PPT-CALIFES for impedance measurements

LR Carver W Farabolini B Salvant Acknowledgements F Caspers R Corsini G D Michele A Grudiev A Latina T Lefevre E Metral H . Electrical impedance extends the concept of resistance to AC circuits describing not only the relative amplitudes of the voltage and current but also the r elative phases When the circuit is driven with direct current DC there is no distinction be 63mm VM with unshielded Bellows. Tuesday 6/11 2012. O.Berrig. & B. Salvant . 1. CST model of the VM module (diameter = 63 mm). 2. 63 mm. CST model of the RF fingers. 3. The natural state of the RF fingers. Matching (1). Maximum Power Transfer. Choose an RL in order to maximize power delivered to RL.. Power Delivered to the Load. Numerical Example. V. TH. =1 V. R. TH. =50 . Ω. Conclusion!. Maximum power is delivered to the load resistor when . Elliot . Mylott. . (. emylott@pdx.edu). Sabrina Hoffman. Ralf . Widenhorn. . (ralfw@pdx.edu). Physics Department. Portland State University, Portland, OR. European Journal of Clinical Nutrition 63, 619-626 (May 2009). Y-Chamber for . SPS Crab . cavity. By Phoevos Kardasopoulos. Thanks to Benoit Salvant. ,. Pei Zhang, Fred Galleazzi, Roberto Torres-Sanchez and Alick MacPherson . Impedance Meeting. Date: 14/04/14 . Karl Bane. SLAC National Accelerator Laboratory. 27 October 2016. LER 2016. Synchrotron SOLEIL, France. In low emittance rings, in colliders, in . linac. -based X-ray free electron lasers (FELs), the impedance/wakes of the vacuum chamber objects can lead to performance degradation. They can cause . Preliminary analysis. . . C. . Zannini, E. . Metral, G. Rumolo, B. . Salvant . Model studied. LHC design as it is built and installed. weld. In this step we are only interested to understand the effect of the weld .. Split Core Ferrites for . Low-Frequency Applications. Rachael Parker. Vice President of Fair-Rite Products Corp.. This presentation is brought to you by:. Rachael Parker. Vice President. Fair-Rite Products Corp.. Update. Fritz Caspers and Jose E. Varela. Outline. Introduction. The ‘Thomas Bohl’. Simulations. Measurements. Next . Steps. Conclusions. Introduction. We . continue to search for possible causes of the suspected 1.4GHz . Split Core Ferrites for . Low-Frequency Applications. Rachael Parker. Vice President of Fair-Rite Products Corp.. This presentation is brought to you by:. Rachael Parker. Vice President. Fair-Rite Products Corp.. W. Farabolini . on behalf of all the CALIFES beam users. 01/121/2015. CLIC Project Meeting #23. 1. Studies repartition with CALIFES and TBM. Test Beam Module : 21 days W. Farabolini. Wake Field Monitors : 48 days R. Lillestol et al.. ATB 10k 5k 1k 500 100 95 90 85 80 75 70 65 60 55 50 [Hz] Max. mech. excursion mm Impedance Resonance frequency fs 850 Hz Mechanical Q factor Qms Electrical Q factor Qes Total Q factor Qt aspects of fast-slow mode coupling instability. N.Biancacci. , . E.Métral. , . M.Migliorati. LER2020 – 27. th. October 2020. Outline. Introduction. Coasting beams fast and slow waves. Effect of driving impedance . Mario Beck - HSC section meeting - 2 October 2017. Thanks to: The . Impedance Working Group, Bruno Balhan, Mike Barnes, Giovanni . Rumolo. , . Carlo Zannini. Introduction I. Beam coupling impedance describes the interaction of the beam with its surrounding in frequency domain (wake in time domain).