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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Dynamic Datum Transformations in Australia and New Zealand</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Dr. Craig Harrison Geoscience Australia Canberra</string-name>
          <email>R@Locate14</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
          <xref ref-type="aff" rid="aff3">3</xref>
          <xref ref-type="aff" rid="aff4">4</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Dr. Chris Crook National Geodetic Office Land Information New Zealand Wellington</institution>
          ,
          <country>New Zealand CRC for Spatial Information</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Dr. Chris Rizos Dr. Craig Roberts Civil and Environmental EngineeringCivil and Environmental Engineering University of New South Wales University of New South Wales Sydney, NSW Sydney, NSW CRC for Spatial Information CRC for Spatial Information</institution>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Joel Haasdyk Survey Infrastructure and Geodesy NSW Land and Property Information Bathurst, NSW CRC for Spatial Information</institution>
        </aff>
        <aff id="aff3">
          <label>3</label>
          <institution>Nic Donnelly National Geodetic Office Land Information New Zealand Wellington</institution>
          ,
          <country>New Zealand CRC for Spatial Information</country>
        </aff>
        <aff id="aff4">
          <label>4</label>
          <institution>Richard Stanaway Civil and Environmental Engineering University of New South Wales Sydney, NSW CRC for Spatial Information</institution>
        </aff>
      </contrib-group>
      <fpage>48</fpage>
      <lpage>59</lpage>
      <abstract>
        <p>Dynamic datums, which account for crustal dynamics, are widely used in Australia and New Zealand, although in many cases users may not be aware that they are using such a datum. The most widely-used global dynamic datums in Australia and New Zealand are the International Terrestrial Reference Frame (ITRF) and the World Geodetic System 1984 (WGS84). The use of WGS84 presents particular challenges, as it cannot be directly accessed at the sub-metre level by most spatial professionals. The relationship between WGS84 and ITRF is explored in detail, leading to recommendations on how users should deal with WGS84 datasets. New Zealand and Australia have taken different approaches to modelling the relationship between global dynamic datums and their local geodetic datums. Australia has calculated a set of local transformation parameters, which incorporate tectonic movements. New Zealand has adopted a set of global parameters, and uses a deformation model to account for crustal dynamics. As both countries seek to modernise their geodetic datums, the availability of simple yet accurate transformations will be critical to the success of the modernisation process. This paper outlines the options for dynamic datum transformations within a modernised datum, discussing the strengths and weaknesses of each approach.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1 Introduction</title>
      <p>Global positioning technologies have driven a profound change in the way in which geospatial data is collected and
referenced. There is an ongoing shift away from relative measurements, made in local coordinate reference systems,
to absolute positioning, made in terms of global coordinate reference systems. Global Navigation Satellite Systems
(GNSS), of which the U.S. Global Positioning System (GPS) is the most widely used, provide positions in a global
geocentric reference frame. Such positions may be regarded as three-dimensional position vectors originating at the
centre of mass of the Earth, and terminating at the physical feature or point being measured with the GNSS device.</p>
      <p>The points being measured are attached to the surface of the Earth, which is continually moving due to crustal
dynamics and other localised deformations. Thus if a point is regularly re-measured, its coordinates will change to
reflect the reality that the point’s relationship to the centre of the Earth has changed due to crustal dynamics. A
reference frame or datum which enables this changing position to be tracked is referred to as ‘dynamic’.</p>
      <p>The two most widely used global dynamic reference frames in Australia and New Zealand (and much of the rest
of the world) are the International Terrestrial Reference Frame (ITRF) and the World Geodetic System 1984
(WGS84). There are in fact a number of versions (or realisations) of each of these reference frames, and correct
management of the various realisations is critical for high-precision positioning applications.</p>
      <p>
        It is common practice for individual countries or geographic regions to define their own geodetic datums. These
datums are often mandated for use in activities such as national mapping and cadastral surveying. Even where their
use is not mandated, the national datum is usually the most appropriate reference frame to use for geospatial data, as
that data is then easily integrated or compared with other datasets using the same datum. For Australia the national
datum is the Geocentric Datum of Australia 1994 (GDA94)
        <xref ref-type="bibr" rid="ref11 ref12 ref16">(ICSM, 2013a)</xref>
        . This is a static datum aligned to
ITRF92 at epoch 1994.0. For New Zealand, the national datum is New Zealand Geodetic Datum 2000 (NZGD2000)
        <xref ref-type="bibr" rid="ref5">(Blick, 2003)</xref>
        . NZGD2000 is referred to as a ‘semi-dynamic’ datum, as it incorporates a deformation model to refer
measurements and coordinates to a common epoch. It is aligned with ITRF96 at epoch 2000.0.
