'T-Phase'
seismic events recorded at EPSO,
Coonabarabran, NSW.
Date |
Time
(UTC) |
Details |
Summary Seismogram |
PSN data file |
2019-10-24 |
08:53:37 |
A ML=5.7 event SW of the South Island of New Zealand generated a T-phase which arrived 22m36s following the origin time of the event, implying a mean propagation speed of 1.61km/s. The frequency spectrum of the vertical component of motion peaked at 1.6Hz. | ||
2019-08-04 |
11:44:19 |
A ML=6.7 event SW of the South Island of New Zealand generated a T-phase which arrived 23m43s following the origin time of the event, implying a mean propagation speed of 1.66km/s. The frequency spectrum of the vertical component of motion peaked at 1.6Hz. | Willmore
(Z) |
psn |
2019-08-04 |
00:11:09 |
A ML=5.6 event SW of the South Island of New Zealand generated a T-phase which arrived 23m43s following the origin time of the event, implying a mean propagation speed of 1.63km/s. The frequency spectrum of the vertical component of motion peaked at 1.6Hz. | Willmore
(Z) |
psn |
2018-11-24 |
23:42:39 |
A ML=5.8
event SW of the South Island of New Zealand
generated a T-phase which arrived 24m39s following the
origin time of the event, implying a mean propagation
speed of 1.56km/s. The frequency spectrum of the
three axes of motion peaked at 1.6-1.8Hz. |
S6000
triaxial BB-13 (Z) |
psn psn |
2018-10-06 |
09:37:15 |
A ML=5.2 event in the ocean nearby Milford Sound generated a T-phase which arrived 22m16s following the origin time of the event, implying a mean propagation speed of 1.64km/s. The frequency spectrum of the three axes of motion peaked at 1.6-2.7Hz. | S6000
triaxial EPSO Array |
psn psn |
2017-09-20 |
01:43:24 |
A ML=6.1 event in the ocean nearby the Auckland Islands generated a T-phase which arrived 25m15s following the origin time of the event, implying a mean propagation speed of 1.61km/s. The frequency spectrum of the three axes of motion peaked at 1.6-1.7Hz. | S6000
triaxial |
psn |
2017-07-11 |
07:00:08 | A ML=6.5
event in the ocean nearby the Auckland Islands
generated a T-phase which arrived 23m49s following the
origin time of the event, implying a mean propagation
speed of 1.64km/s. EPSO's recorded peak horizontal
ground velocity was around 1.4µ/s, which is more than
twice as large as any T-phase motion recorded thus far in
this log. The frequency spectrum of the horizontal
motion peaked at 1.6-2.0Hz, whereas the frequency spectrum
of the vertical component appeared to peak at a slightly
higher frequency of around 2.3Hz. |
VM hor velocity S6000 triaxial EPSO Array |
psn psn psn |
2016-11-13 2016-11-14 2016-11-15 2016-11-18 |
11:32:09 11:52:47 13:21:13 13:31:30 18:59:07 22:19:32 00:34:23 06:47:54 07:21:05 17:30:33 14:22:57 |
Following the M7.9 quake below, there were
numerous large aftershocks located in the north-eastern
region of the South Island of New Zealand, and many of
these quakes transmitted hydroacoustic T-phase waves into
the Tasman Sea. T-phase producing quakes varied in
size between M5.2 to M6.2, and what this earthquake
sequence has demonstrated is that any land based
earthquake occurring in New Zealand's South Island with a
magnitude of ≈5.2 or greater, is likely to generate a
T-phase into the Tasman Sea, which then arrives in south
eastern Australia around 20-25 minutes later. The
psn files shown to the right are all of 30 minutes
duration and have been band-pass filtered between 1-4Hz. |
S6000
triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial S6000 triaxial |
psn psn psn psn psn psn psn psn psn psn psn |
2016-11-13 |
11:03:01 | A Mwp=7.9
earthquake located on the east coast of the South Island
of New Zealand generated a T-phase which arrived
24m56s following the origin time of the quake, giving mean
propagation speed of 1.63km/s. Unusually, this event
occurred on land on the eastern side of
New Zealand (≈140km from the nearest western coast) yet
still generated a large ocean T-phase signal which crossed
