This application is a non-provisional of U.S. provisional patent application No. 61/723,312, filed Nov. 6, 2012, which is incorporated by reference.
The amount of data transferred between electronic devices has grown tremendously the last several years. Large amounts of audio, streaming video, text, and other types of data content are now regularly transferred among desktop and portable computers, media devices, handheld media devices, displays, storage devices, and other types of electronic devices. Since it is often desirable to transfer this data rapidly, the data rates of these transfers have substantially increased.
These data transfers may occur over various media. For example, the data transfers may be made wirelessly, over cables including wire conductors, over fiber optic cables, or they may be made in other ways.
Cables that include wire conductors may include a connector insert at each end. The connector inserts may be inserted into receptacles in the communicating electronic devices. Other cables may be tethered, that is, they may be connected directly to components internal to one of the communicating electronic devices.
Transferring data at these rates has proven to require new types of cable. Conventional cables are proving to have insufficient capabilities to handle signals at these higher data rates. New cables having improved capabilities are thus needed.
For example, conventional cables tend to have higher parasitic components, such as series resistance, than may be desirable. These parasitic components may degrade signal levels and, along with other factors (such as reflections and parasitic capacitances), lead to higher insertion losses. These higher insertion losses may lead to reduced signal amplitude and corrupted signal edges, making accurate data reception more difficult.
Thus, what is needed are circuits, methods, and apparatus that provide cables capable of high-speed data transmission and have a low insertion loss.
Accordingly, embodiments of the present invention may provide cables capable of high-speed data transmission and having a low insertion loss. Specifically, embodiments of the present invention may provide cables having an eliminated, shifted, or reduced suckout component of insertion loss.
Various embodiments of the present invention may mitigate or reduce the effect of the suckout component of insertion loss. Embodiments of the present invention may accomplish this by eliminating, or at least partially eliminating, the suckout component by providing a continuous return path. Other embodiments may shift the frequency of the suckout component to a high frequency where it no longer interferes or significantly attenuates signals being conveyed by the cable. Still other embodiments of the present invention may reduce or control the magnitude of the suckout component.
Suckout may contribute to the insertion loss for cables. The result of suckout may be a band-stop filter characteristic in the transmission curve or a cable. This suckout may be partially due to losses in return paths of the cables. For example, a cable may include one or more conductors, such as a twisted pair. Forward current may (locally) flow in a first direction in the twisted pair. A return current may flow in a conductive tape layer, where the conductive tape layer is wrapped around the twisted pair. The return current may attempt to (locally) flow through the conductive tape layer in a second direction, which may be 180 degrees out of phase with the first direction. The return current path may cross one or more boundaries where the conductive tape overlaps itself. This boundary or overlap crossing may generate losses, which may cumulatively be referred to as suckout.
Accordingly, embodiments of the present invention may eliminate, or at least partially eliminate, this suckout component by providing a continuous return path, that is, a return path without boundary crossings. An illustrative embodiment of the present invention may provide a cable including a twisted pair and a conductive tape layer. The twisted pair may be twisted in a first direction such that it has a first pitch or lay length. The conductive tape layer may be wrapped around the twisted pair such that it overlaps itself to form boundaries or overlaps. The conductive tape layer may have a second pitch or lay length. The first lay length may match the second lay length. In this way, the local return current may flow in the conductive tape layer without, or with minimal, boundary or overlap crossings. These embodiments of the present invention may further include shields between the twisted pair and the tape layer, one or more drain lines twisted with the twisted pair, or they may include other structures.
Another illustrative embodiment of the present invention may provide a cable including a twisted pair and a shield layer. The shield layer may include a number of wires or conductors. The twisted pair may be twisted in a first direction such that it has a first lay length. The shield layer may be wrapped around the twisted pair in the first direction such that it has a second lay length. The first lay length may match the second lay length. Again, the local return current may flow in the shield layer without, or with minimal, crossings between shield wires or conductors. These embodiments of the present invention may further include tape layers around the twisted pair and the shield layer, one or more drain lines twisted with the twisted pair, or they may include other structures.
Another illustrative embodiment of the present invention may provide a cable including a twisted pair, a shield layer, and a conductive tape layer. The twisted pair may be twisted in a first direction such that it has a first lay length. The shield layer may include a number of conductors and may be wrapped around the twisted pair in the first direction such that it has a second lay length. The conductive tape layer may be wrapped around the twisted pair and shield layer such that it is in contact with the shield layer and such that it overlaps itself to form boundaries or overlaps. The conductive tape layer may have a third lay length. The second lay length and the third lay length may be mismatched such that they form a continuous return path for the length of the cable.
Various illustrative embodiments of the present invention may provide twisted pairs including one or more drain wires that are used in conjunction with a shield and a tape layer. In these embodiments of the present invention, lay lengths of the shield and tape layer may match each other, lay lengths of the twisted pair and drain wires may match, or all these lay lengths may match.
Other illustrative embodiments of the present invention may provide cables where the suckout component of the insertion loss is pushed out to high frequencies such that signals conveyed by the cable are not severely affected. In these embodiments, a lay length of either or both a twisted pair and tape layer are significantly reduced.
