CONTROL OF ELECTRIC FIELD EFFECTS IN A PRINTED CIRCUIT BOARD ASSEMBLY USING EMBEDDED NICKEL-METAL COMPOSITE MATERIALS
20230009440 · 2023-01-12
Assignee
Inventors
Cpc classification
H05K1/0218
ELECTRICITY
H05K7/02
ELECTRICITY
H05K9/0088
ELECTRICITY
H05K5/065
ELECTRICITY
International classification
H05K7/02
ELECTRICITY
Abstract
A printed circuit board assembly (PCBA) controls an electrically initiated device (EID) in an electric field. The PCBA includes a conductive layer, a dielectric layer, and a trans-conductive layer (TCL). The conductive layer of the PCBA designated protected areas. An electrical current with a predetermined current density is impressed in the conductive layer when the PCBA is in the electric field. The TCL is a nickel-metal composite metamaterial positioned between the conductive and dielectric layers and configured to change in shape or thickness in the electric field such that the impressed current is steered away from the conductive layer and into the dielectric layer to prevent premature activation of the EID. A system includes an outer housing, power supply, an EID such as a sonobuoy or medical device, and the PCBA, all of which are encapsulated in the housing. A method is also disclosed for manufacturing the PCBA.
Claims
1. A printed circuit board assembly (PCBA) device, comprising: a first conductive layer; a first dielectric layer attached to the first conductive layer; a second conductive layer attached to the first dielectric layer, wherein an electrical current is impressed on the second conductive layer when the PCBA is exposed to an externally generated electric field exterior to the PCBA; a trans-conductor layer (TCL) attached to the second conductive layer and including a plurality of TCL islands of a nickel-metal composite metamaterial, each of the TCL islands having a distinct shape providing a respective impedance value in response to a variation in an intensity and/or a wavelength of the externally generated electric field; and a second dielectric layer attached to the TCL such that the TCL is positioned between the second dielectric layer and the second conductive layer, wherein the TCL has a surface roughness configured to change in response to an energy level of the externally generated electric field to thereby change an effective permittivity of the second dielectric layer and thereby direct the impressed electrical current away from the second conductive layer.
2. The PCBA device of claim 1, wherein the plurality of TCL islands includes a first TCL island spaced from a second TCL island, the first TCL island having a first irregular shape, and the second TCL island having a second irregular shape distinct from the first irregular shape of the first TCL island.
3. The PCBA device of claim 1, wherein the plurality of TCL islands includes a first TCL island spaced from a second TCL island, the first TCL island having a first size, and the second TCL island having a second size distinct from the first size of the first TCL island.
4. The PCBA device of claim 1, wherein the plurality of TCL islands includes a first TCL island spaced from a second TCL island, the first TCL island having a first surface area, and the second TCL island having a second surface area distinct from the first surface area of the first TCL island.
5. The PCBA device of claim 1, wherein the nickel-metal composite metamaterial of the TCL includes a nickel-phosphorus metamaterial and/or a nickel-chromium metamaterial.
6. The PCBA device of claim 1, wherein a nickel content of the nickel-metal composite metamaterial of the TCL is between about 10% and about 45% by weight of the TCL.
7. The PCBA device of claim 1, wherein the first and second conductive layers each includes a metallic foil sheet.
8. The PCBA device of claim 1, further comprising a pre-pregnated layer attached to the second conductive layer, the pre-pregnated layer including an uncured resin-treated glass and/or ceramic material.
9. The PCBA device of claim 1, further comprising a plurality of circuit components located on one or both of the first and second conductive layers.
10. The PCBA device of claim 1, characterized by an absence of an electromagnetic interference (EMI) shield and a Faraday cage mounted to the PCBA
11. The PCBA device of claim 1, further comprising a third conductive layer attached to the second dielectric layer.
12. The PCBA device of claim 1, further comprising a via electrically connecting the first and second conductive layers.
13. The PCBA device of claim 1, further comprising a pre-pregnated layer, wherein the first dielectric layer is mounted to an inside surface of the first conductive layer, the pre-pregnated layer is mounted to an inside surface of the first dielectric layer, the second conductive layer is mounted to an inside surface of the pre-pregnated layer, the TCL is mounted to an inside surface of the second conductive layer, and the second dielectric layer is mounted to an inside surface of the TCL.