      </p>
      <p>
        GNSS measurements are often made in terms of a global reference frame, but presented as a derived final
product in terms of the national geodetic datum. An important component of a nation’s positioning infrastructure is
the determination and maintenance of transformations from commonly used global reference frames to the national
geodetic datum. A coordinate transformation is a mathematical operation that enables coordinates expressed in one
reference frame (or datum) to be represented in terms of another
        <xref ref-type="bibr" rid="ref3">(ISO, 2008)</xref>
        . It is distinguished from coordinate
propagation, which enables coordinates referenced to a particular epoch to be represented at another epoch, within
the same reference frame. Official transformations in New Zealand and Australia focus on the relationship between
the various ITRF realisations and the national datum. Conversely, despite the widespread use of WGS84,
transformation parameters from WGS84 coordinates to the national datums are generally not widely known. This is
due to factors such as the inaccessibility of WGS84 as a reference frame for sub-metre positioning (since there is a
lack of accurate WGS84 ground control for relative positioning), and the consequent relatively high uncertainties
associated with WGS84 datasets. Nevertheless, accurate transformations between WGS84 realisations and national
datums can be determined via the relationship between ITRF and WGS84. For some datasets, knowing these
transformations may be important.
      </p>
      <p>
        The concept of ‘uncertainty’ is an important, but often overlooked, aspect of coordinate transformations. When
considering positioning in terms of global reference frames, uncertainty of Cartesian coordinates is the relevant
measure. This concept is referred to as ‘positional uncertainty’ in Australia
        <xref ref-type="bibr" rid="ref11 ref12">(ICSM, 2013b)</xref>
        , and ‘network accuracy’
in New Zealand (LINZ, 2009). There is usually little value in performing a transformation if the accuracy of a
geospatial dataset is low, and consequently the uncertainty of the coordinates is substantially greater than the
coordinate change determined from those transformation parameters. On the other hand, the uncertainty resulting
from the process of the transformation itself is also rarely accounted for
        <xref ref-type="bibr" rid="ref9">(Haasdyk &amp; Janssen, 2011)</xref>
        , and more
attention will need to given to this process as measurements and datums improve in accuracy.
      </p>
      <p>This paper describes the dynamic global reference frames used in Australia and New Zealand, with a focus on
WGS84, which is widely used but frequently misunderstood. It reviews the transformation parameters used in both
countries between ITRF and the national datum, extending these for use with WGS84 datasets. Finally, as both
Australia and New Zealand work towards modernisation of their national datums, options for dynamic datum
transformations are considered in terms of future trends in positioning and geodetic datums.</p>
    </sec>
    <sec id="sec-2">
      <title>2 The International Terrestrial Reference Frame (ITRF)</title>
      <p>
        The International Earth Rotation and Reference Systems Service (IERS) is responsible for the maintenance and
development of the International Terrestrial Reference Frame (ITRF), upon which all modern national geodetic
datums are based. A reference frame is a realisation, according to a set of agreed conventions
        <xref ref-type="bibr" rid="ref18 ref6">(Petit and Luzum,
2010)</xref>
        , of the idealised International Terrestrial Reference System (ITRS).
      </p>
      <p>A terrestrial reference system is one which is co-rotating with the Earth about a conventional pole (ibid, 2010).
Various models are applied to remove the impact of phenomena such as ocean loading and earth tides, with the
effect that the coordinates of a point on the Earth's surface do not change in response to these geophysical effects
(ibid, 2010). The reference system needs to be very stable for monitoring long-term global phenomena such as
sealevel change.</p>
      <p>
        The latest realisation of the ITRF is ITRF2008
        <xref ref-type="bibr" rid="ref1 ref4">(Altamimi et al., 2011)</xref>
        . A realisation of ITRF produces estimates
of station coordinates and linear velocities for hundreds of stations worldwide. ITRF is now stable at the
centimetrelevel or better (ibid, 2011). Transformation parameters between the two most recent realisations of the ITRF
        <xref ref-type="bibr" rid="ref1 ref2">(ITRF2008 and ITRF2005)</xref>
        are at the sub-centimetre level, a level of agreement which is likely to continue (or
improve) for future realisations.
 
 
      </p>
      <p>
        There is also a global tectonic plate model published in conjunction with ITRF2008
        <xref ref-type="bibr" rid="ref2">(Altamimi et al., 2012)</xref>
        which may be used to propagate coordinates between epochs using the defined Euler pole for 14 major tectonic
plates. This model is a No-Net-Rotation (NNR) model derived from the station velocities published for ITRF2008,
which aligns the orientation of all ITRFs to each other, and to the available geophysical models. Such a plate
motion model works well for most of the Earth, where it is assumed that tectonic plates are non-deforming (that is,
they are rigid plates that rotate about a point). This assumption is not valid near plate boundaries, which is the case
for New Zealand, or where high accuracy over large distances is required, which is the case for all national geodetic
datums. Both New Zealand and Australia have their own models for propagating coordinates, and do not directly
use the ITRF2008 plate motion model.
      </p>
      <p>
        The majority of users access the ITRF through GNSS technology, and associated products and services. The
most precise products (such as satellite orbits) are produced by the International GNSS Service (IGS). The IGS
produces its own ITRF-aligned reference frame, the current realisation being aligned to ITRF2008 and denoted
IGb08
        <xref ref-type="bibr" rid="ref14">(IGS, 2010)</xref>
        . The high degree of alignment between these frames means that they can be considered identical
for all but the highest precision geodetic applications.
