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Growth of capillaries in skeletal and cardiac muscle
O Hudlicka
Circ Res. 1982;50:451-461.
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Sodium, divalent cations, and guanine nucleotides regulate the affinity of the rat mesenteric artery angiotensin II receptor
GB Wright, RW Alexander, LS Ekstein, and MA Gimbrone, Jr
Circ Res. 1982;50:462-469.
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JA Bevan, GM Buga, VM Florence, A Gonsalves, and A Snowden
Circ Res. 1982;50:470-476.
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Interactions between intrarenal epinephrine receptors and the renal baroreceptor in the control of PRA in conscious dogs
ER Farhi, JR Cant, and AC Barger
Circ Res. 1982;50:477-485.
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A Kawasaki and P Needleman
Circ Res. 1982;50:486-490.
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Increased myothermal economy of isometric force generation in compensated cardiac hypertrophy induced by pulmonary artery constriction in the rabbit. A characterization of heat liberation in normal and hypertrophied right ventricular papillary muscles
NR Alpert and LA Mulieri
Circ Res. 1982;50:491-500.
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Influence of the pericardium on left ventricular end-diastolic pressure- segment relations during early and later stages of experimental chronic volume overload in dogs
MM LeWinter and R Pavelec
Circ Res. 1982;50:501-509.
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Responsiveness to cardiac sympathetic nerve stimulation during maximal coronary dilation produced by adenosine
UJ Johannsen, AL Mark, and ML Marcus
Circ Res. 1982;50:510-517.
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WT Clusin, MR Bristow, DS Baim, JS Schroeder, P Jaillon, P Brett, and DC Harrison
Circ Res. 1982;50:518-526.
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MJ Janse and FJ van Capelle
Circ Res. 1982;50:527-537.
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GJ van der Vusse, TH Roemen, FW Prinzen, WA Coumans, and RS Reneman
Circ Res. 1982;50:538-546.
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W Lewis, J Kleinerman, and S Puszkin
Circ Res. 1982;50:547-553.
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GB Guo, MD Thames, and FM Abboud
Circ Res. 1982;50:554-565.
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R Graham, C Skoog, L Oppenheimer, J Rabson, and HS Goldberg
Circ Res. 1982;50:566-572.
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KR Walley, M Grover, GL Raff, JW Benge, B Hannaford, and SA Glantz
Circ Res. 1982;50:573-589.
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Comments on "Wall shear stress distribution in a model canine artery during steady flow" which appeared in Circ Res 41: 391-399, 1977
AJ Schwartz
Circ Res. 1982;50:590.
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