Abstract:
A system, method and device may be used to monitor conditions in a borehole. Energy is transmitted to a pulse generator located proximate a position to be interrogated with a sensor. The pulse generator stores the energy, then releases it in a pulse of electromagnetic energy, providing the energy to resonant circuits that incorporate the sensors. The resonant circuits modulate the electromagnetic energy and transmit the modulated energy so that it may be received and processed in order to obtain the desired measurements.

Description:
RELATED APPLICATION 
     This application claims priority to U.S. Provisional Patent Application No. 60/842,936, filed Sep. 8, 2006, which is incorporated herein by reference in its entirety. 
    
    
     BACKGROUND 
     1. Field 
     The present invention relates generally to remote sensing and more particularly to passively communicating remote conditions by modulated reflectivity. 
     2. Background 
     In resource recovery, it may be useful to monitor various conditions at locations remote from an observer. In particular, it may be useful to provide for monitoring conditions at or near to the bottom of a borehole that has been drilled either for exploratory or production purposes. Because such boreholes may extend several miles, it is not always practical to provide wired communications systems for such monitoring. 
     U.S. Pat. No. 6,766,141 (Briles et al) discloses a system for remote down-hole well telemetry. The telemetry communication is used for oil well monitoring and recording instruments located in a vicinity of a bottom of a gas or oil recovery pipe. Modulated reflectance is described for monitoring down-hole conditions. 
     As described in U.S. Pat. No. 6,766,141, a radio frequency (RF) generator/receiver base station communicates electrically with the pipe. The RF frequency is described as an electromagnetic radiation between 3 Hz and 30 GHz. A down-hole electronics module having a reflecting antenna receives a radiated carrier signal from the RF generator/receiver. An antenna on the electronics module can have a parabolic or other focusing shape. The radiated carrier signal is then reflected in a modulated manner, the modulation being responsive to measurements performed by the electronics module. The reflected, modulated signal is transmitted by the pipe to the surface of the well where it can be detected by the RF generator/receiver. 
     SUMMARY 
     An aspect of an embodiment of the present invention includes an apparatus for sensing a characteristic of a borehole. The apparatus includes a transmission line, constructed and arranged to transmit an electromagnetic signal within the borehole, and a probe, positionable at a location within the borehole at which the borehole characteristic is to be sensed, and at which energy propagated via the transmission line may be received. The probe includes an energy storing circuit element, configured to receive and store energy transmitted through the transmission line, a pulse generator, configured to receive stored energy from the energy storing circuit element and to discharge the energy to generate a pulse of electromagnetic energy, a resonant circuit portion that is configured and arranged to receive energy from the pulse of electromagnetic energy and produce a modulated electromagnetic signal representative of the borehole characteristic, and a coupler, configured to couple the modulated electromagnetic signal to the transmission line and to transmit a signal representative of the modulated electromagnetic signal via the transmission line. 
     An aspect of an embodiment of the present invention includes an apparatus for sensing a characteristic of a borehole, that is positionable at a location within the borehole at which the borehole characteristic is to be sensed, and at which electromagnetic energy propagated along the borehole may be received. The apparatus includes an energy storing circuit element, configured to receive and store the electromagnetic energy, a pulse generator, configured to receive stored energy from the energy storing circuit element and to discharge the energy to generate a pulse of electromagnetic energy, a resonant circuit portion that is configured and arranged to receive energy from the pulse of electromagnetic energy and produce for analysis a modulated electromagnetic signal representative of the borehole characteristic. 
     An aspect of an embodiment of the present invention includes a method for sensing a characteristic of a borehole, that includes receiving electromagnetic energy proximate a location within the borehole at which the borehole characteristic is to be sensed, storing the received electromagnetic energy, then discharging the stored energy to generate an electromagnetic pulse within the borehole, receiving energy from the electromagnetic pulse in a resonant circuit to produce an electrical signal in the resonant circuit, modulating the electrical signal to produce a modulated electromagnetic signal representative of the borehole characteristic, and transmitting the modulated electromagnetic signal for analysis. 