14. A method for assembling a printed circuit board assembly (PCBA) device, the method comprising: attaching a first dielectric layer to a first conductive layer; attaching a second conductive layer to the first dielectric layer, wherein an electrical current is impressed on the second conductive layer when the PCBA is exposed to an externally generated electric field exterior to the PCBA; attaching a trans-conductor layer (TCL) to the second conductive layer, the TCL including a plurality of TCL islands of a nickel-metal composite metamaterial, each of the TCL islands having a distinct shape providing a respective impedance value in response to a variation in an intensity and/or a wavelength of the externally generated electric field; and attaching a second dielectric layer to the TCL such that the TCL is positioned between the second dielectric layer and the second conductive layer, wherein the TCL has a surface roughness configured to change in response to an energy level of the externally generated electric field to thereby change an effective permittivity of the second dielectric layer and thereby direct the impressed electrical current away from the second conductive layer.
15. The method of claim 14, wherein the plurality of TCL islands includes a first TCL island spaced from a second TCL island, the first TCL island having a first irregular shape, and the second TCL island having a second irregular shape distinct from the first irregular shape of the first TCL island.
16. The method of claim 14, wherein the nickel-metal composite metamaterial of the TCL includes a nickel-phosphorus metamaterial and/or a nickel-chromium metamaterial.
17. The method of claim 14, wherein a nickel content of the nickel-metal composite metamaterial of the TCL is between about 10% and about 45% by weight of the TCL.
18. The method of claim 14, wherein the first and second dielectric layers each includes an epoxy-resin fiberglass or a glass-reinforced epoxy laminate.
19. The method of claim 14, wherein the first and second conductive layers each includes a metallic foil sheet.
20. The method of claim 14, further comprising attaching a pre-pregnated layer to the second conductive layer, the pre-pregnated layer including an uncured resin-treated glass and/or a ceramic material.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0014]
[0015]
[0016]
[0017]
DETAILED DESCRIPTION
[0018] Referring to the drawings, wherein like reference numbers correspond to like or similar components throughout the several figures, a system 10 is shown schematically in
[0019] A printed circuit board assembly (PCBA) 16 is encapsulated within the cavity 15, along with other possible components such as a power supply 18 such as a DC battery (BAT) and an electrically-activated device (EID) 19, both of which may be collocated with the PCBA 16 as shown, i.e., external to the PCBA 16 in proximity thereto as shown in
[0020] A sonobuoy may be a submarine, air, or surface-launched device used to detect acoustic emissions or reflections in a body of water, and to transmit the detected signals to a remote source for processing. A sonobuoy may employ acoustic sensors that aid in the detection, classification, and localization of targets in the body of water via determination of sonar propagation properties and acoustic range prediction. Thus, the EID 19 of
[0021] In general, the PCBA 16 of
[0022] Instead, the PCBA 16 in all embodiments includes an embedded trans-conductor layer (TCL) 20. As explained in detail below, the TCL 20 is an embedded layer of a nickel-metal composite metamaterial, i.e., artificial materials that are structured on a size scale that is smaller than the wavelength of external stimuli, e.g., nanomaterials. Such materials may exhibit properties that are not typically found in nature. One such property used herein is the tendency to compress in the presence of energy from an externally-generated electric field, which is represented schematically in
[0023] The TCL 20 as described herein is configured to act as a filter or waveguide of broad-band energy from the externally generated electric field {right arrow over (E)}. The ability to change in shape or thickness in the presence of the electric field {right arrow over (E)} allows an impressed current in the conductive layer 30 to be steered or guided away from the conductive layer 30 and into the dielectric layer 40 to thereby prevent premature activation of the EID 19. As used herein, the term “broadband” refers to a sufficiently wide range of radio frequency (RF) energy, e.g., 2 MHz-20 GHz in an example embodiment, and any complex resonant fields associated with this incident energy. It is recognized herein that the electric field {right arrow over (E)} may induce a current with a current density J in the PCBA 16. The term “current density” refers to the electric current (I) per unit area (A) of cross section. The magnitude of the current density J, as measured in amperes/m.sup.2, may be given as:
[0024] In particular, the TCL 20 may be shaped, sized, and positioned, i.e., configured, to direct undesirable energy from the electric field {right arrow over (E)} through the PCBA 16 without penetrating into an any conductive layers. The TCL 20 is embedded in the PCBA 16 itself, and thus unlike Faraday cages and other EMI shielding designs does not cover the PCBA 16, i.e., the TCL 20 is not positioned between an uppermost surface 35 of the PCBA 16 and the incident electric field {right arrow over (E)}. Likewise, the TCL 20 does not reflect energy away from the PCBA 16 like a Faraday shield, and also does not suffer from the same Z-dimensional packaging issues of such shields.
