Proceedings. [Imperf. With] Index, vol.i to lxii, Томи 12 – 15 |
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Сторінка 52
... whole angle , between the component axes , is divided by the new axis of rotation . Again AC : AD = or = sin ADC : sin ACD sin BAD : sin ABD vv sin BAD : sin BAC . : v " = v ' Let ALBK ( Figs . 4 and 5 ) be a sphere rotating about the ...
... whole angle , between the component axes , is divided by the new axis of rotation . Again AC : AD = or = sin ADC : sin ACD sin BAD : sin ABD vv sin BAD : sin BAC . : v " = v ' Let ALBK ( Figs . 4 and 5 ) be a sphere rotating about the ...
Сторінка 53
... whole arc AFB , tends to make the sphere rotate about the axis AB in the direction of the arrow M. Again , the impulse applied at A , in the direction AR , causes B to move in the direction BQ ; when the particle at B is carried by the ...
... whole arc AFB , tends to make the sphere rotate about the axis AB in the direction of the arrow M. Again , the impulse applied at A , in the direction AR , causes B to move in the direction BQ ; when the particle at B is carried by the ...
Сторінка 54
... whole sphere AMBM ' be divided into laminæ AB , & c . , whose planes are parallel to each other , and at right angles to SC . If the whole of the matter of each lamina be collected into its centre of gravity , the equilibrium of the ...
... whole sphere AMBM ' be divided into laminæ AB , & c . , whose planes are parallel to each other , and at right angles to SC . If the whole of the matter of each lamina be collected into its centre of gravity , the equilibrium of the ...
Сторінка 55
... whole line M'M always lies between G and M ; therefore the orbitual motion of the line M'M about the centre S , resists the rotatory motion of the same line M'M about the centre of gravity G. But the line M'M is made up of the centres ...
... whole line M'M always lies between G and M ; therefore the orbitual motion of the line M'M about the centre S , resists the rotatory motion of the same line M'M about the centre of gravity G. But the line M'M is made up of the centres ...
Сторінка 60
... whole circumference in latitude A : time of describing the whole circumference at P = ab : cd . = 1 sin lat . A. Time in lat A = Time at P sin lat . = 24 hours sin lat . 24 hours = Infinity . and Time at Equator = As I am by no means ...
... whole circumference in latitude A : time of describing the whole circumference at P = ab : cd . = 1 sin lat . A. Time in lat A = Time at P sin lat . = 24 hours sin lat . 24 hours = Infinity . and Time at Equator = As I am by no means ...
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