      </p>
    </sec>
    <sec id="sec-3">
      <title>3 The World Geodetic System 1984 (WGS84)</title>
      <p>The term ‘WGS84’ is one of the more ambiguous in global geodesy, which sometimes leads to confusion about the
exact nature of this datum. Firstly, depending on context, WGS84 may refer to a reference system, a reference
frame or a reference ellipsoid, which are each defined in more detail below. Secondly, even where it is clear from
the context that it is the reference frame WGS84 which is the subject of discussion, the fact that there have been
several different WGS84 reference frames is often not made clear. In general all are simply referred to as ‘WGS84’.</p>
      <p>WGS84 is managed by the National Geospatial Intelligence Agency (NGA), formerly the National Imagery and
Mapping Agency (NIMA), which was itself the successor to the Defense Mapping Agency (DMA). The DMA was
responsible for developing the WGS84 reference system and for the initial reference frame realisation.</p>
      <sec id="sec-3-1">
        <title>3.1 WGS84: the reference system</title>
        <p>
          The WGS84 reference system is designed to coincide as closely as possible with the ITRS
          <xref ref-type="bibr" rid="ref15">(NIMA, 2000)</xref>
          . The
origin is the centre of mass of the Earth, scale is that of the local Earth frame (in the sense of the theory of general
relativity) and initial orientation was consistent with that defined by the Bureau International de l'Heure (BIH) in
1984. The evolution of the orientation in time is such that there is no overall rotation of the system with respect to
the Earth's surface
          <xref ref-type="bibr" rid="ref15">(NIMA, 2000)</xref>
          .
        </p>
        <p>
          WGS84 is a right-handed, orthogonal reference system. Its X-axis is consistent with the IERS Reference
Meridian (which is approximately equal to the Greenwich Meridian), the Z-axis is coincident with the IERS
Reference Pole (which is approximately the geographical North Pole), and the Y-axis is oriented at ninety degrees
with respect to the other two axes
          <xref ref-type="bibr" rid="ref15">(NIMA, 2000)</xref>
          .
        </p>
        <p>It is the consistency of definition between the WGS84 and ITRS reference systems which results in the high
levels of consistency between coordinates realised in the WGS84 and ITRF reference frames.</p>
      </sec>
      <sec id="sec-3-2">
        <title>3.2 WGS84: the ellipsoid</title>
        <p>
          The WGS84 ellipsoid is a reference surface approximating the size and shape of the Earth. Its origin is the centre of
mass of the Earth, and it is formed by rotating an ellipse about the Z-axis. It is almost identical to the Geodetic
Reference System 1980 (GRS80) ellipsoid associated with the ITRF. The slight difference in flattening is due to a
truncation during the computation of the WGS84 flattening value, but is insignificant for all but the highest
precision geodetic applications
          <xref ref-type="bibr" rid="ref15">(NIMA, 2000)</xref>
          . The difference in ellipsoidal heights calculated using the two
ellipsoids is a maximum of just 0.1mm, at the poles. Table 1 lists the key parameters of the two ellipsoids.
        </p>
      </sec>
      <sec id="sec-3-3">
        <title>3.3 WGS84: the reference frames</title>
        <p>
          A WGS84 reference frame is a realisation of the WGS84 reference system through the defined coordinates (and
more recently, velocities) for a set of reference stations
          <xref ref-type="bibr" rid="ref22">(Wong et al., 2012)</xref>
          . These reference stations and their
coordinates are then used for applications such as calculating the orbits of GPS satellites. It is through orbital
products such as the GPS broadcast ephemeris that the geospatial community is able to access the WGS84 reference
frame. As at the start of 2014, the current realisation of the WGS84 system is the fifth such realisation.
        </p>
        <p>
          The first realisation is the only one officially denoted as ‘WGS84’. To avoid confusion, in the remainder of this
paper, we denote this first WGS84 reference frame as ‘WGS84(Doppler)’, since it was based on the TRANSIT
Doppler system, the predecessor positioning system to GPS. Each subsequent WGS84 realisation is distinguished
by appending the GPS week in which the reference frame was implemented
          <xref ref-type="bibr" rid="ref15">(NIMA, 2000)</xref>
          . For example, the
current realisation is denoted ‘WGS84(G1674)’, as it was implemented by the GPS Operational Control Segment
(OCS) on 8 February 2012, which is GPS Week 1674
          <xref ref-type="bibr" rid="ref22">(Wong et al., 2012)</xref>
          .
