Abstract:
The present invention achieves technical advantages as an improved Parallel Damping scheme suitable for very-low-supply preamp operation. The improved Parallel Damping Scheme accurately generates a programmable Iw flowing through the write head while compensating for a leakage current path through a Parallel Damping resistor.

Description:
FIELD OF THE INVENTION 
   The present invention is generally related to hard disk drives (HDDs), and more particularly to damping out head current ringing. 
   BACKGROUND OF THE INVENTION 
   A writer in a hard disk drive (HDD) preamplifier drives an inductive head by passing a write current (Iw) from the writer to the head. Current Iw toggles between +Iw and −Iw values as consecutive one&#39;s are written on the disk. If there is impedance mismatch between the writer output and the head, ringing in the Iw waveforms occurs when current Iw is settling after switching state. Customarily, there are two methods of “damping” out the Iw ringing. However, there are pros and cons associated with each method. 
   Conventional Methods 
   (1) Series Damping ( FIG. 1 ): 
   Two resistors Rs are added at the output of the “H-bridge” writer. In general, Rs&gt;Rh, where Rh is the write head resistance. For a low CLK signal, transistors M 1  and M 4  are turned on, and thus current Iw flows in the direction shown in the diagram. Transistors M 2  and M 3  are turned off during this time. During the next Iw cycle (with a high CLK signal), current Iw flows in the reverse direction. 
   Pros: If a large VDD is available, Iw=Iwref. In this way, a predictable Iw current value flows through the head because there is only one path for Iw to flow when it goes from transistor M 1  to M 4 . 
   Cons: Loss of voltage headroom due to the voltage potential developed across the two Rs, given by ΔV=2Rs*Iw. As a result, Iw&lt;Iwref due to channel modulation effect on transistors M 5  and M 6  caused by reduced Vds. In an extreme case, transistors M 5  and M 6  enter into triode region of operation. Then, these transistors cease to be true output current mirror devices for MREF; thus, Iw&lt;&lt;Iwref. 
   (2) Parallel Damping ( FIG. 2 ): 
   Iw ringing can also be tamed by a resistor Rp placed in parallel with the head. Note that, in general, Rp&gt;&gt;Rh. 
   Pros: No “additional” voltage drop across the damping resistor Rp. 
   Cons: Part of current Iw, denoted by current Iw 2 , now flows through resistor Rp, i.e., current flowing through the head is no longer Iw, but Iw 1 =Iw−Iw 2 , where Iw 1 &gt;&gt;Iw 2 . To a first order: 
   
     
       
         
           
             
               
                 
                   Iw2 
                   Iw1 
                 
                 = 
                 
                   Rh 
                   Rp 
                 
               
             
             
               
                 EQ 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 
                   ( 
                   1 
                   ) 
                 
               
             
           
         
       
     
   
   Note that the current loss of Iw 2  is also a function of the silicon wafer process due to inherent process variation of Rp. Because Rp is an internal on-chip resistor, while resistor Rh comes from an external “head” component, the Iw 1 -to-Iw 2  ratio will change with process. As a result, the unpredictability of Iw 1  will add uncertainty and cause degradation to the write process. 
   A schematic of one conventional DAC implementation establishing write current Iw is shown in  FIG. 3 . 
   SUMMARY OF THE INVENTION 
   The present invention achieves technical advantages as an improved Parallel Damping scheme suitable for very-low-supply preamp operation. The improved Parallel Damping Scheme accurately generates a programmable Iw flowing through the write head while compensating for a leakage current path through a Parallel Damping resistor. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1  is a schematic of a prior art H-bridge writer with series damping; 
       FIG. 2  is a schematic of a prior art H-bridge writer with parallel damping; 
       FIG. 3  is a schematic of a prior art DAC implementation of the circuit of  FIG. 1 ; 
       FIG. 4  is a schematic of the present invention including improved parallel damping; 
       FIG. 5  is a schematic of a DAC implementation of the invention depicted in  FIG. 4 ; 
       FIG. 6  is a graph depicting the Iw waveform of the present invention compared to the Iw waveform of the prior art approaches of a No Damping case and of  FIG. 2 ; 
       FIG. 7  is a graph the prior art parallel damping approach for different currents Iw and for two extreme resistor Rint process variations; and 
       FIG. 8  is a graph depicting the current Iw according to the present invention for different currents Iw and for two extreme resistor Rint process variations. 
   

   DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT 
   The Case for Parallel Damping 
   For a high-end preamp design where a total supply voltage of 10 V is available to operate the writer, the design can afford to tolerate some loss in voltage drop associated with the Series Damping scheme. For example, 2*Rs could be 60Ω. When the Rs&#39;s are coupled with an Iw range of 20 to 60 mA, there can be 1.2V to 3.6V of voltage headroom loss. 
   However, for low-voltage ultra-portable applications, such as the MicroDrive, the available voltage to the preamp can be as low as 2.7 V. It can be appreciated that any appreciable amount of voltage drop due to Rs will impact the writer performance substantially. Therefore, in a very low supply-voltage environment, the Parallel Damping scheme becomes very attractive. However, the write current flowing through the head has to be predictable and stable for the scheme to become viable. 
   Referring to  FIG. 4 , there is shown an H-bridge write circuit at  10  according to a preferred embodiment of the present invention. Circuit  10  provides an improved Parallel Damping Scheme including a programmable write current Iw, and at least three (3) advantageous features. 
   First feature: More current, ΔIw, is injected to the writer to make up for the current loss through resistor Rp. The idea is to force Iw through Rh and ΔIw through Rp. 
   Second feature: According to EQ (1), with Iw 1 =Iw and Iw 2 =ΔIw, ΔIw is scaled with Iw to maintain a constant Rh-to-Rp ratio. 
   Third feature: According to EQ(1), ΔIw is inversely proportional to Rp to take care of Rp variations due to process changes. 
   According to one preferred embodiment, as shown in  FIG. 5 , the programmable Iw is obtained by feeding the output of a current digital-to-analog converter (DAC) to the H-bridge writer circuit  10  such that
 
 Iw (old)= N*I ( lsb )+ Iwo   EQ(2)
 
where I(lsb) is the Iw least significant bit (of the binary DAC code; hereinafter, “LSB”) current, N is the decimal equivalent of the binary DAC code, and Iwo is the “residue” Iw independent of DAC code. Both I (lsb) and Iwo are derived from the IREF such as shown in  FIGS. 1–3 . Note that Iw scales with N.
 
