American socialites used to be listed in the Social Register. It was a list of names and addresses of the people who were thought to be more socially acceptable in the socially important families in the 19th century. In 1886, Louis Keller had the idea of combining these lists and selling them. Mr. Keller had great success. By 1918 there were 18 yearly volumes that covered 26 cities.
The term includes many people who are "famous because they are famous". These people are not famous because of something they have done. They are famous most often because of which family they are a member of and/or how they are talked about by the media.
Magnetic moment
The magnetic moment of a magnet is a quantity that determines the force that the magnet can exert on electric currents and the torque that a magnetic field will exert on it. A loop of electric current, a bar magnet, an electron, a molecule, and a planet all have magnetic moments.
Both the magnetic moment and magnetic field may be considered to be vectors having a magnitude and direction. The direction of the magnetic moment points from the south to north pole of a magnet. The magnetic field produced by a magnet is proportional to its magnetic moment as well. More precisely, the term "magnetic moment" normally refers to a system's magnetic dipole moment, which produces the first term in the multipole expansion of a general magnetic field. The dipole component of an object's magnetic field is symmetric about the direction of its magnetic dipole moment, and decreases as the inverse cube of the distance from the object.
In text books, two complementary approaches are used to define magnetic moments. In pre-1930's textbooks, they were defined using magnetic poles. Most recent textbooks define it in terms of Ampèrian currents.
Physicists represent sources of magnetic moments in materials as poles. The North and South poles are an analogy to the positive and negative charges in electrostatics. Consider a bar magnet which has magnetic poles of equal magnitude but opposite polarity. Each pole is the source of magnetic force which weakens with distance. Since s always come in pairs, their forces partially cancel each other because while one pole pulls, the other repels. This cancellation is greatest when the poles are close to each other i.e. when the bar magnet is short. The magnetic force produced by a bar magnet, at a given point in space, therefore depends on two factors: on both the strength formula_1 of its poles, and on the vector formula_2 separating them. The moment is defined as
It points in the direction from South to North pole. The analogy with electric dipoles should not be taken too far because magnetic dipoles are associated with angular momentum (see Magnetic moment and angular momentum). Nevertheless, magnetic poles are very useful for magnetostatic calculations, particularly in applications to ferromagnets. Practitioners using the magnetic pole approach generally represent the magnetic field by the irrotational field formula_4, in analogy to the electric field formula_5.
Suppose a planar closed loop carries an electric current formula_6 and has vector area formula_7 (formula_8, formula_9, and formula_10 coordinates of this vector are the areas of projections of the loop onto the formula_11, formula_12, and formula_13 planes). Its magnetic moment formula_14, vector, is defined as:
By convention, the direction of the vector area is given by the right hand grip rule (curling the fingers of one's right hand in the direction of the current around the loop, when the palm of the hand is "touching" the loop's outer edge, and the straight thumb indicates the direction of the vector area and thus of the magnetic moment).
If the loop is not planar, the moment is given as
In the most general case of an arbitrary current distribution in space, the magnetic moment of such a distribution can be found from the following equation:
where formula_18 is the position vector pointing from the origin to the location of the volume element, and formula_19 is the current density vector at that location.
The above equation can be used for calculating a magnetic moment of any assembly of moving charges, such as a spinning charged solid, by substituting
where formula_21 is the electric charge density at a given point and formula_22 is the instantaneous linear velocity of that point.
For example, the magnetic moment produced by an electric charge moving along a circular path is
where formula_18 is the position of the charge formula_25 relative to the center of the circle and formula_22 is the instantaneous velocity of the charge.
Practitioners using the current loop model generally represent the magnetic field by the solenoidal field formula_27, analogous to the electrostatic field formula_28.
A generalization of the above current loop is a multi-turn coil, or solenoid. Its moment is the vector sum of the moments of individual turns. If the solenoid has formula_29 identical turns (single-layer winding),
The unit for magnetic moment is not a base unit in the International System of Units (SI) and it can be represented in more than one way. For example, in the current loop definition, the area is measured in square meters and formula_6 is measured in amperes, so the magnetic moment is measured in ampere–square meters (formula_32). In the equation for torque on a moment, the torque is measured in Newton.meters and the magnetic field in tesla, so the moment is measured in N.m per Tesla (formula_33). These two representations are equivalent:
In the CGS system, there are several different sets of electromagnetism units, of which the main ones are ESU, Gaussian, and EMU. Among these, there are two alternative (non-equivalent) units of magnetic dipole moment in CGS:
and (more frequently used)
The ratio of these two non-equivalent CGS units (EMU/ESU) is equal exactly to the speed of light in free space, expressed in cm/s.
All formulas in this article are correct in SI units, but in other unit systems, the formulas may need to be changed. For example, in SI units, a loop of current with current I and area A has magnetic moment I×A (see below), but in Gaussian units the magnetic moment is I×A/c.
For relation between the notions of magnetic moment and magnetization see magnetization.
Bedworth
Bedworth is a small market town in Warwickshire, England. It is northwest of London, east of Birmingham, and north of the county town of Warwick. The town is home to many sights including The Bedworth Water Tower and The Nicholas Chamberlaine Almshouses. It was also known for mining, which is not done anymore. They also are known for the vast amount of Charity Shops which are located in most parts of the town.
The town is pronounced "Beduf" by the people that live there.
Thomas Schaaf
Thomas Schaaf (born 30 April 1961 in Mannheim) is a former German football player. Schaaf was a defender. He is now coach of SV Werder Bremen in the German Bundesliga.
After the death of his father the Schaaf family went to Bremen. They lived near the Weser Stadion. And so Thomas Schaaf came to SV Werder. He spent all his active and manager time with SV Werder. In 1972 he came to Werder Bremen's youth academy. 1978 he turned professional. Till 1994 he played 281 matches for Werder Bremen. He was with Bremen two times German Champion (1988, 1993) and two times Cup winner (1991, 1994). He also won the UEFA Cup in 1992. As player he played two times for the German U21 national team.