An Introduction to BiophysicsJ. & A. Churchill, 1921 - 435 Seiten |
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Seite 14
... rays 470 μu , green 510 μμ , and orange 620 μμ . ( These are average figures , e.g. the various lengths classed under orange vary from 595 to 645 μμ [ μμ = 1 / 1,000,000 mm . ] . ) Beyond these visible rays exist both shorter ( ultra ...
... rays 470 μu , green 510 μμ , and orange 620 μμ . ( These are average figures , e.g. the various lengths classed under orange vary from 595 to 645 μμ [ μμ = 1 / 1,000,000 mm . ] . ) Beyond these visible rays exist both shorter ( ultra ...
Seite 15
... rays ( violet and a small amount of the ultra- violet rays ) . There is also a well - marked absorption band in the red portion of the spectrum between 665 and 685 μμ . The figure for the maximal energy of solar radiation is given by ...
... rays ( violet and a small amount of the ultra- violet rays ) . There is also a well - marked absorption band in the red portion of the spectrum between 665 and 685 μμ . The figure for the maximal energy of solar radiation is given by ...
Seite 20
... rays are converted into nitrites with an absorption of energy . One gram molecule of nitrite formed from nitrate transforms about 10,000 gram - calories of radiant energy into the potential state a strong endothermic reaction . This is ...
... rays are converted into nitrites with an absorption of energy . One gram molecule of nitrite formed from nitrate transforms about 10,000 gram - calories of radiant energy into the potential state a strong endothermic reaction . This is ...
Seite 70
... the atmosphere cause lateral diffusion of light of short wave - length giving a blue colour , while the red rays are transmitted direct , FARADAY - TYNDALL PHENOMENON 71 producing the gorgeous sunset colours 70 DISPERSE SYSTEMS.
... the atmosphere cause lateral diffusion of light of short wave - length giving a blue colour , while the red rays are transmitted direct , FARADAY - TYNDALL PHENOMENON 71 producing the gorgeous sunset colours 70 DISPERSE SYSTEMS.
Seite 74
... rays of light . ( Hatschek . ) objective is that diffracted from the particles present in and optically dif ferent from the fluid ( Fig . 7 ) . The apparent image bears no relation to the actual size of the particle , but depends on the ...
... rays of light . ( Hatschek . ) objective is that diffracted from the particles present in and optically dif ferent from the fluid ( Fig . 7 ) . The apparent image bears no relation to the actual size of the particle , but depends on the ...
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A. V. Hill absorbed absorption acid action adsorption alterations amount animal arterial basilar membrane blood body bone calcium capillary carbohydrate carbon cartilage cause cell cent changes Chap chemical chloride CO₂ collodion colloidal colour concentration constant contraction corpuscles crystalloids decrease dialysing diffusion dispersed dissociation effect efficiency elastic electrical electrolytes emulsion emulsoid endosmosis enzyme external fibres fluid force gland glass glucose gram growth haemoglobin heat hydrated hydrogen ion increase ionisation kidney lactic acid layer light liquid litre lungs maltose material mechanism membrane mercury metres minute molecules movement muscle muscular negative nerve nitrogen normal organism osmotic pressure oxygen particles pass permeability phase physical physiological plasma polarisation positive potassium potential energy produced protein rays reaction result salts secretion soap sodium sodium chloride solution stapes stimulation substance surface tension suspensoids TABLE temperature thermometer tissue tube velocity ventricle vibrations viscosity volume wall