the Tasman Sea. The peak spectral amplitude was
around 2.0Hz with a FWHM
of ≈2Hz, which is fairly typical for T-phase events
originating on the ocean floor near New Zealand. The
peak T-phase amplitude was around 0.6µm/s (as recorded by
EPSO Array's SS-1 Ranger geophones) which is more that
twice the amplitude of any ocean-floor-generated T-phase
yet recorded at EPSO. |
VM hor acceln VM hor velocity EPSO Array |
psn psn psn |
2016-07-25 |
19:42:24 |
A ML=5.0
event in the ocean off the West Coast of New Zealand
generated a T-phase which arrived 22m43s following the
origin time of the event, giving mean propagation speed of
1.61km/s. The arrival of this T-Phase was masked by
an earlier M6.5 event located in the Bismark Sea, but the
signal was clear after suitable filtering. The
arrival of the P-Phase at EPSO was buried in the noise. |
S6000
triaxial Willmore (Z) EPSO Array |
psn psn psn |
2016-07-16 |
14:42:40 |
A ML=4.6
event in the ocean NW of the Snares Island generated
a T-phase which arrived 22m26s following the origin time
of the event. A initial P-phase arrived at EPSO
4m33s following the event. The mean propagation
speed of this T-phase was 1.67km/s, which is typical for
events originating in this region. |
S6000
triaxial Willmore (Z) EPSO Array |
psn psn psn |
2016-06-07 |
02:55:21 |
A
Mb=5.5 event offshore New Zealand's Fiordland
generated a T-phase which arrived 22m11s following* the
origin time of the event (*EPSO peak amplitude time for
the T-phase was recorded at 03:17:32). Thus
the mean propagation speed of this T-phase was
1.63km/s. The peak of the T-phase amplitude was
recorded at DNSO*, Sydney with a provisional arrival time
of 03:16:31±10s (*range 331.6km @ 148.9º from EPSO).
Since EPSO's bearing to DNSO (148.9º) is similar to that
of the event (139.9º) then the difference in arrival time
of the T-phase waves between the two stations gives an
indication of the propagation speed of the T-phase signal
over land. In this case ΔEPSO-DNSO is ≈61s implying
a speed over land of ≈5.4km/s. Assuming the transition between hydro-acoustical T-phase waves to seismic waves occurs nearby the coast, and that ocean T-phase waves propagate along straight lines, then the DNSO T-phase arrival time implies a wave propagation speed in ocean of 1852km/1270s = 1.46km/s. 1.5km/s is approximately the speed of sound in seawater. |
S6000
triaxial Willmore (Z) EPSO Array |
psn psn psn |
2016‑01‑14 |
12:15:29 |
A
M5.6 event in the Macquarie Island region generated
a T-phase which arrived 22m37s following* the first
P-phase arrival at EPSO (*peak amplitude time for the
T-phase, at 12:41:15). This event occurred around
100km southward of a very
similar event that occurred on 2015-07-01, making
this one the most southerly T-phase yet recorded at
EPSO. The mean propagation speed of this T-phase was
1.66km/s. |
S6000_triaxial EPSO Array |
psn psn |
2015-10-28 |
13:33:41 |
A M4.6
event off West Coast of South Island, New Zealand,
generated a T-phase with no detectable regular phases
recorded at EPSO. Implied mean propagation speed =
1.6km/s. |
S6000
triaxial EPSO Array |
psn psn |
2015-07-02 |
20:25:09 |
A M5.1 event off West Coast of South Island, New Zealand, generated a T-phase with no detectable regular phases recorded at EPSO. Implied mean propagation speed = 1.6km/s. | S6000
triaxial EPSO Array |
psn psn |
2015-07-01 |
14:30:19 |
The most southerly event to generate a
T-phase yet recorded at EPSO. An
M6.0 event in the Macquarie Island region generated
a T-phase which arrived 20m46s following* the first
P-phase arrival (*peak amplitude time for the T-phase, at
14:56:07). |
S6000
triaxial |
psn |
2015-05-06 |
16:23:54 |
T-phase from a M5.0
earthquake in New Zealand, with the Geonet epicentre
location in the ocean around 50
km NW of Milford Sound. The P-phase arrival at
EPSO was 16:28:23 with first T-phase first arrival at
about 16:44:45, reaching peak amplitude at 16:46:27.