     An aspect of an embodiment of the present invention includes a system for monitoring a characteristic of a borehole, including a transmitter configured and arranged to transmit an electromagnetic signal into the borehole, a transmission line constructed and arranged to guide propagation of the electromagnetic signal within the borehole, a probe, positionable at a location within the borehole at which the borehole characteristic is to be sensed, and at which energy propagated via the transmission line may be received, the probe portion including an energy storing circuit element, configured to receive and store energy transmitted through the transmission line, a spark generator, configured to receive stored energy from the energy storing circuit element and having electrodes separated by a gap, the spark generator being further configured and arranged such that when a voltage across the gap exceeds a breakdown voltage of a medium in which the probe is located, a spark discharge between the electrodes generates an electromagnetic pulse, a resonant circuit portion that is configured and arranged to receive energy from the electromagnetic pulse and produce a modulated electromagnetic signal representative of the borehole characteristic, a coupler portion, configured to receive the modulated electrical signal and to transmit a radio frequency signal representative of the modulated electromagnetic signal via the transmission line, a receiver, configured and arranged to receive the radio frequency signal representative of the modulated electrical signal and to output an electrical signal representative of the received radio frequency signal, and a processor, configured and arranged to accept as an input the electrical signal output by the receiver and to process the received electrical signal to determine information relating to the monitored characteristic. 
    
    
     
       DESCRIPTION OF THE DRAWINGS 
       Other features described herein will be more readily apparent to those skilled in the art when reading the following detailed description in connection with the accompanying drawings, wherein: 
         FIGS. 1A-1D  show an embodiment of an apparatus for sensing a characteristic of a borehole; 
         FIG. 2A  shows an embodiment of a resonant cavity for use in an embodiment of the apparatus illustrated in  FIG. 1 ; 
         FIG. 2B  shows an example of a resonant network device formed as a magnetically coupled electrically resonant mechanical structure for performing electrical resonance; 
         FIG. 2C  illustrates an alternate example of a wellhead connection; 
         FIG. 3  shows a bottom view of an embodiment of a resonant cavity; 
         FIG. 4  shows an alternate embodiment of a resonant cavity; 
         FIG. 5  shows an embodiment of a circuit for detecting a characteristic; 
         FIG. 6  schematically illustrates an embodiment of a method for sensing a characteristic of a borehole; and 
         FIG. 7  is an example of a pulse generator in accordance with embodiments of the present invention. 
     
    
    
     DETAILED DESCRIPTION 
       FIG. 1  illustrates an example of an apparatus  100  for sensing a characteristic of a borehole. The borehole can be any cavity, configured with any orientation, having a characteristic such as a material composition, temperature, pressure, flow rate, or other characteristic, which can vary along a length of the borehole. 
     The apparatus  100  includes an electromagnetically transmissive medium, such as a conductive pipe  102 , for conducting electromagnetic energy through the borehole. An input  104 , coupled (e.g., connected) to the conductive pipe  102 , is provided for applying electromagnetic energy to the conductive pipe. In embodiments, the electromagnetic energy can be of any desired frequency selected, for example, as a function of characteristics to be measured within the borehole and as a function of the length and size of the borehole. 
     The inlet includes a connector  106  coupled with the conductive pipe  102 . The connector  106  can be formed, for example, as a coaxial connector having a first (e.g., interior) conductor coupled electrically to the conductive pipe  102 , and having a second (e.g., exterior) conductive casing coupled to a hollow borehole casing  111 . An insulator, for example, a PTFE or nylon material, may be used to separate the interior conductor from the exterior conductive casing. 
     The inlet can include an inductive isolator, such as a ferrite inductor  108  or other inductor or component, for electrically isolating the inlet from a first potential (e.g., a potential, such as a common ground, of the return current path of the borehole casing  111 ) at a location in a vicinity of the input  104 . The apparatus  100  can include a source of electromagnetic energy, such as a signal generator  105 , coupled to the inlet for generating the electromagnetic energy to be applied to the conductive pipe or other type of transmission line. The signal generator  105  may be configured to produce a pulsed or a continuous wave signal, as necessary or desirable. 
     The hollow borehole casing  111  can be placed into the borehole whose characteristics are to be monitored. The hollow borehole casing  111  can, for example, be configured of steel or other suitable material. In a typical drilling application, the borehole casing  111  may be a standard casing used to provide structural support to the borehole in ordinary drilling applications and it is not necessary to provide any additional outer conductive medium. 
