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Sommaire du brevet 2586101 

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(12) Demande de brevet: (11) CA 2586101
(54) Titre français: DISPOSITIF CHRONOMETRIQUE POUVANT DETECTER DES ONDES DE GRAVITE
(54) Titre anglais: TIME MEASURING DEVICE CAPABLE OF DETECTING GRAVITATIONAL WAVES
Statut: Réputée abandonnée et au-delà du délai pour le rétablissement - en attente de la réponse à l’avis de communication rejetée
Données bibliographiques
Abrégés

Abrégé anglais


A device for measuring changes in the flow of time, capable of detecting
gravitational
waves, is disclosed. The device consists of an array of coherent light sources
(such as
lasers) with optical spectrum analyzers located in the center. The lasers are
located as
far away from each other as possible and are connected to the Optical Spectrum
Analyzers through a fiber optic network. The optical spectrum analyzers
continuously
measure the frequency output of each laser and send the results to analogue to
digital
converters. The output of the Analogue to Digital converters is then stored on
a multi--track
storage device for subsequent signal processing.

Revendications

Note : Les revendications sont présentées dans la langue officielle dans laquelle elles ont été soumises.


THE EMBODIMENTS OF THE INVENTION IN WHICH AN EXCLUSIVE PROPERTY
OR PRIVILEGE IS CLAIMED ARE DEFINED AS FOLLOWS:
1. A time-based detector, capable of detecting gravitational waves, in a
network of
components including:
a. An array of ultra-stable coherent light sources (i.e. laser) separated by
large
geographical distances, connected to a fiber optic network.
b. Centrally located Optical Spectrum Analyzers connected to the fiber optic
network configured to measure the frequency fluctuations of each coherent
light source, as stated in claim 1a.
c. Analogue to Digital converters designed to convert the output of each
Optical
Spectrum Analyzer, as stated in claim 1b, into a digital format.
d. Multi-track storage device for storing the digital output streams of the
Analogue to Digital converters.
e. Comparators used to compare the frequency fluctuations of a laser pair,
thereby reducing the chance of false signals created by local disturbances.
f. Computer, with appropriate signal processing software, to analyze the
signals
stored in the device in claim 1d.
1

Description

Note : Les descriptions sont présentées dans la langue officielle dans laquelle elles ont été soumises.


CA 02586101 2007-04-02
SUMMARY OF THE INVENTION:
This invention is a device for measuring minute variations in the flow of time
that can be
used to detect the presence of gravitational waves.
The general theory of relativity predicts that large astronomical bodies in
motion will
cause distortions in the surrounding geometry of space-time, thereby producing
gravitational waves. These gravitational waves will propagate in an outward
direction
and may pass through the earth. There will be a momentary change in the rate
of flow
of time if a gravitational wave passes through the earth. This change in the
flow of time,
at the earth's surface, is predicted by foamy ether theory
(http://www3.telus.net/foamyether/). There are numerous other gravitational
wave
detectors currently in operation, but they are designed to measure changes in
the length
of the device, not changes in the flow of time. For example, the LIGO project
(Laser
Interferometer for Gravitational Waves Observatory) uses lasers to measure
changes in
the length of its two arms. The AURIGA resonant bar detector uses a three
meter long
aluminum cylinder. Sensors are built in to the device to measure changes in
the
dimensions of the cylinder as gravitational waves pass through it.
Although many detectors around the world have been in operation for several
years,
none of them have been successful in detecting gravitational waves. The design
of
interferometer based detectors, such as LIGO, is based on the assumption that
light
travels at a constant velocity. It fails to take into account that as the
gravitational wave
distorts (stretches or compresses) space, the tension on that space is
affected as well,
thereby causing the speed of light to increase or decrease. In other words,
the change
in the speed of light is proportional to the change in the length of the LIGO
detector's
two arms. The wavelength of the laser light also becomes stretched, thereby
causing
the two returning beams of light to always be in phase. This will result in a
failure of
interferometer type devices in detecting gravitational waves.
1

CA 02586101 2007-04-02
The present invention, time-based gravitational wave detector, avoids the
problems
inherent in interferometer and resonant bar detectors by measuring changes in
the rate
of flow of time instead of changes in the length of space.
BRIEF DESCRIPTION OF THE DRAWINGS:
Figure 1 shows a gravitational wave approaching earth, and the inflow of foamy
ether
(or space) around the earth;
Figure 2 is a simplified view of the present invention;
Figure 3 is a more detailed view of the components of the present invention
and how it
can be connected to other external systems;
Figure 4 is a graph that shows how a gravitational wave could affect time
dilation on the
west side of the earth, as displayed in Figure 1;
Figure 5 is a graph that shows how time dilation is affected as the same
gravitational
wave (as shown in Figure 4) passes through the earth. This waveform is
predicted by
foamy ether theory;
Figure 6 is a graph that shows how time dilation is affected as the same
gravitational
wave (as shown in Figure 4) passes through the earth. This waveform is
predicted by
general relativity theory.
DETAILED DESCRIPTION OF THE INVENTION
Figure 1 illustrates the distortions produced in foamy ether as a
gravitational wave
approaches the earth. Arrows indicate the inward flow of ether towards the
planet. As
stated in ether theory, the speed of this ether at the earth's surface is 11.2
km/sec.
Slight variations in the speed of ether will occur as the gravitational wave
passes
2

