Watt balance

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The NIST watt balance; the vacuum chamber dome, which lowers over the entire apparatus, is visible at top

A watt balance is an experimental electromechanical weight measuring instrument that measures the weight of a test object very precisely by the strength of an electric current and a voltage. It is being developed as a metrological instrument that may one day provide a definition of the kilogram unit of mass based on electronic units,[1] a so-called "electronic" or "electrical" kilogram. The name watt balance comes from the fact that the weight of the test mass is proportional to the product of the current and the voltage, which is measured in units of watts.

Design[edit]

Precision Ampere balance at the US National Bureau of Standards (now NIST) in 1927. The current coils are visible under the balance, attached to the right balance arm. The Watt balance is a development of the Ampere balance.

The watt balance is a more accurate version of the Ampere balance, an early current measuring instrument in which the force between two current-carrying coils of wire is measured and then used to calculate the magnitude of the current. In this new application, the balance will be used in the opposite sense; the current in the coils necessary to support the weight of a standard kilogram mass will be measured, "weighing" the kilogram. The weight of the kilogram is then used to compute the mass of the kilogram by accurately determining the local gravitational acceleration. This will define the mass of a kilogram in terms of a current and a voltage, as described below. Since current and voltage units are defined in terms of fundamental physical constants such as the speed of light and Planck's constant, this will provide an alternative definition of the kilogram in terms of these absolute constants. This may be a better definition than the current one, which defines the kilogram as the mass of a physical artifact, the international prototype kilogram, which is vulnerable to deterioration or damage.

Origin[edit]

The principle of the watt balance was proposed by B. P. Kibble of the UK National Physical Laboratory (NPL) in 1975.[2] The main weakness of the ampere balance method is that the result depends on the accuracy with which the dimensions of the coils are measured. The watt balance method has an extra calibration step in which the effect of the geometry of the coils is eliminated, removing the main source of uncertainty. This extra step involves moving the force coil through a known magnetic flux at a known speed.

The watt balance originating from the British National Physical Laboratory was transferred to the National Research Council of Canada in 2009 and is currently being recommissioned.[3] Other watt balance experiments are being undertaken[when?] in the US National Institute of Standards and Technology (NIST), the Swiss Federal Office of Metrology (METAS) in Berne, the International Bureau of Weights and Measures (BIPM) near Paris and Laboratoire national de métrologie et d’essais (LNE) in Trappes, France.[4] As of 2011, the accuracy record is held by the U.S. NIST, with a relative uncertainty of 3.6×10−8,[5] and experiments are continuing towards a goal of 1×10−8.[3]

Principle[edit]

A conducting wire of length L which carries an electric current I perpendicular to a magnetic field of strength B will experience a Laplace force equal to BLI. In the watt balance, the current is varied so that this force exactly counteracts the weight of a standard mass m, which is given by the mass multiplied by the local gravitational acceleration g. This is also the principle behind the ampere balance.

Kibble's watt balance avoids the problems of measuring B and L with a second calibration step. The same wire (in practice a coil of wire) is moved through the same magnetic field at a known speed v. By Faraday's law of induction, a potential difference U is generated across the ends of the wire, which is equal to BLv. Hence the unknown quantities B and L can be eliminated from the equations to give

UI = mgv\,

Both sides of the equation have the dimensions of power, measured in watts in the International System of Units, hence the name "watt balance".

Measurements[edit]

Accurate measurements of electric current and potential difference are made in conventional electrical units (rather than SI units), which are based on fixed "conventional values" of the Josephson constant and the von Klitzing constant, KJ–90 and RK–90 respectively. The current watt balance experiments are equivalent to measuring the value of the conventional watt in SI units. From the definition of the conventional watt, this is equivalent to measuring the value of the product KJ2RK in SI units instead of its fixed value in conventional electrical units.

K_{\rm J}^2 R_{\rm K} = K_{\rm J-90}^2 R_{\rm K-90}\frac{mgv}{U_{90}I_{90}}

The importance of such measurements is that they are also a direct measurement of the Planck constant h:

h = \frac{4}{K_{\rm J}^2 R_{\rm K}}

The principle of the "electronic kilogram" would be to define the value of the Planck constant in the same way that the meter is defined by the speed of light. In this case, the electric current and the potential difference would be measured in SI units, and the watt balance would become an instrument to measure mass.

m = \frac{UI}{gv}

Any laboratory which had invested the (very considerable) time and money in a working watt balance would be able to measure masses to the same accuracy as they currently measure the Planck constant.

In addition to measuring UI, the laboratory must also measure v and g using experimental methods that do not depend on the definition of mass. The overall precision of m depends on the precisions of the measurements of U, I, v and g. Since there are already methods of measuring v and g to very high precision, the uncertainty of the mass measurement is dominated by the measurement of UI, which is the value measured by the watt balance.

References[edit]

  1. ^ Palmer, Jason (2011-01-26). "BBC News - Curbing the kilogram's weight-loss programme". Bbc.co.uk. Retrieved 2011-02-16. 
  2. ^ Kibble, B. P. (1975), Sanders, J. H.; Wapstra, A. H., eds., Atomic Masses and Fundamental Constants 5, New York: Plenum, pp. 545–51 
  3. ^ a b UK National Physical Laboratory: The Watt Balance
  4. ^ Mohr, Peter J.; Taylor, Barry N.; Newell, David B. (2008). "CODATA Recommended Values of the Fundamental Physical Constants: 2006". Rev. Mod. Phys. 80 (2): 633–730. arXiv:0801.0028. Bibcode:2008RvMP...80..633M. doi:10.1103/RevModPhys.80.633. 
  5. ^ Steiner, R. L.;Williams, E. R.; Liu, R.; Newell, D. B. (2007), "Uncertainty Improvements of the NIST Electronic Kilogram", IEEE Trans. Instrum. Meas. 56 (2): 592–596, doi:10.1109/TIM.2007.890590 

External links[edit]