The drawings referenced herein form a part of the specification. Features shown in the drawing are meant as illustrative of only some embodiments of the invention, and not of all embodiments of the invention, unless otherwise explicitly indicated, and implications to the contrary are otherwise not to be made.
In the following detailed description of exemplary embodiments of the invention, reference is made to the accompanying drawings that form a part hereof, and in which is shown by way of illustration specific exemplary embodiments in which the invention may be practiced. These embodiments are described in sufficient detail to enable those skilled in the art to practice the invention. Other embodiments may be utilized, and logical, mechanical, and other changes may be made without departing from the spirit or scope of the present invention. The following detailed description is, therefore, not to be taken in a limiting sense, and the scope of the present invention is defined only by the appended claims.
The sensing elements 102 detect the data stored on the portion of the magnetic storage medium over which the sensing elements 102 are currently incident. The sensing elements 102 may be thin-film sensors in one embodiment. Each of the sensing elements 102 has an inherent resistance, RseY, which varies depending on the data on the current portion of the magnetic storage medium over which these sensors are currently located. That is, a transition in the magnetic polarity of the portion of the magnetic storage medium over which the sensor is currently located causes the resistance of each of the sensing elements 102 to vary. In this way, the sensing elements 102 can be used to read the data stored on the magnetic storage medium. The inherent resistance RseY of each of the sensing elements 102 is nominally equal, but in actuality is different, due to manufacturing tolerances, local heating and other factors that affect these resistances. Thus, the resistance RseY, where Y=1 . . . N, corresponding to the N sensing elements 102, are typically different for each sensing element Y. The resistances also may be different from one magnetic storage device to another, while the biasing circuitry within the sensing mechanism 100 (i.e., including the voltage source 108) is nominally identical due to the much higher tolerances achievable within the electronics industry.
To either end of the sensing elements 102 are electrically connected the variable resistive elements 104 and the variable resistive elements 106. The variable resistive elements 104 and 106 are together referred to as the variable resistive mechanisms. Thus, for the sensing element 102A, the variable resistive element 104A is electrically connected to one end of the sensing element 102A, one end of the variable resistive element 106A is electrically connected to the other end of the sensing element 102A, and the other end of the element 106A is connected to the ground of the voltage source 108, or to another offset voltage, which can be arbitrary. Thus, there exists a variable resistive mechanism that is electrically connected to the sensing element 102A that is made up of the elements 104A and 106A. Likewise, for the sensing element 102B, the variable resistive element 104B is electrically connected to one end of the sensing element 102B, and the variable resistive element 106B is electrically connected to the other end of the sensing element 102B, and so on.
The first variable resistive elements 104 each have a variable resistance value R1vrY, and the second variable resistive elements 106 each have a variable resistance value R2vrY, where Y=1 . . . N, corresponding to the N variable resistive elements 104 and the N variable resistive elements 106. The resistances R1vrY and R2vrY can be set independent of one another. Thus, the resistance R1vrY for any first variable resistive element Y can be set differently than that for any other first variable resistive element Y. Likewise, the resistance R2vrY for any second variable resistive element Y can be set differently than that for any other second variable resistive element Y. Similarly, the resistance R1vrY for any first variable resistive element Y can be set differently than the resistance R2vrX for any second variable resistive element X, where X may be equal to or different than Y. For a given element Y, the values of R1vrY and R2vrY are selected to be nominally equal.
There are currents 110A, 110B, . . . , 110N, collectively referred to as the currents 110, flowing through the sensing elements 102. For any given sensing element Y, the corresponding current iY flowing through the sensing element is equal to
In equation (1), for the sensing element Y, R1vrY is the resistance of the first variable resistive element Y that is electrically connected to one end of this sensing element, and R2vrY is the resistance of the second variable resistive element Y that is electrically connected to the other end of this sensing element. The resistance RseY is the resistance of the sensing element Y itself. The voltage Vcc is the voltage provided by the voltage source 108. The same voltage source 108 is connected to the sensing elements 102 as is depicted in
The current iY flowing through any given sensing element Y is varied so that it is the current corresponding to the optimum sensing capability of the sensing element relative to the magnetic storage medium in question. The manner by which the optimum current is determined is known by those of ordinary skill within the art. To vary the current iY flowing through any given sensing element Y so that it is the optimum, or desired, current, the variable resistances of the first variable resistive element Y connected to one end of the sensing element and of the second variable resistive element Y connected to the other end of the sensing element are set in accordance with equation (1) above. That is, because Vcc is known, and RseY is known, the desired current iY can be specified by appropriately varying the variable resistances R1vrY and R2vrY of the first and second variable resistive elements Y in accordance with equation (1) above. The current iY flowing through any given sensing element Y is thus independent of the currents flowing through the other of the sensing elements 102.