First arrival of the T-phase was around 20m51s following
the quake, implying an average propagation velocity from
the epicentre of around 1.73km/s. |
S6000
triaxial EPSO Array |
psn psn |
2015-05-04 |
02:29:10 |
T-phase from a M5.8
earthquake in New Zealand, with the Geonet epicentre
location around 30
km north-west of Wanaka. The P-phase arrival
at EPSO was 02:33:51 with first T-phase first arrival at
about 02:50:30, which was 21m20s following the quake,
implying an average propagation velocity from the
epicentre of around 1.76km/s. Of particular note
with this event, is that the epicentre was located inland
around 70km from the nearest coastline, at a supposed
depth of 4km. |
VM
hor velocity S6000 triaxial EPSO Array |
psn psn psn |
2015-02-25 | 12:29:55 | Another seismic T-phase from a M4.8
earthquake in New Zealand, with the Geonet epicentre
location around 75km
west of Te Anau. In this case the P-phase
arrival at EPSO was too weak to be detected above the
noise. The T-phase first arrival at EPSO was about
12:51:10, which was 21m15s following the quake, implying
an average propagation velocity from the epicentre of
around 1.7km/s. |
S6000 triaxial EPSO Array |
psn psn |
2014-01-13 | 11:40:01 |
Another seismic T-phase from a M5.5 earthquake in southwest New Zealand, with the Geonet's epicentre location placed around 25km inland from the open ocean. P-arrival at EPSO commenced at 11:44:28 with T-arrival following around 16.8 minutes later at around 12:01:18. As measured by the EPSO Array SS-1 Ranger sensors (vertical) the peak frequency amplitude of the P-waves was ≈1.0Hz and for the T-waves ≈1.6Hz. As is the usual case for T-waves waves arriving from the south-west New Zealand region, the T-waves arrived with greater amplitude than the P-waves, by a factor of around 1.6× in this case. Analysis of the arrival directions of the T- & P-waves by EPSO Array again indicate (within experimental error) identical arrival directions. | EPSO Array | psn |
2014-01-05 |
17:48:41 | Yet another seismic T-phase associated with an earthquake originating from the southern New Zealand region, but this time from an event located inland about 40km from the nearest coast. As with earlier events listed below, analysis of EPSO Array data indicate that the P-phase and T-phase waves arrived at EPSO from almost identical directions. P-arrival at EPSO commenced at 17:53:29 with T-arrival following around 17.6 minutes later at around 18:11:10. As measured by the SS-1 Ranger sensors (vertical) the peak frequency amplitude of the P-waves was 1.0Hz and for the T-waves, 2.4Hz. | VM hor acceln VM hor velocity S6000 triaxial EPSO Array |
psn psn psn psn |
2014-12-12 |
08:02:07 |
Yet another seismic T-phase has arrived
from our local T-phase 'nursery' located SW of the South
Island of New Zealand. USGS reported an event had
occurred at 08:02:07, located at -46.963,
165.832 and although no usual seismic phases were
detected at EPSO, around 22 minutes after the event
(≈08:24:05) an apparent T-wave arrived. A quick
check of the relevant EPSO Array data showed the arrival
direction of these waves was almost identical to the event
recorded on 2014-12-01 described immediately below. |
S6000
triaxial EPSO Array |
psn psn |
2014-12-01 | 13:04:27 | A seismic T-phase from an undersea
earthquake located in the Auckland
Islands Region of New Zealand. This T-phase
event was very similar to another which occurred in the
same area on 2013-12-16 (see below),
but this latest event was recorded by EPSO
Array and apparent arrival angles of various
earthquake waves may now be estimated. There has
been some speculation that the T-waves may preferentially
originate from particularly steep sections of the
Australian continental shelf, where the ocean sound waves
are more efficiently converted to a seismic P-wave in the
