A New Potential Principle in Nature Elasticity a Mode of Motion Being a Popula
A New Potential Principle in Nature Elasticity a Mode of Motion Being a Popula
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In our eReader you can find the full English version of the book. Read A New Potential Principle in Nature Elasticity a Mode of Motion Being a Popula Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book A New Potential Principle in Nature Elasticity a Mode of Motion Being a Popula
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To quickly assess the difficulty of the text, read a short excerpt:
Let us take the body m moving with velocity v in the straight line A B. Hang another body mi = to m from a point O by an inextensible cord, so that the body m\ will be at rest in the straight line A B, and m will impinge and give up all its energy to m l . See Fig. 2.
Now mi by means of the cord and fixture at o will be constrained to move in the circumference of a circle of which the cord is the radius, and with the same velocity in the curve that it had in the straight line, which proves that... it has the same kinetic energy as formerly.
But we also become cognizant of another stress or energy, or capacity to do work along the cord, which we can measure by a spring balance inserted in place of the cord and fixed to O, and the measure of that stress as shown by the balance is m\ v\ and in different circles is - But the actual stress due to m\ = ~, that is 2i easily proven by using another mass #z 2 = to mi caused to revolve by an extension of the cord, forming a diameter to the circle.
What to read after A New Potential Principle in Nature Elasticity a Mode of Motion Being a Popula?
You can find similar books in the "Read Also" column, or choose other free books by Robert Stevenson to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
Let us take the body m moving with velocity v in the straight line A B. Hang another body mi = to m from a point O by an inextensible cord, so that the body m\ will be at rest in the straight line A B, and m will impinge and give up all its energy to m l . See Fig. 2.
Now mi by means of the cord and fixture at o will be constrained to move in the circumference of a circle of which the cord is the radius, and with the same velocity in the curve that it had in the straight line, which proves that... it has the same kinetic energy as formerly.
But we also become cognizant of another stress or energy, or capacity to do work along the cord, which we can measure by a spring balance inserted in place of the cord and fixed to O, and the measure of that stress as shown by the balance is m\ v\ and in different circles is - But the actual stress due to m\ = ~, that is 2i easily proven by using another mass #z 2 = to mi caused to revolve by an extension of the cord, forming a diameter to the circle.
What to read after A New Potential Principle in Nature Elasticity a Mode of Motion Being a Popula?
You can find similar books in the "Read Also" column, or choose other free books by Robert Stevenson to read onlineMoreLess
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