Furthermore, there are mid-point voltages 112A, 112B, . . . , 112N, collectively referred to as the mid-point voltages 112, at the midpoints of the sensing elements 102. That is, the mid-point voltage at any given sensing element is the voltage measurable halfway between the ends of the sensing element, at the center of the sensing element in one embodiment. For any given sensing element Y, the corresponding mid-point voltage VmY at the mid-point of this sensing element is equal to
As in equation (1), in equation (2), for the sensing element Y, R1vrY is the resistance of the first variable resistive element Y that is electrically connected to one end of this sensing element, and R2vrY is the resistance of the second variable resistive element Y that is electrically connected to the other end of this sensing element. The resistance RseY is the resistance of the sensing element Y itself. The voltage Vcc is the voltage provided by the voltage source 108.
To minimize, if not to completely eliminate, the electrochemical-plating effects, as well as other electrochemical effects, among the sensing elements 102, as described in the background section, the mid-point voltages 112 are desirably set so that they are equal to one another. That is, by having VmY be the same value, regardless of the sensing element Y in question, embodiments of the invention substantially reduce or eliminate the electrochemical effects described in the background section, since there are then no absolute voltage differences among the sensing elements 102. Thus, the potential for the interaction between the sensing mechanism 100 and the magnetic storage medium being read by the sensing elements 102 to cause such electrochemical effects in relation to the sensing elements 102 is reduced.
Embodiments of the invention achieve maintenance of equal mid-point voltages 112, while still allowing the individual currents 110 to be independently varied, by setting R1vrY equal to R2vrY for any given sensing element Y. Therefore, the desired current iY for any given sensing element Y can be achieved by appropriately varying the variable resistances R1vrY and R2vrY. Stipulating an additional constraint, that R1vrY is equal to R2vrY for any given sensing element Y, further ensures that VmY is the same for all the sensing elements 102.
This can be simply proven by setting R2vrY equal to R1vrY in equation (2) above. Making this substitution yields the following:
Therefore, so long as R2vrY equals R1vrY, for any given sensing element Y, VmY is dependent only on Vcc, and not on any of the values of the resistances RseY, and R1vrY, As such, the desired current iY through any given sensing element Y can be achieved by varying the resistances R1vrY and R2vrY of the first and second variable resistive elements Y connected to this sensing element, while maintaining the same VmY for all the sensing elements 102, so long as R1vrY remains equal to R2vrY.
It is noted that
While embodiments of the invention are substantially described herein in relation to a magnetic storage medium that is a magnetic tape cartridge, other embodiments are amenable to implementation in relation to other types of magnetic storage media, such as hard disk drives, and so on. Thus, in an embodiment in which the magnetic storage medium is a magnetic tape cartridge, the magnetic storage medium is removably insertable into the mass storage device 300, as can be appreciated by those of ordinary skill within the art. In an embodiment in which the magnetic storage medium is a hard disk drive, the magnetic storage medium is part of and fixed within the mass storage device 300, as can also be appreciated by those of ordinary skill within the art.
The variable resistive element 104A is shown in
More particularly, the variable resistance R1vr1 of the variable resistive element 104 is equal to
In equation (4), RY is the resistance of a given of the resistors 402 referred to as the resistor Y, where there is a total of M of the resistors 402. Furthermore, SY is a binary variable that is equal to one when a given of the switches 404, referred to as the switch Y, is closed, and that is equal to zero when the switch is open. Therefore, for each resistor Y, the resistance RY of this resistor contributes to the total resistance R1vr1 if its corresponding switch Y is closed, such that SY is equal to one, and does not contribute to the total resistance R1vr1 if its corresponding switch Y is open, such that SY is equal to zero.
