The Mathematical Principles of Natural Philosophy, Volumen1H.D. Symond, 1803 |
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Página xv
... quantities of matter in the bodies . This is collected from the equal acceleration of all bodies that fall from a state of reft by the force of their weights ; for the forces by which unequal bodies are equally accelerated must be ...
... quantities of matter in the bodies . This is collected from the equal acceleration of all bodies that fall from a state of reft by the force of their weights ; for the forces by which unequal bodies are equally accelerated must be ...
Página xvi
... quantity of matter in the body ; and therefore the force with which every body attracts the earth , or the abfolute force of the body , will be as the fame quantity of matter . . Therefore the attractive force of the entire bodies ...
... quantity of matter in the body ; and therefore the force with which every body attracts the earth , or the abfolute force of the body , will be as the fame quantity of matter . . Therefore the attractive force of the entire bodies ...
Página xvii
... quantity of that aberration , and find it perfectly infenfible . For the ratio of the lunar centripetal force itfelf , which muft be the moft irregular of them all , will be , indeed , a little greater than the duplicate , but will be ...
... quantity of that aberration , and find it perfectly infenfible . For the ratio of the lunar centripetal force itfelf , which muft be the moft irregular of them all , will be , indeed , a little greater than the duplicate , but will be ...
Página xxi
... quantity of matter ; as was fhewn above of the terreftrial par- ticles . At different diftances thefe forces will be alfo in the duplicate ratio of the distances reciprocally ; for it is mathe- " matically demonstrated that particles ...
... quantity of matter ; as was fhewn above of the terreftrial par- ticles . At different diftances thefe forces will be alfo in the duplicate ratio of the distances reciprocally ; for it is mathe- " matically demonstrated that particles ...
Página 1
... quantity of matter is the measure of the fame , arifing from its denfity and bulk conjunctly . THUS air of a double density , in a double space , is quadruple in quantity ; in a triple space , fextuple in quantity . The fame thing is to ...
... quantity of matter is the measure of the fame , arifing from its denfity and bulk conjunctly . THUS air of a double density , in a double space , is quadruple in quantity ; in a triple space , fextuple in quantity . The fame thing is to ...
Otras ediciones - Ver todas
Términos y frases comunes
ABFD abfolute accelerative alfo alſo angle VCP apfides apfis arifing attracting body axis becauſe bifected body revolving cafe caufes cauſe centre of force centre of gravity centripetal force circle common centre conic fection corpufcle curve line cycloid decreaſe defcend defcribe demonftrated diminiſhed diſtance drawn duplicate ratio ellipfis fame ratio fecond feveral fhould fides figure fince firft firſt fituate focus folid fome force tending fquare fubduplicate ratio fuch fuperficies fuppofe fyzygies given by pofition given ratio globe greateſt half-fheets hyperbola immovable increaſed interfections inverfely latus rectum lefs LEMMA let fall moſt motion move muſt obferved ofcillate orbit paffing parabola parallel particles perpendicular plane principal vertex prop proportional PROPOSITION quadratures quantity radius reafon reciprocally rectangle reft right line SCHOLIUM ſhall ſpace ſphere tangent thefe themſelves THEOREM theſe thofe thoſe trajectory triangles velocity whofe Widegate
Pasajes populares
Página 6 - Absolute, true, and mathematical time, of itself, and from its own nature, flows equably without relation to anything external, and by another name is called duration: relative, apparent, and common time, is some sensible and external (whether accurate or unequable) measure of duration by the means of motion, which is commonly used instead of true time; such as an hour, a day, a month, a year.
Página 11 - The effects which distinguish absolute from relative motion are the forces of receding from the axis of circular motion. For there are no such forces in a circular motion purely relative, but in a true and absolute circular motion they are greater or less, according to the quantity of the motion.
Página xxviii - Therefore the retardation is proportional to the motion communicated, and the communicated motion, when the velocity of the moving body is given, is as the density of the fluid; and therefore the retardation or resistance will be as the same density of the fluid; nor can it be taken away, unless the fluid, coming about to the hinder parts of the body, restore the motion lost.
Página 10 - A property near akin to the preceding is this, that if a place is moved, whatever is placed therein moves along with it; and therefore a body which is moved from a place in motion partakes also of the motion of its place. Upon which account all motions, from places in motion, are no other than parts of entire and absolute motions; and every entire motion is composed of the motion of the body out of its first place and the motion of this place out of its place; and...
Página 3 - ... line to the distance of two miles before it falls to the ground; the same, if the resistance of the air were taken away, with a double or decuple velocity, would fly twice or ten times as far.
Página 47 - ... increased or diminished in the ratio of the same length to the radius of the circle; that is, as the square of that length applied to the radius; and therefore the polygon, by having its sides diminished in infinitum, coincides with the circle, as the square of the arc described in a given time applied to the radius. This is the centrifugal force, with which the body impels the circle; and to which the contrary force, wherewith the circle continually repels the body towards the centre, is equal.
Página 46 - From the same demonstration it likewise follows that the arc which a body, uniformly revolving in a circle by means of a given centripetal force, describes in any time is a mean proportional between the diameter of the circle and the space which the same body falling by the same given force would descend through in the same given time.
Página 2 - This force consists in the action only and remains no longer in the body when the action is over. For a body maintains every new state it acquires, by its inertia only. Impressed forces are of different origins, as from percussion, from pressure, from centripetal force.
Página 13 - And thus we might find both the quantity and the determination of this circular motion, even in an immense vacuum, where there was nothing external or sensible with which the globes could be compared.
Página 27 - ... both. But the one extreme part HKI will with its whole weight bear upon and press the middle part towards the other extreme part EGF; and therefore the force with which EGI, the sum of the parts HKI and EGKH, tends towards the third part EGF, is equal to the weight of the part HKI, that is, to the weight of the third part EGF. And therefore the weights of the two parts EGI and EGF, one towards the other, are equal, as I was to prove. And indeed if those weights were not equal, the whole earth...