     The conductive pipe  102  can be located within, and electrically isolated from, the hollow borehole casing using spacers  116 . The spacers can, for example, be configured as insulated centralizers which maintain a separation distance of the conductive pipe  102  from the inner walls of the hollow borehole casing  111 . These insulating spacers can be configured as disks formed from any suitable material including, but not limited to nylon or PTFE. As will be appreciated, the conductive pipe  102  in conjunction with the casing  111  together form a coaxial transmission line. Likewise, it is contemplated that alternate embodiments of a transmission line may be employed, such as a single conductive line, paired conductive lines, or a waveguide. For example, the casing alone may act as a waveguide for certain frequencies of electromagnetic waves. Furthermore, lengths of coaxial cable may be used in all or part of the line. Such coaxial cable may be particularly useful when dielectric fluid cannot be used within the casing  111  (e.g., when saline water or other conductive fluid is present in the casing  111 ). 
     The apparatus  100  includes a pulse generator  109 , for generating an electrical pulse to be transmitted through the conductive pipe  102 . Alternatively, the pulse generator can generate an electromagnetic pulse that is transmitted through the ground to an above ground antenna. The pulse generator may be attached to or otherwise magnetically coupled to the conductive pipe  102 . The pulse generator  109  may be any device including, but not limited to, an electronic structure for receiving electromagnetic energy and generating a resonant signal therefrom. An exemplary embodiment of the pulse generator  109  is schematically illustrated in  FIG. 5  and more particularly illustrated in  FIG. 7 . As shown in  FIG. 2B , the pulse generator  109  may be stacked along with the resonant network devices  120  described below. 
     As schematically illustrated in  FIG. 5 , the pulse generator  109  may include a component such as a power absorber  110 , for storing the electromagnetic energy transmitted through the conductive pipe  102 . The power absorber  110  stores the electrical pulse in capacitors, batteries or other electrical energy storage devices. 
     The power absorber  110  also may include a converter, such as a rectifier  112 , for converting the electrical pulse into constant power or direct current energy. The rectifier  112  provides the direct current energy on its output to the electrical energy storage device  114 . 
     The pulse generator  109  may also include a pulse generator such as a spark gap  118  for generating an electromagnetic pulse using the energy stored in the electrical energy storage device  114 . Those of ordinary skill in the art will appreciate that the spark gap  118  may be formed between two electrodes that are housed in a glass enclosure, which may be filled with an inert gas. As the energy stored in the electrical storage device  114  increases, the breakdown potential of the spark gap also increases when the breakdown potential reaches its limit an arc of energy is generated across the spark gap  118 . In the case that the electrodes are partially consumed by the process of spark generation, it may be useful to include a feed mechanism that feeds additional electrode material into the spark generation region. For example, lengths of conductive wire may serve as the electrodes and may be continuously or intermittently fed into the enclosure in order to replenish the electrodes over time. 
     The pulse generator  109  includes reactive components, such as a resonant network device  120  responsive to the pulse of the spark gap  118 , for resonating at a frequency which is modulated as a function of a characteristic of the borehole. The resonant circuit  118  may include a resonator L/C circuit composed of inductive and capacitive elements that are configured and arranged to produce a ringing output. The resonant network device  120  can be, for example, any electro-acoustic or other device including, but not limited to any magnetically coupled electrically resonant mechanical structure for performing an electrical resonance, such as the resonant cavity of  FIG. 2A , the tank circuit of  FIG. 2B , or any other suitable device. The resonant network device  120  can be connected with or mechanically coupled to the conductive pipe  102 . In an embodiment, the resonant network device  120  may include an inductor formed with a toroidal core and magnetically coupled to the conductive pipe  102 . The toroidal core is a magnetic core formed as a medium by which a magnetic field can be contained and/or enhanced. For example, the resonant network device  120  can be a single turn coil with a one inch cross-section wrapped around a ferrite core, or any other suitable device of any suitable shape, size and configuration can be used. 
     The ringing signal generated by the resonant network device includes information of interest because it is modulated by changes in either the capacitor, inductor or both, which thus act as the sensors. For example, the frequency of the ringing is determined by the shifts in the L/C circuit&#39;s value of capacitance and/or inductance. Note this frequency is chosen so as not to be at the same frequency of the input charging frequency (which is typically 300 kHz) so as to not confuse data interpretation. By way of example, the capacitor of the L/C circuit may be configured as a capacitive pressure sensor, in which distance between plates of the capacitor is reduced as pressure is increased, and vice versa. Likewise, inductive displacement sensors may be used, where inductance changes with motion of a permeable core in accordance with changes in pressure in a volume, or strains in a structure. 