The variable resistive element 106A is also shown in
More particularly, the variable resistance R2vr1 of the variable resistive element 106 is similarly equal to
In equation (5), RY is the resistance of a given of the resistors 406 referred to as the resistor Y, where there is a total of M of the resistors 406. Furthermore, SY is a binary variable that is equal to one when a given of the switches 406, referred to as the switch Y, is closed, and that is equal to zero when the switch is open. Therefore, for each resistor Y, the resistance RY of this resistor contributes to the total resistance R2vr1 if its corresponding switch Y is closed, such that SY is equal to one, and does not contribute to the total resistance R2vr1 if its corresponding switch Y is open, such that SY is equal to zero. When a given resistor has its corresponding switch closed, it is said that the resistor has been switched on. Likewise, when a given resistor has its corresponding switch opened, it is said that the resistor has been switched off.
To ensure that R1vr1 is always equal to R1vr2, the resistors 402 of the variable resistive element 104A should be equal in number and correspond in value to the resistors 406 of the variable resistive element 106A. Thus, the resistance of the resistor 402A should be equal to the resistance of the resistor 406A, the resistance of the resistor 402B should be equal to the resistance of the resistor 406B, and so on. Furthermore, corresponding of the switches 404 and 408 should be both opened or both closed. Thus, if the switch 404A is open, then the switch 408A should be open, if the switch 404B is closed, then the switch 408B should also be closed, and so on.
In one embodiment, the sensing mechanism 100 in the embodiment of
In one embodiment, the variable resistive mechanism for the sensing element 102A is said to include the variable resistive elements 104A and 106A, and thus their constituent resistors 402 and 406 and switches 404 and 408, as well as the constant resistive elements 410 and 412. The resistors 402 and 406 of the variable resistive elements 104A and 106A, as well as the constant resistive elements 410 and 412, may be implemented as discrete resistors that are soldered or otherwise mounted onto a printed circuit board of the sensing mechanism 100. Alternatively, they may be thin-film resistors formed within an integrated circuit of the sensing mechanism 100. The switches 404 and 408 may be field-effect transistors (FET's), other types of transistors, or other types of switches completely.
The desired current 110A flowing through the sensing element 102A is controlled in the embodiment of
As can be appreciated by those of ordinary skill within the art, the sensing mechanism 100 of
As another example, there may be coupling points 416A and 416B, collectively referred to as the coupling points 416. The coupling points 416 may connect to detection circuitry of the sensing mechanism 100, which is not particularly shown in
The resistance of the sensing element 102A, Rsel, is uniformly distributed over the length 506 of the sensing element 102A. This is why the mid-point voltage 112A at the mid-point 508 of the sensing element 102A is based on Rsel divided by two in equation (3) above. Thus, from the end 504 to the mid-point 508 of the sensing element 102A, the resistance of the sensing element 102A is half of its total resistance, or Rsel divided by two.
As depicted in
It is noted that throughout the discussion of the method 600 of
Rvr=Rx (6)
In equation (6), Rx is the largest resistance of any of the N resistors, where just the resistor having this resistance Rx is switched on, such that none of the other resistors are switched on and such that none of the other resistors contribute to the resistance Rvr. The resistance of the sensing element 102A is then determined (604), by using any of a number of different conventional approaches. For instance, Kirkov's laws may be employed, as can be appreciated by those of ordinary skill within the art.
Thereafter, based on the resistance of the sensing element 102A, it is determined which of the possible values of the variable resistances may be desirably employed, as a set of resistances (606). That is, for the sensing element to optimally function, it may be known that a desired range of currents should flow through the sensing element 102A. This desired range of currents may be based on, among other things, the sensor amplitude, proper signal time response, reliability for thermal and electrical degradation, and minimization of the bit error rate (BER). Therefore, since the current flowing through the sensor is the voltage provided by the voltage supply 108, divided by the resistance of the sensing element in series with the variable resistances of the variable resistive elements 104A and 106A, a set of resistances that the variable resistive elements 104A and 106A may take on to yield currents within the desired range can be determined.
