Elements of Natural Philosophy, Volume 1 |
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Page 47
It is clear that these three elementary component strains may be applied in any
other order as well as that stated . Thus , if the simple elongation is made first ,
the body thus altered must get just the same shear in planes perpendicular to the
...
It is clear that these three elementary component strains may be applied in any
other order as well as that stated . Thus , if the simple elongation is made first ,
the body thus altered must get just the same shear in planes perpendicular to the
...
Page 55
... or the edge of the sharpest knife , is still a surface , and acts as such on the
bodies to which it may be applied . Even the most rigid substances , when
brought together , do not touch at a point merely , but mould each other so as to
produce a ...
... or the edge of the sharpest knife , is still a surface , and acts as such on the
bodies to which it may be applied . Even the most rigid substances , when
brought together , do not touch at a point merely , but mould each other so as to
produce a ...
Page 59
... preceding statement , by making the parts into which we divide them
sufficiently small . On this understanding the preceding definition may be applied
to define the centre of inertia of a system of material points , whether given equal
or not .
... preceding statement , by making the parts into which we divide them
sufficiently small . On this understanding the preceding definition may be applied
to define the centre of inertia of a system of material points , whether given equal
or not .
Page 66
If any force generates motion , a double force will generate double motion , and
so on , whether simultaneously or successively , instantaneously or gradually ,
applied . And this motion , if the body was moving beforehand , is either added to
...
If any force generates motion , a double force will generate double motion , and
so on , whether simultaneously or successively , instantaneously or gradually ,
applied . And this motion , if the body was moving beforehand , is either added to
...
Page 67
... be the equivalent of any number of simultaneously acting forces . Hence The
resultant of any number of forces ( applied at one point ) is to be found by the
same geometrical process as the resultant of any number of simultaneous
velocities .
... be the equivalent of any number of simultaneously acting forces . Hence The
resultant of any number of forces ( applied at one point ) is to be found by the
same geometrical process as the resultant of any number of simultaneous
velocities .
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Common terms and phrases
acceleration according acting action amount angle angular applied attraction axes axis body called centre centre of inertia circle component condition consider constant corresponding couple course curvature curve denote density described determined direction displacement distance divided effect elastic elements energy equal equations equilibrium evidently expression figure fixed fluid force friction give given gravity harmonic Hence important increase infinitely small instant interval kinetic length less mass matter mean measured method motion moving natural normal observation opposite parallel particle passing path perpendicular plane portion position potential practical pressure principle problem produce projection proportional quantity radius reference relative remain remarkable respectively rest resultant right angles rigid rotation round sides simple solid space spherical square straight strain stress suppose surface theory turned uniform unit velocity weight whole wire