CA 02586101 2007-04-02
through the earth. This variation in ether flow will manifest itself as
momentary changes
in time dilation at the earth's surface. This time dilation is also explained
in general
relativity theory.
Figure 2 shows a simplified diagram of the invention that can be used to
measure
variations in time dilation caused by a passing gravitational wave. It is
comprised of
three lasers 1,2,3 located in three separate locations, arranged in a roughly
triangular
configuration. These lasers should be separated by as large a geographical
distance as
possible. Fiber optic cables 4 are used to transport the signals from these
lasers to a
central receiver. (Current fiber optics technology is capable of transmitting
a light signal
from distances of up to 120 km).
At the center, an Optical Spectrum Analyzer 5 is set up to measure the
frequency
fluctuations of the three lasers. The frequency shift of the lasers is caused
by a change
in time dilation, which is caused by the incoming gravitational wave varying
the speed of
the inflowing ether. For example, a gravitational wave may cause the flow of
ether to
momentarily increase at laser 1. This would cause an increase in time
dilation, and
consequently decrease the laser's frequency, compared to the other lasers (2
and 3).
The gravitational wave's direction and wavelength can then be determined by
comparing the differences in the shift of frequency of these three lasers.
A more detailed drawing of the gravitational wave detector is shown in Figure
3. The
sensitivity of the gravitational wave detector can be greatly increased by
installing the
lasers in pairs, so that there are three pairs of lasers arranged in a
triangular
configuration. Paired lasers 1,2,3 are located in the same town or vicinity,
but not in the
same building. For example, the laser in building Al is located on the east
side of town
A, and the laser in building A2 is located on the west side of town A. By
placing these
two lasers a small distance apart, the local disturbances, such as doors
slamming,
trucks rolling by, etc., are isolated. An atomic clock 6 could be connected to
each laser
to ensure the laser's frequency remains as constant as possible.
3

CA 02586101 2007-04-02
Each of the six lasers is then connected to fiber optic cables 4 that
terminate on six
Optical Spectrum Analyzers (OSA) 5 located at a Central Hub. The Optical
Spectrum
Analyzers measure the lasers' frequency changes (Af) and feed that into
Analogue to
Digital Converters (A/D) 7. The Analogue to Digital Converters convert the
analogue
frequency fluctuations into a digital format (i.e. Pulse Code Modulation)
which is then
stored on an electronic Multi-track Storage Device 8.
Signals from the three towns (A, B and C) can then be fed into three
comparators 9 to
remove local disturbances. For example, Cmp A will compare the two signals Al
and
A2. Any differences between signals from Al and A2 will be considered local
disturbances and will be discarded. Only signals that are identical between Al
and A2
will pass through Cmp A. This will eliminate random frequency fluctuations
caused by
an individual laser's instability (or environmental effects). The comparators
will only
allow frequency shifts to pass through that are identical within a laser pair,
since any
change in time dilation will affect both lasers in an equal manner. Any
frequency shift
that occurs on only one laser, will be considered an invalid signal. The
central detector
is also affected by time dilation as the gravitational wave passes through it,
but this will
register as identical, simultaneous frequency fluctuations coming from all
three laser
pairs.
The output of the three comparators can now be sent over the intemet for
analysis by a
computer 10, or to a distributed system such as BOINC (Berkeley Open
Infrastructure
for Network Computing). BOINC could analyze the signals in the same manner as
it
does for other gravitational wave detector projects, such as Einstein@Home.
The output data of this invention can also be sent over the internet to the
SETI@HOME
project, which can analyze the data to search for other types of signals.
Figure 4 shows a sample graph of the effects that a gravitational wave could
have on
ether inflow. Normally, the velocity of ether is a steady downward flow of
11.2 km/sec at
the earth's surface. A gravitational wave may momentarily cause the velocity
to increase
to 11.4 km/sec, and then to decease to 11.0 km/sec. This will cause the
laser's
4

CA 02586101 2007-04-02
frequency to decrease and increase respectively. Figure 4 shows a sample
gravitational
wave coming in from the west side of the earth as illustrated in Figure 1.
Since gravitational waves travel at the speed of light, 42.5 msec of time will
elapse
before the wave reaches the opposite side of the earth. Figure 5 illustrates
this. Notice
that the wave is inverted. This inversion is a result of the ether on the east
side of earth
flowing in an opposite direction to ether on the west side. Referring back to
Figure 1,
you can see that the ether is flowing from left to right on the west side of
the earth, and
from right to left on the east side. If the gravitational wave increases the
ether's velocity
on the west side of the earth, it will decrease ether velocity on the east
side. Ether
theory predicts this wave inversion as shown in Figure 5. General relativity
theory,
however, predicts a non-inverted wave as shown in Figure 6.

