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 The principle of the watt balance
 Summary The BIPM watt balance: general concept The principle of the watt balance Present status Coil suspension and electrostatic motor Current source and voltage reference Magnet Magnetic field alignment Optical systems to measure coil displacements Dynamic alignment mechanism Vibration isolation Local gravitational acceleration cartography Cryogenic watt balance: general concept Cryogenic watt balance: present status BIPM collaborators on the project Recent publications Director's Report 2012
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The concept of the moving coil watt balance was proposed by B. P. Kibble (NPL) in 1975. The experiment consists of two parts: the weighing and the moving experiments.

 Weighing experiment Moving experiment In the weighing experiment, a mass and a coil are suspended from a balance. The coil (wire length L) is placed in a magnetic field of flux density B. The gravitational force on the mass m is balanced by an equal and opposite electromagnetic force on the coil by sending a current I through it: m g = I L B In the moving experiment, the coil is moved at a vertical speed v through the magnetic field so that a voltage U is induced: U = B L v

If the properties of the coil and the magnetic field, L and B, and their alignment, do not change between the two experiments, they can be eliminated from both equations, which leads to the new equation

U I = m g v

which shows an electrical power on the left-hand side and a mechanical power on the right-hand side. This explains the name of the experiment, since the watt is the unit of power. It is important to understand that both types of power are only "virtual", in the sense that they do not appear in one of the single phases of the experiment. In the case of the electrical power, the voltage is measured in the moving experiment, and the current in the weighing experiment.

To establish a link between the macroscopic mass m and the Planck constant h, the electrical quantities voltage and current are measured by using two macroscopic quantum phenomena, the Josephson effect and the quantum Hall effect.

The Josephson effect allows us to determine an unknown voltage U as a dimensionless multiple u' of a combination of the Planck constant, the elementary charge and a precisely measurable frequency fJ:

 U = u' fJ h = u' fJ 2e KJ

The quantum Hall effect allows us to determine an unknown resistance R as a dimensionless multiple r' of a different combination of the Planck constant and the elementary charge:

 R = r' h = r' RK e2

The application of both effects on the measurement of the voltage and the current in the watt balance equation leads to:

 m = u1' u2' fJ,1 fJ,2 1 h r' g v 4

where the first component on the right-hand side shows the quantities related to the measurement of the voltage and the current using the macroscopic quantum effects, the second component shows the mechanical measurands gravitational acceleration g and velocity v, and the last term is the Planck constant. This equation establishes the link between the macroscopic mass m and the Planck constant h.

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