Other illustrative embodiments of the present invention may provide cables where the suckout component of the insertion loss is reduced in magnitude. One embodiment of the present invention may provide a cable where a lay length for a tape layer is greatly increased. This may reduce the number of boundary or overlap crossings, thus reducing the magnitude of the suckout.
Another illustrative embodiment of the present invention may provide a cable where a difference between a lay length of a twisted pair and a lay length of a tape layer is minimized. This minimization again may reduce the number of boundary or overlap crossings, thus reducing the magnitude of the suckout.
Another illustrative embodiment of the present invention may provide a cable where a lay length of a tape layer may vary over the length of a cable. Another illustrative embodiment of the present invention may provide a cable where a width of a tape layer, and therefore the overlap, may vary over the length of a cable. In still other embodiments, both the lay length and the width of the tape layer may vary over the length of a cable. These variations may effectively spread the suckout over a larger range of frequencies such that its effect is minimized or mitigated.
Embodiments of the present invention may be well-suited to improving the performance of twisted pairs, particularly twisted pairs conveying differential signals. Other embodiments of the present invention may be used to improve the performance of other types of conductors, such as coaxial cables, and other types of conductors.
Embodiments of the present invention may provide cables for various types of devices, such as portable computing devices, tablets, desktop computers, laptops, all-in-one computers, cell phones, smart phones, media phones, storage devices, portable media players, navigation systems, monitors, power supplies, adapters, and chargers, and other devices. These cables may provide pathways for signals and power compliant with various standards such as Universal Serial Bus (USB), a High-Definition Multimedia Interface (HDMI), Digital Visual Interface (DVI), power, Ethernet, DisplayPort, Thunderbolt, Lightning and other types of standard and non-standard interfaces.
Various embodiments of the present invention may incorporate one or more of these and the other features described herein. A better understanding of the nature and advantages of the present invention may be gained by reference to the following detailed description and the accompanying drawings.
Electronic system 100 may include cable 110 joining electronic devices 120 and 130. Electronic device 120 may be a laptop or portable computer having screen 122. Electronic device 130 may be an all-in-one computer including screen 132, keyboard 134, and mouse 136. In other embodiments of the present invention, cable 110 may couple various types of devices, such as portable computing devices, tablets, desktop computers, cell phones, smart phones, media phones, storage devices, portable media players, navigation systems, monitors power supplies, adapters, and chargers, and other devices. These cables may provide pathways for signals and power compliant with various standards such as Universal Serial Bus (USB), a High-Definition Multimedia Interface (HDMI), Digital Visual Interface (DVI), power, Ethernet, DisplayPort, Thunderbolt, Lightning and other types of standard and non-standard interfaces.
Ideally, cable 110 would not attenuate or distort signals being transmitted between electronic device 120 and electronic device 130. But cable 110 may include various parasitics and non-ideal characteristics that may attenuate and distort these signals. These losses may be referred to as insertion losses. A simplified example is shown in the following figure.
One component of this insertion loss may be referred to as suckout. One source of this suckout may be caused by aspects of the construction of a ground or return path in cable 110. This is shown further below. A graph showing the suckout frequency characteristics of a cable are shown in the following figure.
Suckout 312 may be the result of physical characteristics of the components in cable 110.
Tape layer 430 may be formed of polyester or other type of film, which may be metallized on one side. The polyester film may be Mylar™ or other such film. One side of tape layer 430 may be metallized with copper, aluminum, or other conductive material. Tape layer 430 may be oriented such that the copper metallization may be in contact with drain wire 440.
Cables 110 may include various conductors such as twisted pairs formed by conductors 410 and 510. Cable 110 may also include other component such as drain wires, shielding, jacket pairs, single conductors, fibers, such as cotton or aramid fibers, and other components. Also, while embodiments of the present invention may be well-suited to improving the performance of twisted pairs, particularly twisted pairs conveying differential signals, other embodiments of the present invention may be used to improve the performance of other types of conductors, such as coaxial cables, and other types of conductors.
Tape layers 430 and 540 may wrap around their twisted pairs in a helical fashion. A length of a single twist or 360-degree rotation of this helix may be referred to as a pitch or lay length. An example is shown in the following figure.
In this example, twists in tape layers 430 and 540 are shown as having a gap between them. In other embodiments of the present invention, tape layer 430 or 540 may overlap itself by a certain amount. This overlap may be anywhere from zero or a few percent of the width of the tape, to 10 to 20 percent, and up to 50 percent or more of the width of the tape.
Tape layer 430 or 540 may be twisted in one of two directions. That is, it may be twisted in a first or second direction. Directions may be thought of as clockwise or counterclockwise rotation directions. Whether a rotation appears to be clockwise or counterclockwise may depend on ones frame of reference.
Just as the tape layer may have a pitch or lay length associated with it, so do the twisted-pairs formed by conductors 410 or 510. An example is shown in the following figure.
Just as the twisted-pair and tape layers may have a lay length, so may shield 530. An example is shown in the following figure.
