ELECTRICITY MEASUREMENT APPARATUS
The present invention relates to an electricity measurement apparatus and a method of
electricity measurement, in particular for current measurement, power measurement and
Watthour metering.
When current flows through a conductor, a rotational magnetic field is set up. The magnitude of this magnetic field is proportional to the density of current flowing:
B α I/A (Equation 1)
where I is the total current, and A is the cross sectional area of the conductor. This value I/A
is the current density J.
It is known to use sensors, such as Hall effect sensors, to measure current flow though a
conductor by detecting the magnetic field. For example, using a Hall effect sensor, the sensor output signal has a voltage. VH. which is proportional to the magnetic field strength B at the
sensor, and a reference current Iref flowing through the sensor as follows:
VH = S x B x Iref (Equation 2).
The proportionality coefficient S is the sensitivity of the sensor. By keeping constant the current through the Hall sensor, a linear relationship is achieved between the detected
magnetic field and output voltage
If such a sensor is placed near a conductor, the two equations ( 1) and (2) above can be
combined allowing current flow J to be determined, current flow J being proportional to Hall
voltage VH
The present invention is defined in the claims to which reference should now be made
Preferred features are laid-out in the sub claims
The present invention preferably provides electricity measurement apparatus operative to
measure current flow along a conductor, the apparatus including a first sensor and a second sensor, each sensor being operative to detect magnetic field and to provide a current signal
dependent thereon at an output port, the output ports of the first and second sensors being connected together so as to provide a combined current signal of the difference between the current signals from the sensors, a systematic error in the combined signal being smaller in
magnitude than systematic error components in the current signals from the sensors Preferably, the systematic error components in the signals from the sensors are substantially cancelled by the differencing
The two sensors are preferably disposed equidistant from an magnetic field inducing conductor such that the sensors experience equal magnitude fields The conductor can be a mains electricity supply conductor, in particular conducting A C electricity of an electrical
supply network Alternatnely the conductor can conduct D C electricity The sensors can be on the same side of the conductor, or on opposite sides such that the impinging field is
of the same magnitude but opposite polarity. There can be multiple pairs of sensors.
The sensors are preferably Hall sensors, sensors of a pair preferably being supplied with
supply currents in opposite directions. Sensors are preferably connected via voltage to current
convertors such that alternate positive and negative output terminals of the convertors are
connected to a common line to provide the combined current signal. This has the advantage
that differential voltage amplifiers, which would themselves give rise to errors, are not
required to do the differencing operation.
A preferred embodiment of the present invention will now be described, by way of example,
and with reference to the figures, in which:
Figure 1 is a circuit diagram of a preferred embodiment of the invention; and
Figure 2 is a simplified schematic of the circuit.
As shown in Figure 1, the circuit consists of multiple pairs of Hall sensors 2,2'. each having left L and right R terminals connected to terminals of voltage-to-current convenor 4. Each
Hall sensor 2,2' receives a supply current from a current source 6, 14 which passes via a Hall
sensor 2.2' to a current sink 12.8. Each of a pair of Hall sensors 2.2' has current supplied in opposite directions.
The two Hall sensors 2.2' of a pair are equidistant from a mains conductor which transmits A.C. electricity and which induces an electromagnetic field around itself as mains current
flows such that the sensors 2,2' experience the same magnitude of electromagnetic field. In
alternative embodiments D.C. electricity could be conducted by the conductor. All sensors
are constructed on a single integrated circuit and so can be assumed to have common D.C.
offset errors and sensitivities to applied electromagnetic fields.
Each Hall sensor 2.2' has a potential difference VH' across it between left L and right R
terminals dependent on the magnitude of an electromagnetic field detected by that sensor 2.2'.
The voltage signals from left L and right R terminals are supplied to the voltage-to-current
convenor 4 which provides a current value IH' proportional to the potential difference VH'.
Irrespective of the direction of supply current. Hall sensors have D.C. offset errors which can change due to age, temperature and other factors. For multiple Hall sensors manufactured on a single integrated circuit as in the present embodiment, these errors can be assumed to be equal.
Odd sensors will provide voltage signals VH' as:
VH' = VH + VE (Equation 3)
where VH' is a measured potential difference. VH is the true Hall voltage, VE is a D.C.
offset error. Conversely, even sensors provide voltage signals VH' as:
VH' = -VH + VE (Equation 4)
After conversion into currents, the following relations apply:
for odd sensors:
IH' = IH + IE (Equation 5)
for even sensors:
IH' = -IH + IE (Equation 6)
where IH' is the output current signal from a Hall sensor.
Combining the output current signal from a first and second sensor and assuming that both
sensors have the same D.C. offset error IE give:
IH,' - IH:' = IH, + IE - (-IH, + IE) = IH, + IH,
(Equation 7).
Assuming IH, = IH, = IH ie that both sensors experience the same magnitude of magnetic
field and have the same sensitivity, gives:
IH,' - IH,' = 2IH (Equation 8).
Including components for each of the further sensor pairs gives:
n 2 Iouτ = Σ (IH,m.,' - IH:m') = 2m (IH) = n(IH) m=l (Equation 9)
where n is the number of sensors (an even number 2. 4, 6 ).
It can be seen that D.C. error components are simply removed by differencing.
Conversion to current allows this differencing to occur in a very simple manner as illustrated schematically in Figure 2. Simply by connecting alternate positive and negative output
terminals of voltage to current convertors 4 to a common line 10, 10' the current along the
common line is:
Iouτ = IH + IE + IH, - IE + IH, + IE + IH4 - IE (Equation 10)
IQ^J. = n (IH) where n is the number of sensors.