     The intensity of the signal&#39;s energy is such that much energy can be transmitted through the ground itself. The interaction of the signal with the surrounding formation can yield important information about the formation itself. Indeed, the signal can be received by separate above ground surface antennas away from the well site and the signal interpreted by various methods. Shifts in the signal&#39;s frequency, attenuation, delays and echo effects may give valuable underground information. 
     Those skilled in the art will appreciate that a magnetic core is a material significantly affected by a magnetic field in its region, due to the orientable dipoles within its molecular structure. Such a material can confine and/or intensify an applied magnetic field due to its low magnetic reluctance. The wellhead ferrite inductance  108  can provide a compact inductive impedance in a range of, for example, 90-110 ohms reactive between an inlet feed point on the pipe and a wellhead flange short. This impedance, in parallel with an exemplary 47 ohm characteristic impedance of the pipe-casing transmission line can reduce the transmitted and received signals by, for example, about ˜3 dbV at the inlet feed point for a typical band center at 50 MHz. The magnetic permeability of the ferrite cores can range from ˜20 to slightly over 100, or lesser or greater. As such, for a given inductance of an air-core inductor, when the core material is inserted, the natural inductance can be multiplied by about these same factors. Selected core materials can be used for the frequency range of, for example, 10-100 MHz, or lesser or greater. 
     The resonant network device  120  receives energy from the spark gap  118 , and “rings” at its natural frequency. A sensor can include a transducer provided in operative communication with the resonant network device  120 , and coupled (e.g., capacitively or magnetically coupled) with a known potential (e.g., a common ground). The transducer may be configured to sense a characteristic associated with the borehole, and to modulate the vibration frequency induced in the resonant network device  120  when electromagnetic energy is transmitted through the conductive pipe  102  and an energy pulse is received from the spark gap  118 . The modulated vibration frequency can be processed to provide a measure of the borehole characteristic. That is, the vibration frequency induced by the pulse is modulated by a sensed characteristic of the borehole, and this modulation of the vibration can be processed to provide a measure of the characteristic. 
     A sensor can include, or be associated with, a processor (e.g., the CPU or the CPU and associated electronics of computer  121 ). The processor  121  can provide a signal representing the characteristic to be measured or monitored. 
     The processor  121  can be programmed to process the modulated vibration frequency to provide a measure of the sensed characteristic. The measurement can, for example, be displayed to a user via a graphical user interface (GUI)  123 . The processor  121  can perform any desired processing of the detected signal including, but not limited to, a statistical (e.g., Fourier) analysis of the modulated vibration frequency, a deconvolution of the signal, a correlation with another signal or the like. Commercial products are readily available and known to those skilled in the art can be to perform any suitable frequency detection. For example, a fast Fourier transform that can be implemented by, for example, MATHCAD available from Mathsoft Engineering &amp; Education, Inc. or other suitable product to deconvolve the modulated ring received from the resonant network device. The processor can be used in conjunction with a look-up table having a correlation table of modulation frequency-to sensed characteristics (e.g., temperature, pressure, and so forth) conversions. 
     In an embodiment, at least a portion of the hollow borehole casing  111  is at a first potential (e.g., common ground). For example, the hollow borehole casing can be at a common ground potential at both a location in a vicinity of the inlet  104 , and at a location in a vicinity of the pulse generator  109 . The grounding of the hollow borehole casing in a vicinity of the inlet is optional, and may help to establish a known impedance for the conductive pipe. The grounding of the hollow borehole casing in a vicinity of the pulse generator  109  may allow the resonant length to be defined. That is, the resonant cavity has a length within the hollow borehole casing defined by the distance between toroidal coil  112  and by the ground connection at a second, lower end of the resonant cavity. 
     The transducer of the resonant network device  120  of the pulse generator  109  can be configured to include passive electrical components, such as inductors and/or capacitors, such that no down-hole power is needed. Alternately, power may be stored in batteries or capacitors for use in powering active components. During an assembly of the  FIG. 1  apparatus  100 , the conductive pipe can be assembled in sections, and a spacer can be included at each joint between the various pipe sections to ensure stability. Prior to placing the conductive pipe  102  and the pulse generator  109  into a borehole, a transducer used for sensing the modulated vibration frequency can be calibrated using the GUI  123  and processor  121 . 
     Details of the embodiment illustrated in  FIG. 1A  will be described further with respect to  FIG. 1B , which shows an example of a telemetry component of the apparatus. 