Dessin représentatif
Une figure unique qui représente un dessin illustrant l'invention.
États administratifs

2024-08-01 : Dans le cadre de la transition vers les Brevets de nouvelle génération (BNG), la base de données sur les brevets canadiens (BDBC) contient désormais un Historique d'événement plus détaillé, qui reproduit le Journal des événements de notre nouvelle solution interne.

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Historique d'événement

Description Date
Demande non rétablie avant l'échéance 2012-10-01
Inactive : Morte - Aucune rép. dem. par.30(2) Règles 2012-10-01
Réputée abandonnée - omission de répondre à un avis sur les taxes pour le maintien en état 2012-04-02
Inactive : Abandon. - Aucune rép dem par.30(2) Règles 2011-09-29
Inactive : Dem. de l'examinateur par.30(2) Règles 2011-03-29
Modification reçue - modification volontaire 2010-11-22
Modification reçue - modification volontaire 2008-01-03
Demande publiée (accessible au public) 2007-09-12
Inactive : Page couverture publiée 2007-09-11
Lettre envoyée 2007-08-16
Inactive : Lettre officielle 2007-07-18
Inactive : CIB en 1re position 2007-07-05
Inactive : CIB attribuée 2007-07-05
Accessibilité au public anticipée demandée 2007-06-15
Exigences pour une requête d'examen - jugée conforme 2007-06-15
Toutes les exigences pour l'examen - jugée conforme 2007-06-15
Requête d'examen reçue 2007-06-15
Demande reçue - nationale ordinaire 2007-05-22
Exigences de dépôt - jugé conforme 2007-05-22
Inactive : Lettre officielle 2007-05-22
Inactive : Certificat de dépôt - Sans RE (Anglais) 2007-05-22
Déclaration du statut de petite entité jugée conforme 2007-04-02

Historique d'abandonnement

Date d'abandonnement Raison Date de rétablissement
2012-04-02

Taxes périodiques

Le dernier paiement a été reçu le 2011-01-31

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Veuillez vous référer à la page web des taxes sur les brevets de l'OPIC pour voir tous les montants actuels des taxes.

Historique des taxes

Type de taxes Anniversaire Échéance Date payée
Taxe pour le dépôt - petite 2007-04-02
Requête d'examen - petite 2007-06-15
TM (demande, 2e anniv.) - petite 02 2009-04-02 2009-03-09
TM (demande, 3e anniv.) - petite 03 2010-04-06 2010-01-21
TM (demande, 4e anniv.) - petite 04 2011-04-04 2011-01-31
Titulaires au dossier

Les titulaires actuels et antérieures au dossier sont affichés en ordre alphabétique.

Titulaires actuels au dossier
PETER C. M. HAHN
Titulaires antérieures au dossier
S.O.
Les propriétaires antérieurs qui ne figurent pas dans la liste des « Propriétaires au dossier » apparaîtront dans d'autres documents au dossier.
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Description du
Document 
Date
(aaaa-mm-jj) 
Nombre de pages   Taille de l'image (Ko) 
Abrégé 2007-04-02 1 18
Description 2007-04-02 5 206
Revendications 2007-04-02 1 26
Dessin représentatif 2007-08-23 1 47
Page couverture 2007-08-30 2 81
Dessins 2008-01-03 3 114
Dessins 2010-11-22 4 159
Dessins 2007-04-02 3 200
Certificat de dépôt (anglais) 2007-05-22 1 158
Accusé de réception de la requête d'examen 2007-08-16 1 177
Avis de rappel: Taxes de maintien 2009-01-05 1 121
Avis de rappel: Taxes de maintien 2010-01-05 1 128
Avis de rappel: Taxes de maintien 2011-01-05 1 122
Avis de rappel: Taxes de maintien 2012-01-04 1 121
Courtoisie - Lettre d'abandon (R30(2)) 2011-12-22 1 165
Courtoisie - Lettre d'abandon (taxe de maintien en état) 2012-05-28 1 173
Deuxième avis de rappel: taxes de maintien 2012-10-03 1 118
Correspondance 2007-05-22 1 60
Correspondance 2007-05-22 1 13
Correspondance 2007-06-15 1 23
Correspondance 2007-07-18 1 16
Correspondance 2007-07-18 1 17
Correspondance 2007-07-24 1 17
Correspondance 2007-08-16 1 85
Correspondance 2009-01-05 1 54
Taxes 2009-03-09 1 229
Correspondance 2010-01-05 1 53
Taxes 2010-01-21 1 25
Correspondance 2011-01-05 1 54
Taxes 2011-01-31 1 199
Correspondance 2011-12-22 1 71
Correspondance 2012-01-04 1 62
Correspondance 2012-05-28 1 97