[0025] A key element of the present disclosure is the use of nickel in the TCL 20 in a particular manner, which is to control the undesirable effects of the electric field {right arrow over (E)}. The TCL 20, due to its nickel content, is configured to contract or otherwise change shape or deform in the presence of the electric field {right arrow over (E)}, which in turn allows the TCL 20 to be formed with a variable geometry and thus control the effects of the electric field {right arrow over (E)} on the performance of the PCBA 16. The particular design of the TCL 20 is both field and application specific. A general approach for achieving the desired end results via the TCL 20 is described below with reference to
[0026] Specifically, the TCL 20 is configured to reduce or eliminate the effects of high-intensity radiated broadband fields, including peak fields as high as 5000 volts per meter with vertical and horizontal polarization. Energy from the incident electric field {right arrow over (E)} is guided away from the EID 19 by passively controlling the internal complex impedance of the PCBA 16. The same electric field {right arrow over (E)} falls incident upon the PCBA 16 sets up an immediate electric field vector potential from a top side to a bottom side of the PCBA 16, with “top' referring to the surface of the PCBA 16 facing the incident electric field {right arrow over (E)}.
[0027] The true transverse electric field established by the electric field vector potential will change characteristics of the nickel-metal composite materials of the TCL 20, including a change in shape and/or thickness of the TCL 20, thereby changing the impedance of the PCBA 16. As will be appreciated by one of ordinary skill in the art, the impressed current will follow a path of least resistance away, which in the present construction is away from the conductive layer 30 or any protected areas in or on such a layer 30. In particular, the characteristic impedance of the nickel-metal composite materials changes by physically changing the natural surface roughness and physical size and/or shape of the nickel-metal composite materials of the TCL 20 throughout the PCBA 16. Such a change is caused by the high intensity of the magnetic field associated with the predefined polarization of the illuminating spherical electric field.
[0028] As the impressed currents will tend to flow in the path of least resistance, such currents can be steered through the PCBA 16 using the TCL 20, and ultimately dissipated into the dielectric layers 40 shown in
[0029] As used herein, the term “nickel-metal composite” refers to any alloy of nickel, with nickel phosphorus (NiP) and nickel chromium (NiCr) being two possible embodiments exhibiting desirable properties and control results. NiP, for instance, is highly resistive, and in a field such as the electric field {right arrow over (E)}, exhibits a measurable frequency response. This response can be employed to the desired effect as explained below. An alloy having an excessive amount of nickel, however, tends to behave too much like a conductor, and therefore the percentage of nickel by weight should be limited. An example range that achieves the desired effect is 10-45% of nickel by weight of the TCL 20.
[0030] Additionally, the TCL 20 exhibits capacitance due in part to its surface roughness. For this reason, the TCL acts a transmission line, and for this reason is referred to herein as a Trans-Conductor Layer or TCL. In acting like a transmission line, the TCL 20 is able to reduce EMI effects from the externally-generated electric field {right arrow over (E)} via embedding of nickel-based metamaterials in a purposeful, design-specific manner. The TCL 20 guides unwanted current density flow away from any adjacent conductive layers 30 or other predetermined sensitive protected areas of the PCBA 16, with energy dissipated away from such areas via thermal conductance and reactance. In this manner, the internal traces of the PCBA 16 are prevented from inadvertently acting as fuses in the presence of the electric field {right arrow over (E)}, thereby avoiding prematurely firing or triggering some action via the PCBA 16, such as an activation of the EID 19.
