An Introduction to BiophysicsJ. & A. Churchill, 1921 - 435 Seiten |
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Seite 3
... heat . Later , Joule demonstrated the equivalence of these two forms of energy . 427 kilogrammetres of work always pro- duce ( under standard conditions ) one Calorie of heat . Con- versely , heat may be transformed into mechanical ...
... heat . Later , Joule demonstrated the equivalence of these two forms of energy . 427 kilogrammetres of work always pro- duce ( under standard conditions ) one Calorie of heat . Con- versely , heat may be transformed into mechanical ...
Seite 4
... heat energy . E.g. Corollaries of the First Law . The following two deductions are of biological interest : 1. The total energy of a system in a given state is for the system DEGRADED ENERGY 5 in question a definite characteristic of ...
... heat energy . E.g. Corollaries of the First Law . The following two deductions are of biological interest : 1. The total energy of a system in a given state is for the system DEGRADED ENERGY 5 in question a definite characteristic of ...
Seite 5
... though the total cosmical energy may be constant its distribution and its state may alter . Some of the freed energy is always converted into heat , part of which is diffused among surrounding objects and is thus lost , as far as work is.
... though the total cosmical energy may be constant its distribution and its state may alter . Some of the freed energy is always converted into heat , part of which is diffused among surrounding objects and is thus lost , as far as work is.
Seite 7
... would be recovered on letting it fall to the ground ( taking into account the mechanical equivalent of the degraded heat ) . On the other hand , a weight resting on a ledge above the ground may perform work in falling if sufficient.
... would be recovered on letting it fall to the ground ( taking into account the mechanical equivalent of the degraded heat ) . On the other hand , a weight resting on a ledge above the ground may perform work in falling if sufficient.
Seite 8
... Heat ( Entropy ) Totally unavailable Free Energy Total Available Energy Total Unavailable Energy ( 3 ) Called " bound " energy by Helmholtz in 1882 . ( 3 + 4 ) Called " bound " energy by later workers . ( 4 ) Called " bound " energy by ...
... Heat ( Entropy ) Totally unavailable Free Energy Total Available Energy Total Unavailable Energy ( 3 ) Called " bound " energy by Helmholtz in 1882 . ( 3 + 4 ) Called " bound " energy by later workers . ( 4 ) Called " bound " energy by ...
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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 kinetic 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