In cable portion 400 as shown in
Forward current 912 may flow in twisted-pair 910. A return current 922 in shield 920 may thus be generated in the opposite direction. As can be seen, this direction takes current 922 across overlap or boundary areas 930. Again, this overlap or boundary crossing may cause losses, which may result in suckout. Further details are shown in the following figure.
Unfortunately the path formed by the copper metallization layer 1020 has a gap across overlap portion 1030. This may mean that current 1022 flows through a capacitor or gap formed at overlap 1030. Specifically, current 1022 may flow through a capacitor formed by copper layer portions 1024 and 1026, which are insulated by a dielectric formed by polyester layer portion 1012.
While the above examples illustrate overlap portions in tape layers, similar effects can be seen in a shield layer, when a shield layer is present. Again, a shield layer may be formed by one or more conductors wrapped around a twisted pair. Return current may flow in a direction that cuts across several conductors. In this situation, gaps or boundaries between the conductors may cause losses similar to those generated by overlap portions 930.
In order to avoid current flow through the overlap and boundary portions in shield and tape layers, embodiments of the present invention may provide cable portions have a continuous return path. In a particular embodiment of the present invention, this may be achieved by matching a lay length of a twisted-pair to a lay length of a tape layer. An example is shown in the following figure.
Mathematically, this may be explained as follows.
The frequency of the suckout stop band may be found by Equation 1:
where f is frequency of the suckout, λ is pitch or lay length, and ν is phase speed or phase velocity.
The combined speed of propagation, or phase speed, for the twisted pair and tape layer can be found by
where c is the speed of light, p is the twisted pair, t is the tape layer, and α is the pitch angle of the tape layer.
The combined lay length of the twisted pair and tape layer can be found by Equation 2:
again, where p is the twisted pair and t is the tape layer. From Equation 2, we can see if we make the two lay lengths equal, the denominator goes to zero, and the combined lay length goes to infinity. Substituting this result into Equation 1, we may see that
Accordingly, if we make the two lay lengths equal, we can remove the suckout for the cable.
In this and other embodiments of the present invention, a shield may be included. In these embodiments of the present invention, a shield layer may have a lay length that is different than the lay length of the twisted pair (and hence the tape layer), or it may have a lay length that matches the lay length of the twisted-pair. In this way, return currents generated in a shield layer may flow without crossing from one conductive strand to another. In still other embodiments the present invention, the twisted-pair, shield, and tape layers may all have a similar or the same lay length.
In this and other embodiments of the present invention, the shield layer and tape layers maybe electrically connected along the length of the cable. In this case, overlap and boundaries in the tape in shield layers may be offset such that they don't line up. This may provide a current path through the tape layer at shield boundaries, and through the shield layer at tape layer overlap portions. This may therefore provide a continuous return path. An example is shown in the following figure.
Mathematically, this may be seen as placing boundary portions 1212 and overlap portions 1222 at locations such that a length of the cable is shorter than the least common multiple of the lay lengths of the lay length of the tape layer and the shield layer, or
LCM(λt,λs)>Lcable
In other embodiments of the present invention, a shield and one, two, or more drain wires may be included as a return path, or as part of a return path, that may further include a tape layer. An example is shown in the following figure.
λt=λs and λd=λp
In other embodiments of the present invention, each of these pitches or lay lengths may match each other. That is,
λt=λs=λd=λp
In other embodiments of the present invention, instead of providing a continuous return path, the frequency of the suckout can be pushed out to higher frequencies. An example is shown in the following figure.
As can be seen in Equation 2, the numerator, and therefore the combined lay length, may be driven to zero if the lay length of either of the tape layer or twisted pair is driven near zero. This in turn, combined with Equation 1, shows that the suckout frequency may be pushed out in frequency. This may be shown specifically in Equations 3 (for combined lay length) and 4 (for suckout frequency),
An example of such a configuration is shown following figure.
Again, twisted pair 1410 may be twisted such that has a very short lay length. However, this may not be as practical to manufacture as a short lay length for tape layer 1420.
In other embodiments of the present invention, the magnitude of the suckout can be reduced. For example, in other embodiments of the present invention, a lay length of a tape or shield layer may be very long. This long length may reduce a number of boundaries crossed by a return current. An example is shown in the following figure.
As λt increases, N decreases.
In other embodiments of the present invention, instead of providing a continuous return path by matching lay lengths, differences between lay lengths of twisted pairs and tape (or shield) may be minimized. This may again help to reduce the magnitude of the suckout, even if it is not eliminated or nearly eliminated.
In other embodiments of the present invention, the lay length of a shield layer or a tape layer may be varied over length of a cable. This variation may effectively spread the frequencies of the suckout, thereby reducing its magnitude. Examples are shown in the following figures.
As was shown in
The above description of embodiments of the invention has been presented for the purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form described, and many modifications and variations are possible in light of the teaching above. The embodiments were chosen and described in order to best explain the principles of the invention and its practical applications to thereby enable others skilled in the art to best utilize the invention in various embodiments and with various modifications as are suited to the particular use contemplated. Thus, it will be appreciated that the invention is intended to cover all modifications and equivalents within the scope of the following claims.
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Number | Date | Country | |
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20140124236 A1 | May 2014 | US |
Number | Date | Country | |
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61723312 | Nov 2012 | US |