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von Mises stress due to the Lorentz forces during 15-T operation.

A 15-T PULSED SOLENOID FOR A HIGH-POWER TARGET EXPERIMENT. H.G. Kirk, BNL, Upton, NY 11973, USA Efthymiopoulos, A. Fabich, F. Haug, H. Pereira, CERN, CH-1211 Gen é ve 23, Switzerland P. Titus, MIT/PSFC, Cambridge, MA 02139, USA

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von Mises stress due to the Lorentz forces during 15-T operation.

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  1. A 15-T PULSED SOLENOID FOR A HIGH-POWER TARGET EXPERIMENT • H.G. Kirk, BNL, Upton, NY 11973, USA • Efthymiopoulos, A. Fabich, F. Haug, H. Pereira, CERN, CH-1211 Genéve 23, Switzerland • P. Titus, MIT/PSFC, Cambridge, MA 02139, USA • K.T. McDonald, Princeton University, Princeton, NJ 08544, USA • J.R.J. Bennett, CCLRC, RAL, Chilton, OX11 0QX, UK The MERIT experiment, which ran at CERN in 2007, is a proof-of-principle test for a target system that converts a 4-MW proton beam into a high-intensity muon beam for either a neutrino factory complex or a muon collider. The target system is based on a free mercury jet that intercepts an intense proton beam inside a 15-T solenoid magnetic. Here, we describe the design and initial performance of the 15-T, liquid-nitrogen-precooled, copper solenoid magnet. Longitudinal cross section of the 15-T pulsed magnet, showing the 3 coil packages and cryostat Calculated behavior of the 15-T magnet during a pulse. The peak current is 7200 A at a peak voltage of 700 V. Approximately 30 MJ of energy is dissipated in the magnet, which raises its temperature from 80 to 120 K. Model of the cooldown by LN2 over 20 min of 40 K temperature rise of a 15-T magnet pulse. The inner coil, at completion of winding at Everson-Tesla, Allentown, PA. The nested set of 3 coil segments. The axial and circumferential grooves for LN2 flow are visible on the outer surface of the coil. The 15-T magnet in its cryostat, January 2006, at CVIP, Emmaus, PA. Axial stress during LN2 cooldown. von Mises stress due to the Lorentz forces during 15-T operation. Magnetic field and current traces during a 15-T pulse at MIT, March 2006.

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