IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 59, NO. 8, AUGUST 2010 2211
D-Dot Probe for Fast-Front
High-Voltage Measurement
Ibrahim A. Metwally, Senior Member, IEEE
Abstract—This paper presents the operating principle, design,
and testing of a coaxial D-dot (the time derivative of electric
flux density) probe to measure fast-front high voltages, e.g., the
residual voltages of surge arresters (SAs). This probe consists
of three identical copper toroids placed around a high-voltage
electrode, where all are coaxially assembled in a large earthed
cylinder. The probe was first simulated by a finite-element package
to optimize the assembly and reduce the electric field inside it.
This was confirmed by an alternating current test to ensure a
corona-free design. Simultaneous impulse voltage measurements
were done using the designed D-dot probe—two commercial
mixed resistive–capacitive (RC ) probes and a damped capacitive
voltage divider. The linearity of the D-dot probe was checked
under unloaded and loaded conditions. Results reveal that the
larger the toroid separation and/or the lower the attenuator capac-
itance is, the higher the measured voltage from the middle “signal”
toroid will be. The residual voltage waveforms for an 11-kV SA,
measured by two commercial mixed RC probes and the damped
capacitive voltage divider, showed an initial inductive overshoot
superimposed on the waveform and a significant decay, even before
the current peak instant. On the contrary, the voltage measured
by the designed D-dot probe gave a voltage waveform that looked
like that of the current and slightly led the latter. For the damped
capacitive voltage divider and the two commercial mixed RC
probes, neither the peak voltage nor the voltage at peak current
gave the correct current–voltage characteristics. This confirms the
contradiction of some published SA models in the high-conduction
regime because most models were based on measurements done by
different and large-impulse capacitive or resistive voltage dividers
with improper compensation.
Index Terms—D-dot probes, electric field sensors, fast-front
voltages, impulse voltage measurement, surge arresters (SAs),
voltage dividers.
I. I NTRODUCTION
F
AST-FRONT voltages or currents are normally generated
by system faults or disconnector operation within gas-
insulated switchgear (GIS), operation of metal–oxide or zinc
oxide surge arresters (ZnO SA), punctures of insulators, etc.
The fastest one is generated within a GIS, where a steep voltage
with a rise time in the range of some nanoseconds can be found
Manuscript received December 30, 2008; revised July 27, 2009; accepted
August 4, 2009. Date of publication October 13, 2009; date of current version
July 14, 2010. This work was supported by Sultan Qaboos University, Muscat,
Sultanate of Oman. The Associate Editor coordinating the review process for
this paper was Dr. Jerome Blair.
The author is with the Department of Electrical and Computer Engineering,
College of Engineering, Sultan Qaboos University, Muscat 123, Oman (e-mail:
metwally@squ.edu.om; metwally@mans.edu.eg).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TIM.2009.2030928
[1]. Special measuring systems are needed for the measurement
of all previously mentioned fast-front voltages.
SAs protect medium- and high-voltage systems and equip-
ment against lightning and switching surges, i.e., external and
internal overvoltages, respectively. They exhibit an extremely
high resistance during normal operation and a very low resis-
tance during transient overvoltages, i.e., dynamic characteristic
[2], [3]. The highly nonlinear current–voltage (I –V ) character-
istic of ZnO SAs obviates the need for series spark gaps. The
electrical characteristics are determined solely by the properties
of the ZnO blocks.
Several models have been proposed to simulate this
frequency-dependent characteristic [2], [4]–[10]. Difficulties
arise in the calculation and adjustment of their parameters,
where in some cases iterative procedures are required, while
in others the necessary data are not reported on manufacturers’
datasheets. The differences among the proposed models arise in
the difficulties of the parameter estimation.
For the IEEE SA model, an early voltage overshoot occurs at
about 37% of the current front time irrespective of the current
magnitude [5]. In addition, there is a bad response in the voltage
tail for fast-front currents (lightning currents), where the tail
of voltage waveform dropped very sharply [6]. Moreover, it
was observed that for the case of relatively slow surges, only
the conventional model suffices [8], [11]. On the other hand,
the conventional model proposed in electromagnetic transient
program (EMTP) shows that the peak voltage instantaneously
occurs with that of the current because the arrester is modeled
by a pure nonlinear resistor only [8], [11]. Other models in
[7] and [9] also do not give the actual voltage response of
the arrester, particularly for the fast-front currents. None of the
published SA models gives the expected nonlinear behavior of
the arresters because all models are based on measured data,
where the residual voltage is inaccurately measured due to
the following factors: 1) circuit inductance; 2) voltage divider
inductance and response time; and 3) signal cable problems
[4]–[10]. Moreover, some of the previously mentioned models
considered linear [4], [5], [7]–[10] and nonlinear [6] inductance
in series with the nonlinear resistance of the ZnO blocks. While
others represented the ZnO blocks without any inductances at
all, e.g., [11].
In this paper, the operating principle, design, and testing
of a coaxial D-dot probe to measure fast-front high voltages
are presented. The designed probe has proved its advanta-
geous performance over two commercial mixed RC probes
and a damped capacitive voltage divider, particularly when
measuring the residual voltage of SA in the high-conduction
regime. Adopting these D-dot probes in fast-front voltage
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