   According to the present invention, the Iw DAC equation is modified to be: 
                   Iw   ⁡     (   new   )       =       N   *     (       I   ⁡     (     1   ⁢   sb     )       +     k1   *     VBG   Rint         )       +     (     Iw0   +     k0   *     VBG   Rint         )               EQ   ⁢           ⁢     (   3   )                 
where VBG is a process-insensitive voltage derived from a Bandgap Voltage Reference, Rint is an on-chip resistor of the same type as Rp, and k 0 =Iw 0 /IREF and k 1 =I(lsb)/IREF are fixed ratios of device W/L&#39;s. EQ(3) can be re-written as follows:
 
   
     
       
         
           
             
               
                 
                   
                     Iw 
                     ⁡ 
                     
                       ( 
                       new 
                       ) 
                     
                   
                   = 
                   
                     
                       Iw 
                       ⁡ 
                       
                         ( 
                         old 
                         ) 
                       
                     
                     + 
                     
                       Δ 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       Iw 
                     
                   
                 
                 ⁢ 
                 
                   
 
                 
                 ⁢ 
                 
                   where 
                   ⁢ 
                   
                     : 
                   
                 
               
             
             
               
                 EQ 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 
                   ( 
                   4 
                   ) 
                 
               
             
           
           
             
               
                 
                   Δ 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   Iw 
                 
                 = 
                 
                   
                     ( 
                     
                       
                         N 
                         * 
                         k1 
                       
                       + 
                       k0 
                     
                     ) 
                   
                   * 
                   
                     VBG 
                     Rint 
                   
                 
               
             
             
               
                 EQ 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 
                   ( 
                   5 
                   ) 
                 
               
             
           
         
       
     
   
   It can be seen that more write current is fed into Rh//Rp in the improved design of  FIGS. 4 and 5 . This is true for both N=0 and finite N cases. Thus, RHS of EQ (5) contains the term (N*k 1 +k 0 ) to ensure additional write current for all valid N values. In conclusion, EQ (5) gives an ΔIw providing the three features. 
     FIG. 5  shows a modified DAC circuit  20  providing Iw(new) according to the present invention providing the improved parallel damping scheme. From now on, the improved scheme will be referred to as “Parallel Damping with Iw Correction.” 
   In  FIG. 5 , Rint is also shown as a variable resistor to allow for fine tuning of its value to account for different Rh value. The programmable Rint can easily be implemented as a digitally-controlled programmable resistor array. 
   One negative aspect of the improved scheme of  FIG. 4  is more power dissipation when compared to a Parallel Damping scheme without Iw Correction. 
   SIMULATION RESULTS: A prior-art writer with Current Boost was set up. The writer was loaded with Rh=10Ω and Lh of 30 nH. Rp=60Ω in this example.  FIG. 6  shows three Iw waveforms: i) No damping at  30 ; ii) Prior-art Parallel Damping at  32 ; and iii) Improved Parallel Damping of the present invention, shown at  34 . Note that the “Parallel Damping with Iw Correction” waveform  34  restores the current loss due to the parallel Rp path. 
   Three different Iw settings with resistor process variations have been simulated.  FIG. 7  shows the case for Parallel Damping w/o Iw Correction, while  FIG. 8  shows the case for Parallel Damping with Iw Correction according to the present invention. 
   For  FIGS. 7 and 8 , the target Iw settings are 59.9, 39.5 and 15.9 mA. As can be seen, the resultant Iw values are much closer to the targets as shown in  FIG. 8  versus  FIG. 7 . As expected, Iw variations due to resistor process change are narrower in  FIG. 8 , especially so for higher Iw settings. Table 1 shows steady-state Iw values for three Iw settings and two resistor process conditions. 
   
     
       
             
             
             
             
           
         
             
               TABLE 1 
             
             
                 
             
             
                 
               Resistor 
               Parallel Damping 
                 
             
             
                 
               Process 
               without Iw 
               Parallel Damping 
             
             
               Iw Setting 
               Condition 
               Correction 
               with Iw Correction 
             
             
                 
             
           
           
             
               Iw = 59.9 mA 
               Strong 
               50.85 mA 
               60.07 mA 
             
             
                 
               Weak 
               52.05 mA 
               59.25 mA 
             
             
               Iw = 39.5 mA 
               Strong 
               33.45 mA 
               39.46 mA 
             
             
                 
               Weak 
               34.24 mA 
               38.93 mA 
             
             
               Iw = 15.9 mA 
               Strong 
               13.38 mA 
               15.74 mA 
             
             
                 
               Weak 
               13.70 mA 
               15.53 mA 
             
             
                 
             
           
        
       
     
   
   Though the invention has been described with respect to a specific preferred embodiment, many variations and modifications will become apparent to those skilled in the art upon reading the present application. It is therefore the intention that the appended claims be interpreted as broadly as possible in view of the prior art to include all such variations and modifications.