For example, each of the variable resistive elements 104A and 106A in
As a result, there are up to fifteen different possible combinations of the corresponding four resistors, depending on which of the resistors are switched on, and there are thus up to fifteen possible different variable resistances for each of the variable resistive elements 104A and 106A. Of these possible different variable resistances, however, only a smaller (or at least no greater) number may yield the current flowing through the sensing element 102A that is within the optimal range of currents. These resistances thus form the set of variable resistances determined in part 606.
The variable resistances of the variable resistive elements 104A and 106A are next first each set to the highest value within this set of resistances (608). That is, the individual resistors of the elements 104A and 106A are appropriately turned on or off to yield this highest resistance value. The performance of the sensing element 102A is then determined (610), by, for instance, measuring the response of the sensing element 102A to predetermined calibration data written on the magnetic tape media. If all the values within the set of resistances have not yet been tested in this way (612), then the variable resistances of the variable resistive elements 104A and 106A are each set to the next highest value within this set of resistances (614), and the method 600 is repeated at part 610. This process continues until all of the resistance values within the set of resistances have been tested.
The performance of the sensing element 102A will be best, or most optimal, where the variable resistances of the variable resistive elements 104A and 106A have been each set to an optimal given one of the values within the set of resistances. For instance, the response of the sensing element 102A to the predetermined calibration data written on the magnetic tape media may be most sensitive to the predetermined calibration data where the variable resistances of the variable resistive elements 104A and 106A were each set to a particular value within the set of resistances. Therefore, the resistance to which each of the variable resistive elements 104A and 106A is ultimately set as part of the calibration process is that within the set of resistances that provides such optimal performance of the sensing element 102A (616).
Once calibration of the sensing element 102A has been achieved, such that the optimum variable resistance values for the elements 104A and 106A have been set, the read/write head (of which the sensing element 102A is a part) may be ready for normal operation such that magnetic storage medium can be read. The magnetic storage medium is read by detecting an alternating current (AC) resistance signal of the sensing element for a given current portion of the medium (618), and, on the basis of the signal read, determining the data stored in the current portion of the medium (620).
As a simple example, where the AC resistance signal does not change, then the data is determined as a logic zero, and where there is a transition within the AC resistance signal, then the data is determined as a logic one. In actual practice, reading the magnetic storage medium is more complicated, but is well known to those of ordinary skill within the art. Because the mid-point voltages 112 of the sensing elements 102 are equal to one another, even though the currents 110 flowing through the sensing elements 102 are independently varied and may not be equal to one another, electrochemical-plating and other effects are substantially reduced, if not totally eliminated.
Embodiments of the invention provide for advantages over the prior art. Within the prior art, the mid-point voltages of the sensing elements of a sensing mechanism for reading a magnetic storage medium relative to one another and to the surrounding materials at the air-bearing surface (ABS) and the medium itself can vary, causing electrochemical-plating effects, and other electrochemical effects. By comparison, in the claimed invention, these mid-point voltages, particularly the mid-point voltages 112 of the sensing elements 102, are made to be equal to one another. Other conductive materials at the ABS can also be set to the same electrical potential as the mid-points of the elements, or at some fixed value relative to the mid-point voltage of the elements, in a similar manner as has been described in relation to the sensing elements themselves. However, fixed rather than variable resistors may be used, and the resistance values may be much larger, on the order of one-thousand to ten-million ohms. As such, electrochemical-plating effects, and other electrochemical effects, are substantially reduced or eliminated. However, the currents 110 flowing through the sensing elements 102 are nevertheless independently variable via the present invention, so that optimal sensing of the magnetic storage medium by the sensing elements 102 can still be achieved.
It is noted that, although specific embodiments have been illustrated and described herein, it will be appreciated by those of ordinary skill in the art that any arrangement calculated to achieve the same purpose may be substituted for the specific embodiments shown. This application is thus intended to cover any adaptations or variations of embodiments of the present invention. Therefore, it is manifestly intended that this invention be limited only by the claims and equivalents thereof.