Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom
Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom
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In our eReader you can find the full English version of the book. Read Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom 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 Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom
What reading level is Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom book?
To quickly assess the difficulty of the text, read a short excerpt:
D (L cos 0) cos = dx 2. X Cr* At the centre of the circle the force is a maximum, and is = as in 195. The sign shows that with a posi- tive current the force is one of attraction.
38. Position of Equilibrium of a Circuit and Magnet.
Consider the magnet as composed of two poles of strength m and m connected rigidly. -. The formula for the force in the field may be written = sin 3 0.
The forces acting on the two poles are and /I 1 1 \ ^v.
e X & > / A B --- sin r Fig. 10.
The resultant force is ~ ...(sin^ - sin' G').
This is zero when = 0', or when the centre of the magnet is at the centre of the coil. In any other position there will be a force acting and the equilibrium will be unstable. If, there- fore, either the coil or magnet is free to move, the coil will NOTES ON place itself so that the middle of the magnet is at its centre. (See Fig. 87, " Thompson. ") 39. Mutual Potential of two Circuits ( 320).
The work done in bringing one circuit up to another, or the " mutual potential " of the two circuits is, as given in , cos s | 320, cc .
What to read after Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom?
You can find similar books in the "Read Also" column, or choose other free books by J B Joseph Ballard Murdock to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
D (L cos 0) cos = dx 2. X Cr* At the centre of the circle the force is a maximum, and is = as in 195. The sign shows that with a posi- tive current the force is one of attraction.
38. Position of Equilibrium of a Circuit and Magnet.
Consider the magnet as composed of two poles of strength m and m connected rigidly. -. The formula for the force in the field may be written = sin 3 0.
The forces acting on the two poles are and /I 1 1 \ ^v.
e X & > / A B --- sin r Fig. 10.
The resultant force is ~ ...(sin^ - sin' G').
This is zero when = 0', or when the centre of the magnet is at the centre of the coil. In any other position there will be a force acting and the equilibrium will be unstable. If, there- fore, either the coil or magnet is free to move, the coil will NOTES ON place itself so that the middle of the magnet is at its centre. (See Fig. 87, " Thompson. ") 39. Mutual Potential of two Circuits ( 320).
The work done in bringing one circuit up to another, or the " mutual potential " of the two circuits is, as given in , cos s | 320, cc .
What to read after Notes On Electricity And Magnetism Designed As a Companion to Silvanus P Thom?
You can find similar books in the "Read Also" column, or choose other free books by J B Joseph Ballard Murdock to read onlineMoreLess
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