[0031] In the example system 10 shown in
[0032] Referring to
[0033] Three conductive layers 30 are shown in the non-limiting example embodiment of
[0034] Suitable materials for the dielectric layers 40 include epoxy-resin fiberglass or a glass-reinforced epoxy laminate, e.g., FR-4, or any other application-suitable material. The pre-pregnated layer 50 may be formed as an uncured resin-treated glass or ceramic sufficient for filling any gaps or spacing between the outer layers, i.e., conductive layers 30 having the outermost surfaces 35. Use of the pre-pregnated layer(s) 50 may help to bond the various layers 20, 30, and 40 together, and also providing additional structural integrity for the PCBA 16.
[0035] While the layers 20, 30, and 40 are shown with uniform distribution in
[0036] Referring to
[0037] After this step is complete, the components of the PCBA 16 are identified that are susceptible to the identified properties of the electric field {right arrow over (E)}. These components of the conductive layer 30 are referred to hereinafter as the predetermined protected components or areas. Example components or areas can include traces, embedded vias, through vias, connectors, ribbon cable, wires, and the like. The method 100 proceeds to steps 104 and 106 when all of this is completed.
[0038] At step 104, the method 100 includes determining the depth of penetration (DOP) of the expected portions of the electric field {right arrow over (E)} into the identified predetermined protected components from step 102, e.g., via direct measurement, modeling, or theoretical calculation. The end goal of step 104 is to determine the thickness of the TCL 20, which should be sufficient for conducting the required electrical current from the electric field {right arrow over (E)} having a predetermined current density J. The method 100 then proceeds to step 108.
[0039] Step 106, which is performed in tandem with step 104, includes determining the maximum allowable resistance (R.sub.MAX) of the circuit trace being formed by the TCL 20. The circuit embodied as the PCBA 16 has an overall maximum resistance for implementation of the desired application, including control of the EID 19 of
[0040] Step 108 entails determining the power loss (P.sub.LOSS) in the PCBA 16. Step 108 may entail solving the following equation:
where R.sub.S is the sheet resistance and J.sub.S is the current density of the current flowing the TCL 20. The impressed and conducted current densities are also determined, with impressed current being the current due to radiation from the electric field {right arrow over (E)} and the conducted current being the current due to any adjacent sources. The required maximum attenuation for controlling the current density J resulting from the electric field {right arrow over (E)} is ultimately determined as part of step 108. As the TCL 20 is not purely a capacitor, nor is it purely an inductor or a resistor, the embedded TCL 20 will change its impedance in the presence of the electric field {right arrow over (E)}. That is, the TCL 20 will react over a very broad band range of frequencies with variable attenuation. The method 100 proceeds to step 110 once the power loss and maximum attenuation have been determined.
[0041] Step 110 includes defining the shape of the TCL 20. This includes defining the length, width, and thickness of the TCL 20. For commercially available sheets of NiP, for example, market standard sheet resistance R.sub.S is 10, 25, and 250 Ohms/meter, with various sheet thicknesses. For any of the suitable nickel-metal based materials used for construction of the TCL 20, as the magnetic field increases the nickel will contract. Although the nickel contracts, there is more phosphorus, in the example of NiP, so the surface roughness of the TCL 20 will change with the contraction. This in turn changes the capacitance and changes the effective permittivity of the dielectric material located adjacent to the TCL 20, for instance the dielectric layer 40 shown at that location in
[0042] Step 112 includes constructing the TCL 20 with the determined shape from step 110. Constructing the TCL 20 with the desired shape may take place with the fabrication of the PCBA 16, including positioning the TCL 20 with the determined thickness and shape adjacent to the dielectric layer 40 and the protected areas of the conductive layer 30 to form the PCBA 16. The PCBA 16 thereafter can be installed in a system, such as the system 10 shown in
[0043] Aspects of the present disclosure have been described in detail with reference to the illustrated embodiments; those skilled in the art will recognize, however, that many modifications may be made thereto without departing from the scope of the present disclosure. The present disclosure is not limited to the precise construction and compositions disclosed herein; any and all modifications, changes, and variations apparent from the foregoing descriptions are within the spirit and scope of the disclosure as defined in the appended claims. Moreover, the present concepts expressly include any and all combinations and subcombinations of the preceding elements and features.