Original Papers By the Late John Hopkinson 2
Original Papers By the Late John Hopkinson 2
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In Fig. 2 let Ai, A^, A^, A^ be the areas in sq. centims. of coil 1 and the ring-shaped areas included between the coils 1, 2, 3, 4 respectively. Then the induction at time f, as given by the integral of curve 1, divided by Ai is the average induction per sq.
centim. for this epoch over this area. Also, the induction at time ty as given by the integral of curve 2, minus the induction for the same time, as given by the integral of curve 1, divided by -dg, is the average induction per sq. centim.... for this area. Similarly, average induction per sq. centim. for ^s, A^ can be found for any epoch.
Consider area A^, It is obvious that all currents induced within the mass considered external to this area, due to changes of induction, plus the current in the magnetising coil per centim.
linear, at any epoch, go to magnetise this area, and, further, the induced currents in the outside of the area A^ itself go to magnet- ise the interior portion of this area. We know the electromotive forces at the radii 1, 2, 3, 4, and the lengths in centims.
What to read after Original Papers By the Late John Hopkinson 2?
You can find similar books in the "Read Also" column, or choose other free books by Hopkinson, John, 1849-1898 to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
In Fig. 2 let Ai, A^, A^, A^ be the areas in sq. centims. of coil 1 and the ring-shaped areas included between the coils 1, 2, 3, 4 respectively. Then the induction at time f, as given by the integral of curve 1, divided by Ai is the average induction per sq.
centim. for this epoch over this area. Also, the induction at time ty as given by the integral of curve 2, minus the induction for the same time, as given by the integral of curve 1, divided by -dg, is the average induction per sq. centim.... for this area. Similarly, average induction per sq. centim. for ^s, A^ can be found for any epoch.
Consider area A^, It is obvious that all currents induced within the mass considered external to this area, due to changes of induction, plus the current in the magnetising coil per centim.
linear, at any epoch, go to magnetise this area, and, further, the induced currents in the outside of the area A^ itself go to magnet- ise the interior portion of this area. We know the electromotive forces at the radii 1, 2, 3, 4, and the lengths in centims.
What to read after Original Papers By the Late John Hopkinson 2?
You can find similar books in the "Read Also" column, or choose other free books by Hopkinson, John, 1849-1898 to read onlineMoreLess
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