        </p>
        <p>Wong et al (2012) provide full details of the current WGS84 realisation. This was aligned to ITRF2008 through
direct adoption, where possible, of ITRF2008 coordinates published by the IERS for 11 WGS84 monitor stations
distributed around the globe. Corrections were made to account for discontinuities due to activities such as
equipment maintenance. For two stations, BHR2 in Bahrain and OSN1 in South Korea, the ITRF2008 coordinates
could not be constrained without introducing large residuals, so these stations had new coordinates calculated. New
coordinates were also calculated for the six United States Air Force sites which comprise the OCS. Velocities for
the monitor stations were adopted from the ITRF2008 solution. For the OCS stations, velocities were adopted from
a nearby International GNSS Service (IGS) station.</p>
        <p>Table 2 summarises each of the five WGS84 reference frame realisations, indicating that since 2002 the
positional uncertainty of the reference frame relative to the ITRF is about one centimetre, estimated based on the
magnitude of similarity transformation parameters calculated between the ITRF and WGS84 precise orbits.</p>
      </sec>
      <sec id="sec-3-4">
        <title>3.4 WGS84: An operational dynamic datum</title>
        <p>
          WGS84 is probably the most widely used global reference frame. This popularity stems from its use as the
reference frame for GPS orbits – the broadcast ephemeris used for GPS single point positioning. The reference
frame of the GPS orbit determines the reference frame of the user position for this type of absolute positioning. On
the 1 January each year, the coordinates of the GPS master control stations are propagated to an epoch in the middle
of the year, and GPS satellite coordinates are determined relative to these master stations. Thus WGS84 coordinates
determined by GPS single point positioning are related to the epoch of the middle of the calendar year in which the
observations are made
          <xref ref-type="bibr" rid="ref10">(ICG, 2012)</xref>
          , not the reference epoch for the realisation. Thus a full reference for a dataset
collected using GPS single point positioning during 2013 would be WGS84(G1674) Epoch 2013.5.
        </p>
        <p>The dynamic nature of WGS84 is typically ignored by users who fail to account for the WGS84 reference frame
realisation or the epoch of their derived coordinates in their metadata. Indeed it is practically impossible to
rigorously reference WGS84 (and other dynamic datums) in most commonly used software packages. In the case of
WGS84, ignoring the dynamic details does not usually compromise the data as the positional uncertainties
associated with a WGS84 dataset collected via single point positioning are at the metre-level at best.</p>
      </sec>
      <sec id="sec-3-5">
        <title>3.5 The myth of precise WGS84 coordinates</title>
        <p>
          Outside the US military and other authorised users, direct access to sub-metre WGS84 coordinates is almost
impossible. The NGA has published coordinates for only 11 tracking stations worldwide, with one in Australia and
 
 
one in New Zealand
          <xref ref-type="bibr" rid="ref22">(Wong et al., 2012)</xref>
          . The GPS precise ephemeris data is published, which in theory enables the
use of Precise Point Positioning (PPP) to generate centimetre-accurate WGS84 coordinates. In reality though, very
few users have the capability to do the required processing.
        </p>
        <p>Within the geospatial community, therefore, one would expect precise datasets that are referenced to WGS84 to
be exceedingly rare. This is not the case, largely due to misunderstandings about WGS84 and its role in GPS
positioning. Accurate positioning using GPS almost always involves relative pseudorange or carrier phase
positioning to achieve accuracies ranging from centimetres to a metre. In these techniques, some of the stations
occupied have known coordinates, and it is the datum of these coordinates which determines the datum for the
subsequent geospatial dataset. In Australia the datum would typically be GDA94, in New Zealand, NZGD2000.
While many of these techniques do use the broadcast ephemeris during processing, it is not used as a source of
coordinates, so does not determine the datum of the coordinates being generated.</p>
        <p>The mislabelling of precise geospatial datasets as WGS84, when they are not WGS84, can cause problems if the
data epoch is incorrectly assumed. For example, consider the case where a relative positioning dataset is generated
in 2013 from a base station with GDA94 coordinates, but is referenced as WGS84. A future user of the dataset,
knowing it was generated in 2013, might reasonably assume that the reference frame is WGS84(G1674) with an
epoch of 2005.0 (which is the reference epoch for this particular WGS84 frame) or an epoch of 2013.5 (which is the
epoch at which WGS84 coordinates are realised for that year). In fact the epoch for the data is 1994.0, which is
derived from the GDA94 coordinates of the base-station, so a coordinate error of up to 0.8 m (due to the 7 cm/year
tectonic motion of Australia) is immediately introduced.</p>
        <p>A smaller systematic error is caused by the incorrect specification of the reference frame. Using the same
example, the difference between WGS84(G1674) and GDA94 is nearly 0.1m in height. These problems are often
time-consuming and difficult to identify with confidence. Users should be wary if a dataset is purported to be
referenced to WGS84, and positional uncertainties are less than a metre.</p>
        <p>Even the definition of WGS84 as a dynamic datum, while technically correct, is misleading in terms of the way
users access the datum. From the user perspective, it is a series of epoch reference frames, each of which is at the
mid-year epoch as discussed in section 3.4. Thus the ‘dynamic’ WGS84 coordinates derived from point positioning
have up to half a year’s worth of error due to tectonic movement in them. While this is not noticeable to users
accessing WGS84 via single point positioning, it is further reason not to use WGS84 where precise coordinates are
required.</p>