     As shown in  FIG. 1B , the conductive pipe  102  and hollow borehole casing  111  are electrically isolated from one another via the ferrite inductance  108 . Where the resonant network device is a natural resonator, the wavelength of the resonant “ring” frequency can dictate the size (e.g., length) of the device. Those skilled in the art will appreciate that the size constraint can be influenced (e.g., reduced) by “loading” the device with inductance and/or capacitance. For example, the amount of ferrite used in an particular implementation can be selected as a function of desired frequency and size considerations. 
     An instrumentation signal port  112  may be provided for receiving the probe  106 . A wellhead configuration, a depicted in  FIG. 1B , is short circuited to the hollow borehole casing. The ferrite inductor  108  thus isolates the conductive probe of the inlet, which is coupled with the conductive pipe  102 , from the top of the wellhead which, in an embodiment, is at a common ground potential. In an exemplary embodiment, because the wellhead is grounded via short circuiting of the wellhead flange  124  to common ground, the ferrite inductor isolates the short circuited wellhead flange from the conductive pipe used to convey a pulse from the probe to the resonant cavity. 
     As noted above, the conductive pipe  102 , along with the casing  111 , form a coaxial line that serves as a transmission line for communication of the down-hole electronics, such as the transducer, with the surface electronics, such as the processor. 
       FIG. 1C  illustrates an electrical representation of the resonant cavity and transducer included therein. In  FIG. 1C , the toroidal core  125  is represented as an inductor section configured of ferrite material for connecting the conductive pipe  102  with the resonant cavity  120 . As can be seen in  FIG. 1C , for a resonant network device configured as a resonant cavity, an upper portion  132  of the resonant cavity  120  coincides with a lower section of the toroidal core  125  and can be at an impedance which, in an exemplary embodiment, is relatively high as compared to the impedance between conductive pipe  102  and the casing  111 . For example, the impedance at the top of the resonant cavity can be on the order of 2000 ohms, or lesser or greater. For magnetic core based, magnetically coupled resonant networks, those measures may have little or no relevance. 
     This relatively large differential impedance at the top of the resonant cavity relative to the conductive pipe above the resonant cavity provides, at least in part, an ability of the cavity to resonate, or “ring” in response to the pulse and thereby provide a high degree of sensitivity in measuring a characteristic of interest. In addition, the ability of the transducer to provide a relatively high degree of sensitivity is aided by the placing a lower end of the resonant cavity at the common ground potential. 
     The  FIG. 1C  electrical representation of the resonant network device, for a coaxial cavity formed by the conductive pipe and the borehole casing, includes a representation of the resonant network resistance  128  and the resonant network inductance  130 . A lower portion of the cavity defined by the common ground connection  114  is illustrated in  FIG. 1C , such that the cavity is defined by the bottom of the toroidal core  112  and the ground connection  114 . A capacitance of the sleeve associated with the resonant cavity is represented as a sleeve capacitance  134 . 
     The transducer associated with the resonant cavity for modulating the vibration frequency induced by the pulse, as acted upon by the characteristic to be measured, is represented as a transducer  136 . 
     For a resonant cavity configuration, the bottom of the resonant capacity can include a packer seal, to prevent the conductive pipe  102  from touching the hollow borehole casing  111 . The packer  138 , as illustrated in  FIG. 1C  and in  FIG. 1A , may include exposed conductors  140  which can interface with conductive portions of the resonant cavity and the hollow borehole casing  111  to achieve the common ground connection  114  at a lower end of the resonant cavity. 
       FIG. 1D  illustrates another detail of the well telemetry component included at an upper end of the conductive pipe  102 . In  FIG. 1D , a connection of the probe  106  to the conductive pipe  102  is illustrated as passing through the hollow borehole casing  111 , in the inlet  104 .  FIG. 1D  shows that the probe  106  is isolated from the short circuited wellhead flange  124  via the ferrite inductor  108 . 
       FIG. 2A  shows an example of a detail of a resonant network device  120  formed as a resonant cavity. In  FIG. 2A , the hollow borehole casing  111  can be seen to house the conductive pipe  102 . The toroidal core  112  is illustrated, a bottom of which, in the direction going downward into the borehole, constitutes an upper end of the resonant cavity. The transducer  136  is illustrated as being located within a portion of the resonant cavity, and is associated with a conductive sensor sleeve  202 , the capacitance of which is represented in  FIG. 1C  as the sleeve capacitance  134 . 
