setting up the differential equation of motion. The three approaches to setting up differential equation of motion are as follows
SETTING UP THE EQUATION OF MOTION
1.Use D’Alembert’s Principle

 Forces -m x = 0
 Torques - I q = 0
m = Mass x = Displacement
m x = Inertia Force, q = Angular Displacement
I = Mass Moment of Inertia,
I q = Inertia Torque

D’Alembert’s Principle states that the resultant of all forces acting on a body along with the inertia force is equal to zero. For a rotational syste..................[:=> Show Contents <=:]



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