      </sec>
    </sec>
    <sec id="sec-4">
      <title>4 Transformations Between ITRF, WGS84 and National Datums</title>
      <p>The first WGS84 realisation preceded the first ITRF realisation. All subsequent realisations have been aligned to
the ITRF through the use of stations with ITRF coordinates in the realisation of the WGS84 reference frame. The
alignment between WGS84 and ITRF in each instance is sufficiently close that the two are considered identical,
within the uncertainty of the WGS84 reference frame. Table 3 lists the ITRF reference frames to which successive
WGS84 reference frames are aligned.</p>
      <p>WGS84, by definition, tracks a particular realisation of the ITRF, therefore the official transformation
parameters between the national datum and ITRF in each country can be used as a proxy for WGS84 parameters
with careful attention being paid to the epoch of the WGS84 coordinates as previously discussed.</p>
      <sec id="sec-4-1">
        <title>4.1 ITRF/WGS84 transformation parameters for New Zealand</title>
        <p>The parameters in Table 4 should be used to transform from a particular ITRF or WGS84 reference frame to
NZGD2000, which is aligned with ITRF96. To transform between reference frames, the transformation parameters
must first be determined at the epoch of transformation, which in many cases will be the epoch of the coordinates
being transformed. The parameter Tx at time t (in years) is calculated using:
 
 
  = −2000
  , =  +  .Ṫ
(2)</p>
        <p>(1)</p>
        <p>The transformation is then carried out using:
   ,            /   84(3)</p>
        <p>where
cT = 0.001 (millimetres to metres, applies to Tx, Ty and Tz)
cS = 1.0×10-9 (part-per-billion to ratio, applies to S)
cR = π/(180×60×60×1000) = 4.84814×10-9 (milli-arcseconds to radians, applies to Rx, Ry and Rz)</p>
        <p>
          With one exception, these parameters are derived from those published by the IERS
          <xref ref-type="bibr" rid="ref13">(IERS, 2013)</xref>
          . The
transformation parameters between ITRF96 and ITRF97 as calculated by the IGS
          <xref ref-type="bibr" rid="ref20">(Soler and Snay, 2004)</xref>
          were used
in preference to those specified by the IERS. The IERS had determined that no significant transformation existed
between ITRF96 and ITRF97. The calculations by the IGS determined a non-zero transformation, which New
Zealand has adopted since NZGD2000 is based principally on GNSS observations. However, at the time of writing,
New Zealand is reviewing its use of the IGS values, which could lead to a change in the transformation parameters
in Table 4.
        </p>
        <p>Once the transformation has been carried out, the NZGD2000 deformation model would normally be used to
propagate the coordinates to the reference epoch (2000.0).
rates</p>
      </sec>
      <sec id="sec-4-2">
        <title>ITRF89 rates</title>
      </sec>
      <sec id="sec-4-3">
        <title>ITRF88 rates rates</title>
      </sec>
      <sec id="sec-4-4">
        <title>WGS84(Doppler)</title>
      </sec>
      <sec id="sec-4-5">
        <title>4.2 ITRF/WGS84 transformation parameters for Australia</title>
        <p>
          The transformation parameters for Australia have been published in
          <xref ref-type="bibr" rid="ref6">Dawson and Woods (2010)</xref>
          . Note that the signs
of the rotations in Table 5 have been reversed from those published in
          <xref ref-type="bibr" rid="ref6">Dawson and Woods (2010)</xref>
          , so that the
values are consistent with Equation (3).
        </p>
      </sec>
      <sec id="sec-4-6">
        <title>4.3 International Case Studies</title>
        <p>By way of comparison, two international case studies are presented below. The focus is on transformations from
ITRF to the national datum, although using Table 3, transformations to and from the various WGS84 realisations
could be inferred.  </p>
      </sec>
      <sec id="sec-4-7">
        <title>4.3.1 United States</title>
        <p>
          The national datum in the United States is the North American Datum 1983 (NAD83). Like WGS84, this datum
was originally based on TRANSIT Doppler observations and consequently is not strictly geocentric, being offset by
approximately 2 metres
          <xref ref-type="bibr" rid="ref19 ref5">(Soler and Marshall, 2003)</xref>
          . NAD83 has been periodically re-realised to enable the
incorporation of modern observation techniques such as GNSS, with the most recent realisation being
NAD83(2011), which has an epoch of 2010.0
          <xref ref-type="bibr" rid="ref17 ref21">(Pearson and Snay, 2013)</xref>
          .
        </p>
        <p>
          NAD83(2011) is fixed to the North American plate, so that the velocities of stable points are minimised across
the country. For most users, such as those working in central and eastern United States, station velocities in this
plate-fixed frame are negligible. This allows those users to treat NAD83 as a static datum. For regions such as the
western United States and parts of Alaska, the proximity to the plate boundary means that a simple plate motion
model cannot accurately account for the more complex motions present. For these areas, more complex
displacement models, including models which account for earthquakes, are required
          <xref ref-type="bibr" rid="ref17 ref21">(Pearson and Snay, 2013)</xref>
          .
 
 
        </p>
        <p>
          Transformation parameters from ITRF96 to NAD83 were defined jointly by Canada and the United States using
12 Very Long Baseline Interferometry (VLBI) stations with coordinates in each datum. The NUVEL-1A plate
motion model (De Mets et al, 1994) was used to determine the rotations for the North American plate
          <xref ref-type="bibr" rid="ref20">(Soler and
Snay, 2004)</xref>
          . The IGS transformation is used from ITRF96 to ITRF97, but for all subsequent realisations of ITRF,
the transformation parameter values published by the IERS are used. The total transformation from ITRF2008 to
NAD83 is obtained by addition of these individual sets of transformation parameters
          <xref ref-type="bibr" rid="ref17 ref21">(Pearson and Snay, 2013)</xref>
          .
