A Treatise On Electricity And Magnetism Microform volume 1
A Treatise On Electricity And Magnetism Microform volume 1
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To quickly assess the difficulty of the text, read a short excerpt:
This action must be perpendicular to the element ds (Fig. 105); on the other hand, it should not change in direction when the element is made to turn by any quantity about the right line PO ; it is therefore null.
Let there now be an element ds (Fig. 106) which makes an angle a with the right line joining it to the pole; the element of current ds may be replaced by its two projections ds cos a and ds sin a, the one along the right line PO, the other in a perpendicular direction.
The action of t...he pole on the former is null ; there only then remains the action of the pole on ds sin a. This latter is propor- tional, as we have seen, to the mass m of the pole, to the intensity i of the current ; it is also proportional to the length ds sin a of the element, and lastly to a certain function of the distance f (r). Hence, if d is this force, and k a coefficient to be determined by experiment, d = mkids sin of (r) .
LAW OF BIOT AND SAVART.
443 The force is moreover applied to the element, and is per- pendicular to the plane Pds.
What to read after A Treatise On Electricity And Magnetism Microform volume 1?
You can find similar books in the "Read Also" column, or choose other free books by Leuthre Lie Nicolas Mascart to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
This action must be perpendicular to the element ds (Fig. 105); on the other hand, it should not change in direction when the element is made to turn by any quantity about the right line PO ; it is therefore null.
Let there now be an element ds (Fig. 106) which makes an angle a with the right line joining it to the pole; the element of current ds may be replaced by its two projections ds cos a and ds sin a, the one along the right line PO, the other in a perpendicular direction.
The action of t...he pole on the former is null ; there only then remains the action of the pole on ds sin a. This latter is propor- tional, as we have seen, to the mass m of the pole, to the intensity i of the current ; it is also proportional to the length ds sin a of the element, and lastly to a certain function of the distance f (r). Hence, if d is this force, and k a coefficient to be determined by experiment, d
LAW OF BIOT AND SAVART.
443 The force is moreover applied to the element, and is per- pendicular to the plane Pds.
What to read after A Treatise On Electricity And Magnetism Microform volume 1?
You can find similar books in the "Read Also" column, or choose other free books by Leuthre Lie Nicolas Mascart to read onlineMoreLess
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