     The ferrite toroidal core  112  can be configured as toroidal core slipped into a plastic end piece. Such ferrite materials are readily available, such as cores available from Fair-Rite Incorporated, configured as a low μ, radio frequency type material, or any other suitable material. Mounting screws  204  are illustrated, and can be used to maintain the sensor sleeve and transducer in place at a location along a length of the conductive pipe  102 . A bottom of the resonant cavity, which coincides with a common ground connection of the packer to the hollow borehole casing, is not shown in  FIG. 2 . 
       FIG. 2B  illustrates an exemplary detail of a resonant network  120  formed as a tank circuit. In  FIG. 2B , multiple resonant network devices  206  associated with multiple sensor packages can be included at or near the packer. In the  FIG. 2B  embodiment, resonators using capacitive sensors and ferrite coupling transformers are provided. Again, the hollow borehole  111  can be seen to house the conductive pipe  102 . Each resonant network device may be configured as a toroidal core  208  having an associated coil resonator  210 . No significant impedance matching, or pipe-casing shorting modifications, to an existing well string need be implemented. The coaxial string structure can carry current directly to a short at the packer using the ferrite toroid resonators as illustrated in  FIG. 2B , without a matching section as with the resonant cavity configuration. 
     In an electrical schematic representation, the conductive pipe can be effectively represented as a single turn winding  214  in the transformer construct, and several secondary windings  216  can be stacked on the single primary current path. The quality of the packer short is of little or no significance. Metal-toothed packers can alternatively be used. The return signal using this transformer method can be detected, without using a low packer shorting impedance. 
     In the embodiment of  FIG. 2B , spacing between multiple resonant network devices  206  can be selected as a function of the desired application. The resonant network devices  206  can be separated sufficiently to mitigate or eliminate mechanical constraints. In addition, separation can be selected to mitigate or eliminate coupling between the devices  206 . 
     In an embodiment, a distance of one width of a ring can decrease coupling for typical applications. The inductance and/or capacitance of each resonant network device can be modified by adding coil turns, and the number of turns can be selected as a function of the application. For example, the number of turns will, in part, set a ring frequency of each resonant network device. Particular embodiments can be on the order of 3 to 30 turns, or lesser or greater. 
     In particular embodiments, the frequency used for the resonant network devices can be on the order of 3 MHz to 100 MHz or lesser or greater, as desired. The frequency can be selected as a function of the material characteristics of the conductive pipe (e.g., steel). Skin depth can limit use of high frequencies above a certain point, and a lower end of the available frequency range can be selected as a function of the simplification of the resonant network device construction. However, if too low a frequency is selected, decoupling from the wellhead connection short should be considered. 
     Thus, use of ferrite magnetic materials can simplify the downhole resonant network devices mechanically, and can allow less alterations to conventional well components. Use of a ferrite magnetic toroid can permit magnetic material to enhance the magnetic field, and thus the inductance, in the current path in very localized compact regions. Thus, stacking of multiple resonant network devices at a remote site down the borehole can be achieved with minimal interaction among the multiple devices. The multiple sensor devices can be included to sense multiple characteristics. The use of a ferrite magnetic toroid can also be used to achieve relatively short isolation distances at the wellhead connection for coupling signal cables to the conductive pipe  102  as shown in  FIG. 2C . 
       FIG. 2C  illustrates an embodiment of a wellhead connection, wherein a spool  218  is provided to accommodate the ferrite isolator and signal connections. A spool can, for example, be on the order of 8 to 12 inches tall, or any other suitable size to accommodate the specific application. The spool is used for signal connection to the pipe string. 
     The resonant network device configured of a “toroidal spool” can be separated and operated substantially independently of sensor packages which are similarly configured and placed in a vicinity of the spool  218 . An increased inductance in a width of the toroid spool can be used to isolate the signal feed point at the wellhead connection. As is represented in  FIG. 2C , current on the pipe surface will induce magnetic fields within the ferrite toroid for inductive enhancement of the pipe current path. 
       FIG. 3  illustrates a view of the  FIGS. 2A and 2B  devices from a bottom of the borehole looking upward in  FIG. 2 . In  FIG. 3 , the transducer  136  can be seen to be connected via, for example, electrical wires  302  to both the sensor sleeve  202  and the conductive pipe  102 . The sensor sleeve in turn, is capacitively coupled to the hollow borehole casing  111  via the sleeve capacitance  134 . 