This is identical to the approach currently taken in New Zealand, except that NZGD2000 is by definition aligned to
ITRF96.
        </p>
      </sec>
      <sec id="sec-4-8">
        <title>4.3.2 Great Britain</title>
        <p>
          The national mapping datum for Great Britain is Ordnance Survey Great Britain 1936 (OSGB36). This is a local
datum, with its ellipsoid positioned to best fit the Earth’s surface over the landmass of Great Britain. Consequently,
the fit to the Earth as a whole is relatively poor with the origin of OSGB36 being offset from the geocentre by over
700 metres. For high precision positioning applications, the official datum is the European Terrestrial Reference
Frame 1989 (ETRF89), which is a realisation of the European Terrestrial Reference System 1989 (ETRS89).
ETRF89, along with all subsequent ETRF realisations is fixed to the stable part of the Eurasian plate, in much the
same way as NAD83 is fixed to the North American plate. This enables users to ignore the effects of tectonic plate
motion
          <xref ref-type="bibr" rid="ref12 ref16">(Ordnance Survey, 2013)</xref>
          .
        </p>
        <p>
          To transform from ITRF to OSGB36 requires that the coordinates first be transformed to ETRF89. This is
achieved using the procedure recommended by the IAG Subcommission for the European Reference Frame
(EUREF), as outlined in Boucher and
          <xref ref-type="bibr" rid="ref1">Altamimi (2011)</xref>
          . It involves a two-step procedure. Firstly, IERS-published
published parameters are used to transform from the ITRF realisation of the coordinates to ITRF89. Secondly, three
rotation rates (which account for plate motion) are applied to transform from ITRF89 to ETRF89.
        </p>
        <p>
          Because OSGB36 is based on triangulation, distortions in the network mean it is not possible to transform
coordinates from ETRF89 using a 7-parameter transformation to any better than 5 metres. Therefore, a gridded
displacement model is used for this transformation
          <xref ref-type="bibr" rid="ref12 ref16">(Ordnance Survey, 2013)</xref>
          .
        </p>
      </sec>
      <sec id="sec-4-9">
        <title>4.4 Differing approaches to dynamic datum transformations</title>
        <p>Inspection of Tables 4 and 5 reveals substantial disparities in the numerical values used in Australia and New
Zealand, which cannot be solely attributed to the different versions of ITRF and epochs to which each national
datum aligns. These disparities are mainly due to the different approaches taken by New Zealand and Australia to
define their official transformation parameters.</p>
        <p>The New Zealand parameters keep the process of reference frame transformation quite separate from the process
of coordinate propagation. Propagation of coordinates to or from the reference epoch of 2000.0 is achieved using
the NZGD2000 deformation model.</p>
        <p>
          In contrast, Australia has calculated a localised set of transformation parameters between ITRF and GDA94
which are only applicable on the Australian tectonic plate
          <xref ref-type="bibr" rid="ref18 ref6">(Dawson and Woods, 2010)</xref>
          . Transformation and
propagation are carried out in a single process enabling ITRF/WGS84 data at any epoch to be transformed to
GDA94 using a 14-parameter transformation. Note that a standard 14-parameter transformation assumes the same
data epoch for both the input and output coordinates, but the Australian transformation is quite unique in that the
GDA94 coordinates always refer to 1994.0. A user may validly choose to propagate their ITRF coordinates to
epoch 1994.0 (e.g. using the ITRF2008 plate motion model) before or after the ITRF to GDA94 transformation, but
will notice coordinate differences of up to 20 mm compared to a direct transformation at the current epoch
          <xref ref-type="bibr" rid="ref9">(Haasdyk &amp; Janssen, 2011)</xref>
          .
        </p>
        <p>The Australian continent is extremely stable, with very little relative deformation across its landmass. Thus the
fourteen-parameter transformation is able to accurately incorporate the national-scale plate motion. From the user
perspective, there is no need to utilise a deformation model and some geospatial software packages can handle
fourteen-parameter transformations. Those that cannot perform a 14 parameter transformation usually at least have
the capacity to carry out seven-parameter transformations, giving the user the opportunity to enter the appropriate
seven-parameter values for the epoch at which the transformation is required.</p>
        <p>This approach would not work well in New Zealand. Even at a national scale there is significant relative
deformation that would not be modeled adequately using a simple fourteen-parameter transformation for coordinate
transformation and propagation. Thus it is necessary to separate the processes of coordinate transformation and
propagation. Currently, the lack of support for the deformation model in commercial software makes its use
impractical for many users, who continue to rely on a dense network of passive marks which they can use to
calculate local transformations to account for deformation.</p>
        <p>The case studies of the United States and Great Britain further highlight the variation in transformation
approaches, to reflect local circumstances. While crustal dynamics can be simply handled in Great Britain (as in
Australia), the continued use of a local geodetic datum based on terrestrial measurements means that accurate
 
 
transformations to geocentric datums requires the use of a gridded model. The United States has taken the approach
of satisfying the current desire of most users for a static datum by fixing NAD83 to the North American Plate, while
still providing the necessary means for users in areas of significant deformation to accurately transform coordinates.
