A Treatise on Electricity and Magnetism, Vol. II (1873) - Page 13

Article		Page
409.	The potential of a magnetic shell at any point is the product of its strength multiplied by the solid angle its boundary subtends at that point	32
410.	Another method of proof	33
411.	The potential at a point on the positive side of a shell of strength Φ exceeds that on the nearest point on the negative side by 4πΦ	34
412.	Lamellar distribution A distribution of magnetism arranged in thin layers or sheets. of magnetism	34
413.	Complex lamellar distribution	34
414.	Potential of a solenoidal magnet A magnet where the magnetism is distributed along the length of a tube or wire.	35
415.	Potential of a lamellar magnet	35
416.	Vector-potential of a lamellar magnet	36
417.	On the solid angle subtended at a given point by a closed curve	36
418.	The solid angle expressed by the length of a curve on the sphere	37
419.	Solid angle found by two line-integrations	38
420.	Π The Greek letter Pi, here representing a specific mathematical function. expressed as a determinant	39
421.	The solid angle is a cyclic function	40
422.	Theory of the vector-potential of a closed curve	41
423.	Potential energy of a magnetic shell placed in a magnetic field	42

CHAPTER IV.

Article		Page
424.	When a body under the action of magnetic force becomes itself magnetized, the phenomenon is called magnetic induction	44
425.	Magnetic induction in different substances	45
426.	Definition of the coefficient of induced magnetization	47
427.	Mathematical theory of magnetic induction: Poisson's method	47
428.	Faraday's method	49
429.	Case of a body surrounded by a magnetic medium	51
430.	Poisson's physical theory of the cause of induced magnetism	53

Article		Page
431.	Theory of a hollow spherical shell	56
432.	Case when κ The Greek letter kappa, representing the magnetic susceptibility or coefficient of magnetization. is large	58
433.	When i = 1	58
434.	Corresponding case in two dimensions (See Figure 15)	59
435.	Case of a solid sphere, where the coefficients of magnetization are different in different directions	60