crust. Thus T-waves may arrive in somewhat different
directions from the usual P and S phases. However,
for this particular event the P-phase and T-phase had
identical apparent arrival directions, suggesting that the
conversion from ocean-acoustic to seismic-P occurred at
the coast somewhere along the great circle track between
EPSO and the earthquake. Inspection of an undersea
map of this coastal area shows that the continental
shelf is relatively steep and oriented approximately
perpendicular to the earthquake's great circle track, so
it is perhaps not so surprising that the P and T waves
recorded by EPSO Array had very similar arrival
directions. |
VM hor acceln VM hor velocity S6000 triaxial EPSO Array |
psn psn psn psn |
2013-12-16 |
12:07:27 |
A Mb=5.3 earthquake located
off the West Coast of the South Island of New Zealand
generated a conspicuous T-wave, with the T-wave arriving
at EPSO around 16.3 minutes following the initial P-Wave
(a very similar event occurred at 2012-03-14 19:07:44UTC -
see
below for details). For the first time such an
event was also captured by the EPSO Array and served as a
good system test. The initial deep Earth P-waves
from this event passed the EPSO Array with an apparent
horizontal velocity of ≈13km/s, implying that the true
wave fronts impacted the array from the deep Earth with an
inclination angle of ≈60º with respect to the EPSO Array
ground surface. The later T-wave originated
somewhere near the Australian continental shelf, at a
distance of ≈400km. The T-wave passed over the EPSO
Array with an apparent horizontal velocity of ≈8km/s,
implying that the true wave front had an inclination angle
of around 40º, as one might expect from a much closer
event. |
VM
hor acceln S6000 triaxial SS-1 vertical EPSO Array |
psn psn psn psn |
2012-03-14 |
19:07:44 |
A relatively small quake
off the Off W Coast of
South Island, New Zealand, appears to have generated
a conspicuous T-wave,
where acoustical water waves have been generated on the
sea floor by the earthquake, and propagated until they
encountered Australia's continental shelf, where some of
the acoustical energy was converted back to seismic
waves. The Great Circle distance from EPSO to this
earthquake's epicentre is ≈2174km. The
distance from EPSO to the edge of the Australian
continental shelf (on the direct EPSO-earthquake track) is
about 380km. From this
location, a seismic P-wave takes around 54 seconds
to travel to EPSO. By analysing the seismic traces
(see right), the delay between the earthquake's origin
time (19:07:44) and shaking commencing at EPSO (19:28:44)
resulting from the T-wave arrival, is around 1260
seconds. Assuming this shaking was due to T-waves
traveling via the direct Great Circle track and impacting
the Australian continental shelf offshore from Sydney,
these waves were propagating in the ocean for 1260-54=1206
seconds and covered 2174-380=1794km. In this case
the derived speed of the T-waves is 1206/926=1.3km/s in
the ocean. But if the T-waves impacted the
Australian continental shelf at the closest point to the
epicentre (i.e. eastern
Tasmania, 1480km distant from the epicentre, and
1280km from EPSO), from this location a seismic P-wave
would take around 167 seconds to travel to EPSO. So
via this route, the T-waves would have propagated for
1480km for 1206-167=813 seconds, suggesting a T-wave
propagation velocity of 1.8km/s. Therefore the ocean
T-wave propagation speed is in the range
1.3-1.8km/s. The average of these two limits is
around 1.5km/s which is approximately the speed
of sound in seawater, and is consistent with the
propagation of the T-waves waves via the so called SOFAR
channel. Most of the spectral energy in the
T-wave induced shaking observed at EPSO, is contained
within the 1.5-2.6Hz spectral band. |
S6000 SS-1 vertical |
psn psn |