Both New Zealand and Australia are investigating how best to modernise their datums so that they continue to
support high accuracy positioning in each country. In Australia’s case a new dynamic datum is proposed, to be
released in approximately 2020. For New Zealand, modernisation may occur within the framework of the existing
datum which already accounts for dynamics, or a new datum may be developed. For both countries, accurately
representing the dynamics of the Earth’s surface will be a key challenge, as will maintaining compatibility with
international systems.</p>
        <p>
          The development of modernised datums will follow established international conventions and utilise accepted
global models, such as those specified in the IERS conventions
          <xref ref-type="bibr" rid="ref18 ref6">(Petit and Luzum, 2010)</xref>
          . This will ensure maximum
consistency with preferred positioning methodologies such as GNSS, which also follow these conventions. As well
as providing consistency, the use of established conventions and models provides a level of traceability to a datum,
which flows to the positions derived.
        </p>
      </sec>
      <sec id="sec-4-10">
        <title>5.1 Option 1: Local 14 parameter transformation, including national-scale tectonics, plus residual deformation model</title>
        <p>This is an enhancement of the approach already implemented for GDA94. Currently GDA94 assumes that the
Australian continent is stable and that coordinates do not change over time.</p>
        <p>This option assumes that any future dynamic datum retains a single reference epoch. In this option, a
14parameter transformation continues to be provided that includes both the reference frame transformation and
propagation between ITRF and GDA, and between the epoch of the dataset and the reference epoch. A gridded
deformation model can then be used to account for the residual deformation, which is not included in the
14parameter transformation. Most users will only need to use the simpler and more widely supported 14-parameter
transformation.</p>
        <p>For New Zealand, such an approach is unlikely to provide a practical solution. Even national-scale deformation
is so complex that the size of the residual deformation would be significant for most geospatial applications. Thus
both the 14-parameters and the deformation model would need to be applied in the majority of cases.</p>
        <p>In Australia, by contrast, the stable tectonic setting means that the residual deformation field will be
insignificant for many applications, although it is noted that in the future, the accuracy demands of many
applications is likely to increase as centimetre-level absolute positioning becomes mainstream. Applications that
only require decimetre-level accuracy could continue to use the 14-parameter transformation, as they do currently.
This option may present the simplest approach for a large proportion of Australian spatial users.</p>
        <p>Disadvantages of this approach for Australia is that it may not be favoured internationally, as a number of
countries are at least partially straddling plate boundaries (although 94% of the Earth's surface lies within the stable
portion of a tectonic plate). In practical terms this may not matter, given that software needs to handle 14-parameter
transformations for global reference frame transformations.</p>
      </sec>
      <sec id="sec-4-11">
        <title>5.2 Option 2: Global 14 parameter transformation, excluding national-scale tectonics, plus deformation model</title>
        <p>This is the approach currently used for NZGD2000.</p>
        <p>The use of global transformation parameters provides the maximum level of consistency with, and traceability
to, global standards and conventions, an important consideration for a national datum, particularly one which aims
to support the use of global positioning technologies.</p>
        <p>
          A future dynamic datum may use all available global ITRF stations in its processing, following the approach
taken by regional reference frames such as the Asia-Pacific Reference Frame (APREF)
          <xref ref-type="bibr" rid="ref8">(Haasdyk et al., 2014)</xref>
          . At
the very least it will include a substantial subset of global stations distributed over a significant proportion of the
globe. If this is the case, then the future national datum is explicitly aligned to a global network of stations.
Logically therefore, a globally determined set of transformation parameters is appropriate.
        </p>
        <p>With this approach, coordinate propagation is handled in totality by a deformation model, maintaining complete
separation between transformation and propagation. The current disadvantage of this approach is that most software
does not have the capacity to incorporate deformation models. This situation is likely to change in the coming years
as the necessity for incorporating deformation models to fully utilise accurate geospatial data is better understood.
 
 </p>
      </sec>
      <sec id="sec-4-12">
        <title>5.3 Option 3: Local 14 parameter transformation, excluding national-scale tectonics, plus deformation model</title>
        <p>
          This is similar to Option 2, the difference being that rather than using a published set of parameters from the IERS,
a local set is calculated using the ITRF stations in each country. The difference from Option 1 is that the 14
parameters are only accounting for the reference frame transformation – tectonic motion is accounted for by the
deformation model. The advantage of this approach is that it enables any regional biases in ITRF to be accounted
for in the transformation, increasing the alignment of the coordinates generated by the transformation with the ITRF
stations in the region. However, the improving precision of successive realisations of the ITRF should make the
calculation of local parameters unnecessary. Any local discrepancies are likely to be due to deformation not fully
accounted for in the ITRF, which is more properly included within a deformation model. An example of such a
local discrepancy is the 4 mm per year average residual rotation rate identified in Australia when comparing the
ITRF plate motion model with the recently released NNR-MORVEL56 model
          <xref ref-type="bibr" rid="ref2">(Altamimi et al, 2012)</xref>
          .