       FIG. 4  illustrates an embodiment wherein the packer has been modified to include a conduit extension  402  into a zone of interest where the characteristic of the borehole is to be measured. This extension  402  can, in an exemplary embodiment, be a direct port for sensing, for example, a pressure or temperature using an intermediate fluid to the sensor. 
     In particular embodiments, transducers, such as capacitive transducers, are mounted near the top of the resonant cavity as an electrical element of the sensor sleeve. Remote parameters can be brought to the sensor in the resonant cavity via a conduit that passes through and into a sealed sensing unit. The measurement of a desired parameter can then be remotely monitored. The monitoring can further be extended using a mechanical mechanism from the sensor to relocate the sensor within the resonant cavity at different locations along the length of the conductive pipe  102 . In  FIG. 4 , a sensor conduit  404  is provided to a pressure or temperature zone to be monitored. 
       FIG. 6  is a block diagram of a method of telemetry data gathering using the apparatus  100 , the sequence of which will be explained with reference to the embodiment of the pulse generator  109  illustrated in  FIG. 7 . At  600 , electromagnetic energy, for example in the form of radio frequency radiation, is received by the pulse generator  109 . In an example, the electromagnetic energy may be input at a frequency of 300 kHz, however, those of ordinary skill in the art will appreciate that a wide range of frequencies may be used. 
     As illustrated in  FIG. 7 , a multi-wound inductor  702  based on a low frequency ferrite core accepts the input energy from the electromagnetic energy, and produces a current within the components of the pulse generator  109 . Optionally, the current is rectified  602  using rectifier  112  (schematically illustrated in  FIG. 5 ). 
     At  604 , the energy is used to charge a storage device, which in  FIG. 7  is a capacitor  704 . Those skilled in the art will appreciate that the electrical energy storage device may be a capacitor, battery, or other suitable storage device, and the rectifier may be a diode (e.g., diode  706  as shown in  FIG. 7 ). 
     Upon sufficient charging (i.e., upon reaching a threshold, which may be a charge threshold or a voltage threshold, for example) of the energy storage device, an energy pulse is generated ( 606 ) between the electrodes (not illustrated) in the spark gap  708 . By way of example, for an electrode pair separated by a dielectric (e.g., air or an inert gas), upon reaching the dielectric breakdown voltage, the spark is generated. 
     Generation of the spark creates an electromagnetic pulse, energy from which is received by the resonant cavity or cavities  120 . The resonant cavity or cavities modulate a resonant signal ( 608 ) as described above. The modulated signal has an intensity determined by the intensity of the energy pulse and frequency components determined in part by the characteristics of the borehole that are under interrogation. 
     In the example illustrated in  FIG. 7 , the pulse generator  109  also includes a low frequency capacitor  710  that can be selected to set the resonation of the core winding of the core  702  to a low drive frequency (e.g., on the order of 1/20- 1/30 the frequency of the frequencies of the resonant cavities  120 ), providing for large voltage gain in the generator  109 . Resistor  712  is a timing resistor that serves to set the timing of the charging of the storage capacitor  704 . Finally, a single turn coil  714  may be looped through the cores of the resonators  120  in order to couple the electromagnetic energy of the pulse generator  109  into the resonators  120 . 
     In accordance with embodiments, energy can be sent wirelessly to the down-hole telemetry/interrogation device and stored. The energy can be periodically released by the spark gap in a highly energetic form thus enhancing the signal to be received above ground. 
     The signal can be energetic enough that either the pipe structure of the well or separate antennas located away from the well site can be used as receiving antennas. Transmission can thus also occur through the ground itself. 
     The data bandwidth can be of much higher frequency than mud pulsing methods. In addition to transmission of data, such as down-hole temperature and pressure, the signal can be used to interrogate the structure of the local formations. In the through-ground mode, the formation structures underground cause frequency shifts and attenuations and other phenomenon that can be interpreted and thus indicate the nature of the underground structures. 
     Circuits used by the wireless system can be quite robust and can be made to withstand the high temperatures and pressures of down-hole conditions. For example, a single semiconductor device, (e.g., diode  708  of  FIG. 7 ), can be used for power rectification. Power diodes may be selected to be sufficiently rugged to withstand typical conditions down-hole. 
     Those skilled in the art will appreciate that the disclosed embodiments described herein are by way of example only, and that numerous variations will exist. The invention is limited only by the claims, which encompass the embodiments described herein as well as variants apparent to those skilled in the art.