Liquid Metal Loop and Heat Pipe Radiator for Space Reactor Power Systems Jean-Michel P. Tournier * and Mohamed S. El-Genk Institute for Space and Nuclear Power Studies, University of New Mexico, Albuquerque, New Mexico 87131 DOI: 10.2514/1.20031 This paper presents four radiator congurations that could be stowed in the launch bay of the DELTA-IV Heavy vehicle and have effective areas of 69.1 to 350 m 2 . The radiator for a space reactor power system with a lithium- cooled sectored compact reactor and thermoelectric converters has an effective area of 203 m 2 and lowest specic mass. The sectored compact reactor and thermoelectric converters system generates 114 kWe for 710 years. The radiator consists of six panels, each having a forward, xed segment and two rear, deployable segments, and rejects heat into space using rubidium heat pipes with carboncarbon armor and ns. The D-shaped heat pipes operate below 50% of the prevailing sonic or capillary limit. The radiator operates at a constant pressure drop of 12 kPa and inlet and exit temperatures of 780 and 755 K. Investigated are the effects on the radiators specic mass and lithium inventory of 1) tapering and changing width of coolant channels, 2) thermal-hydraulically coupling the panel segments in parallel, and 3) using perforated dividers between inlet- and exit-channels. The radiator with perforated dividers has a wet specic mass of 6:82 kg=m 2 , a liquid-lithium inventory of 179.3 liters, and a stowed height of 8 m. Nomenclature A = surface area, or ow cross section area, m 2 C p = coolant specic heat capacity, J=kg K D = equivalent diameter of ow channel, m D V = diameter of heat pipe vapor space, m d orif = circular orices diameter, m F = local radiation view factor f = Darcy friction coefcient, f a=Re b H = height, height of ow channel, m H V = height of D-shaped, heat pipe vapor space, m h fg = latent heat of vaporization, J=kg h fin = n average heat transfer coefcient, W=m 2 K h = dimensionless, n heat transfer coefcient K = dimensionless pressure loss coefcient k fin = n average thermal conductivity, W=m K L = length of radiator panel segment, m L cd = heat pipe condenser length, m L ev = heat pipe evaporator length, m L i = section length for computing P,m _ M i = crossow rate through orices, kg=s M L = gure-of-merit, W=m 2 _ m i = axial mass ow rate along channel, kg=s N = number of axial sections along radiator segment N 00 = orices number density, # per m 2 n HP = number of heat pipes in radiator segment Q = radiative heat rejection to space, W th R = radius, m Re = ow Reynolds number, Re L VD= T = temperature, K T fin = average carboncarbon n temperature, K T sink = space sink temperature, K V = average ow velocity, m=s W = width of coolant channel, m W fin = width of carboncarbon n, m = aspect ratio of D-shaped heat pipe, H V =D V = orices area ratio, A orif =HZ = thickness, m P = pressure drop, Pa T = coolant temperature drop through radiator, K Z = length of each axial section, Z L=N; m " = wick volume porosity, radiative emissivity " o = orices pressure loss correction factor fin = thermal efciency of carboncarbon n = liquid dynamic viscosity, kg=m s = density, kg=m 3 = StefanBoltzmann constant, 5:67 10 8 , W=m 2 K 4 L = liquid surface tension, N=m vis = coolant viscous dissipation, W Subscripts/Superscripts b = coolant bulk temperature base = base of carboncarbon n C = coolant exit-channel cd = heat pipe condenser dis = orices discharge ev = heat pipe evaporator ex = coolant at exit of radiator segment channel n = carboncarbon n gap = liquid-return annulus in heat pipe H = coolant inlet-channel HP = heat pipe in = coolant at inlet of radiator segment channel L = liquid phase of heat pipe working uid liner = metallic liner/wall of heat pipe, Ti orif = orices in divider wall rad = radiator panel turb = turbulent ow Received 12 September 2005; revision received 24 January 2006; accepted for publication 28 January 2006. Copyright © 2006 by Copyright 2006 by M. S. El-Genk. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Copies of this paper may be made for personal or internal use, on condition that the copier pay the $10.00 per-copy fee to the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923; include the code $10.00 in correspondence with the CCC. * Research Assistant Professor, Chemical and Nuclear Engineering Department, Institute for Space and Nuclear Power Studies. RegentsProfessor of Chemical and Nuclear Engineering and Director, Institute for Space and Nuclear Power Studies; (505) 277-5442; Fax: (505) 277-2814; mgenk@unm.edu. JOURNAL OF PROPULSION AND POWER Vol. 22, No. 5, SeptemberOctober 2006 1117