        </p>
        <p>It would still be worth calculating a local set of transformation parameters before making a decision against this
option, to prove that they are not significantly different from the global parameters.</p>
      </sec>
      <sec id="sec-4-13">
        <title>5.4 Option 4: Deformation model only</title>
        <p>
          This option combines propagation and transformation in a variable resolution grid of site velocities and offsets.
          <xref ref-type="bibr" rid="ref21">Stanaway and Roberts (2013)</xref>
          discuss this option in detail. A key advantage of this option is that coordinate
transformation and propagation are combined, yet the full range of non-secular deformation can be included.
Consequently, loss of precision when propagating uncertainty is minimised. If Australia were to define a refined
GDA94, such a model would enable the propagation of these refined GDA94 coordinates with an uncertainty of 6
mm at the 95% confidence level
          <xref ref-type="bibr" rid="ref17 ref21">(Stanaway and Roberts, 2013)</xref>
          .
        </p>
        <p>For New Zealand, this option has similar advantages, albeit that the more complex nature of the country’s
deformation compared with Australia means that sub-centimetre propagation uncertainties are not realistic. Given
that New Zealand already utilises a deformation model, it would not be a major change to amend this model to
incorporate components for reference frame transformation.</p>
        <p>As for the other options involving deformation grids, the biggest disadvantage to this approach at the current
time is the inability of software to support these models.</p>
      </sec>
      <sec id="sec-4-14">
        <title>5.5 Option 5: Reduced parameter sets</title>
        <p>Other options could involve variations in the number of parameters used in a transformation/propagation model. For
example, a three-parameter transformation of three rotations and the reference epoch could be used to propagate
coordinates to the geodetic datum. In this scenario, scale and translations are assumed to be null. With options such
as this, increased simplicity is being traded off against decreased precision. For applications that only require
limited precision, the accuracy provided by simpler options is likely to be perfectly adequate. Once again, this is
particularly relevant for Australia, given its stable tectonic setting.</p>
        <p>One issue with this approach is that it will not provide the precision required for more demanding applications,
such as engineering or geodetic surveying. Therefore, this option would need to be combined with one of the
options discussed above. Having multiple transformation options requires more care from users to record
appropriate metadata, so that any transformation applied can be confidently reversed.</p>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>6 Concluding Remarks</title>
      <p>As it becomes easier to acquire centimetre-accurate geospatial datasets in terms of global reference frames, it is
important that reference frame transformations are handled correctly. For dynamic datums this means that the
propagation of coordinates between epochs must also be carried out in addition to the transformation itself. While
the concept of a dynamic datum may appear new, they are in fact widely used in Australia and New Zealand
already, through the global reference frames WGS84 and ITRF. For WGS84 in particular, reference frame
transformations are not carried out in a rigorous manner. In many cases this does not matter, due to the relatively
high levels of uncertainty present in most WGS84 positions. However, transformation parameters have been
recommended in this paper to enable rigorous transformations where they are required. These transformation
parameters assume the close alignment of WGS84 with the ITRF. With the increasing prominence of multi-GNSS
positioning, users are encouraged to use ITRF as their reference frame in preference to WGS84. ITRF is more
accessible, with all global positioning technologies being aligned to it. In addition, the application of epoch is much
more transparent and easier to understand for ITRF. The differences in the ITRF/WGS84 transformation parameters
between Australia and New Zealand reflect the different approaches taken by each country to transformations
between ITRF and their national datum. These differences are primarily due to the highly stable tectonic setting in
Australia, contrasted to the relatively unstable plate tectonics in New Zealand.
 
 </p>
      <p>Both countries are actively investigating datum modernisation through implementation of a dynamic datum
(Australia) or improvements to the current semi-dynamic datum (New Zealand). Options for dynamic datum
transformations have been considered. There may be advantages to separating transformation from propagation, and
utilising globally-determined transformation parameters. There may also be advantages to using a gridded model to
handle both transformation and propagation of coordinates. However, a solution that might be preferable from a
geodetic perspective may not be the simplest approach for users of the datum. For this reason, Australia will
probably continue to advocate the use of 14-parameter transformations, at least as a transitional measure until
commonly used software can utilise deformation models. The final determination of a preferred method for
dynamic datum transformations will need to be made considering the current state of ITRF and available user tools
at the time a new datum is promulgated.</p>
      <sec id="sec-5-1">
        <title>Acknowledgements</title>
        <p>This work has been supported by the Cooperative Research Centre for Spatial Information, whose activities are
funded by the Australian Commonwealth's Cooperative Research Centres Programme.</p>
        <p>Dr. Chris Pearson, of the University of Otago, contributed to discussions about the most appropriate transformation
parameters to use in New Zealand.
LINZ (2009). Standard for the geospatial accuracy framework – LINZS25005, 21 September 2009
http://www.linz.govt.nz/sites/default/files/document/25005</p>
        <p>Standard%20for%20the%20geospatial%20accuracy%20framework%20-%20LINZS25005_4.pdf
 
 </p>
      </sec>
    </sec>
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