Susanne
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doc#125 suspension were allowed to stand at room temperature for 1 hr. the tubes were then centrifuged
doc#125 in saline were allowed to stand at room temperature for 1 hr and then were centrifuged at 1000
doc#125 Blood samples were allowed to clot at room temperature for 3 hr, centrifuged and the serum was
doc#122 No detectable reaction was found at room temperature for reaction mixtures allowed to stand
doc#120 over the range of field <formul> gauss and temperature <formul> the asymmetry increases with increasing
doc#118 metal parts. It was calculated from the temperature gradient <formul> at <formul> inch as <formul>
doc#118 energy transfer depends on the current, the temperature in the arc column, the anode material,
doc#117 diagram, to be 0.85. The measured brightness temperature is a good approximation to the brightness
doc#126 nice, sunny day in March or April, when the temperature is close to 50° F and there is not too
doc#120 <formul> as a function of magnetic field and temperature is presented. <formul> is paramagnetic,
doc#117 the planet. The apparent black-body disk temperature is the temperature which must be assumed
doc#117 </p><p> The concept of apparent black-body temperature is used to describe the radiation received
doc#118 temperature of this region was approximated by the temperature measured halfways between the edge of the
doc#118 higher temperatures. </p><p> The upstream gas temperature measured with the thermocouple shown in
doc#120 temperature range of 77-294°K. For the low- temperature measurements the sample was cooled by a
doc#117 might be predicted on the basis of the known temperature of Mars. The low intensity of the radiation
doc#111 have ample light when the sun sets; the temperature of our homes is independent of the seasons
doc#118 voltage was measured. To measure the surface temperature of the anode plug, the surface was scanned
doc#118 sufficiently small compared with the surface temperature of the anode holder, to make the energy
doc#117 body temperature correspond to the physical temperature of the emitting material. </p><p> The radio