Abstract:
A vehicle may include an electric machine that generates motive power for the vehicle, a plurality of cells that store energy for the electric machine, and at least one controller. The at least one controller may cause the cells to receive current for a period of time and, during the period of time, cause at least some of the cells to supply cell load current such that at the expiration of the period of time, the amount of energy stored by the cells is at least equal to a predetermined target energy level.

Description:
BACKGROUND 
     Vehicle battery rebalancing is performed to correct cell voltage imbalance conditions. The voltage of each of the cells is measured and the cell having the minimum voltage identified. All other cells are bled down via resistive circuitry associated with each cell until the other cells have a measured voltage approximately equal to the minimum. Continuous/periodic cell voltage measurements are taken during the bleed down process to monitor change in the cell voltages. Once all of the cell voltage readings are approximately equal, the battery is charged. 
     SUMMARY 
     A method for charging a vehicle battery including a plurality of cells may include causing the cells to receive current for a period of time and during the period of time, causing at least some of the cells to supply cell load current such that at the expiration of the period of time, the capacity in each of the cells is approximately equal. 
     A power system may include a plurality of cells and at least one controller configured to cause the cells to acquire charge for a period of time such that at the expiration of the period of time, the amount of Amp-hrs stored by each of the cells is approximately equal. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  is a schematic diagram of a battery cell and its resistive circuitry. 
         FIG. 2  is a block diagram of an alternatively powered vehicle. 
         FIG. 3  is a flow chart illustrating an algorithm for determining times associated with rebalancing/charging the battery of  FIG. 2 . 
         FIGS. 4A and 4B  are flow charts illustrating an algorithm for rebalancing/charging the battery of  FIG. 2 . 
     
    
    
     DETAILED DESCRIPTION 
     A manufacturer of alternatively powered vehicles (e.g., battery electric vehicles, etc.) may desire to provide vehicles that can be driven for a specified range after battery rebalancing/charging. The drive range of a battery powered vehicle depends on the amount of available energy stored by its battery. Conventional techniques for battery rebalancing attempt to make the battery cell voltages equal before charging the battery cells to a target voltage. For a given cell voltage, however, cell energy content can decrease over time due to cell aging. Hence, the amount of energy stored by the battery (and thus vehicle drive range) can decrease over time if the cells continue to be charged to the same target voltage. 
     Certain embodiments disclosed herein may provide systems and techniques that balance/charge a battery to achieve a specified vehicle drive range. 
     Cell Capacity 
     A battery cell&#39;s maximum capacity, Ihr max , may be found according to the relationship 
                     Ihr     ma   ⁢           ⁢   x       =       Δ   ⁢           ⁢   Ihr       Δ   ⁢           ⁢   SOC               (   1   )               
where ΔIhr is the change in capacity in the cell and ΔSOC is the change in state of charge of the cell. As an example, the SOC of a given cell may be determined before and after 1 A·hr of capacity is provided to it. Assuming a ΔSOC of 10% for this example, the cell&#39;s maximum capacity, Ihr max , would be 10 Amp-hrs according to (1).
 
Cell Energy Content
 
     A battery cell&#39;s energy content, ε, may be approximated from the following sets of equations
 
ε=∫ρ· dt   (2)
 
where ρ is the power applied to the cell over time. ρ may be written as
 
ρ= v   m   ·i   (3)
 
where v m  is the (measured) voltage associated with the power stored and i is the current associated with the power stored. Substituting (3) into (2) yields
 
ε=∫ v   m   ·i·dt   (4)
 
v m  may be written as
 
 v   m   =Δv+v   min   (5)
 
where v min  is the voltage of the cell at 0% state of charge (e.g., 3.1 V) and Δv is the difference between the voltage associated with the power stored and the voltage of the cell at 0% state of charge. Substituting (5) into (4) yields
 
ε=∫(Δ v+v   min ) idt   (6)
 
Δv may be written as
 
                     Δ   ⁢           ⁢   v     =     i   ·         v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr     ma   ⁢           ⁢   x         ·   t             (   7   )               
where v max  is the voltage of the cell at full state of charge, Ihr max  is the cell&#39;s maximum capacity, and t is the time over which the change in voltage occurs. Substituting (7) into (6) yields
 
                   ε   =     ∫       (       (     i   ·         v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr     ma   ⁢           ⁢   x         ·   t     )     +     v     m   ⁢           ⁢   i   ⁢           ⁢   n         )     ⁢   i   ⁢     ⅆ   t                 (   8   )               
Integrating (8) yields
 
                   ε   =         i   2     ·         v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr     ma   ⁢           ⁢   x         ·       t   2     2       +       v     m   ⁢           ⁢   i   ⁢           ⁢   n       ·   i   ·   t               (   9   )               
i·t may be written as
 
 i·t=Ihr   (10)
 
which is the capacity in the cell. Substituting (10) into (9) yields
 
                   ε   =             v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr     ma   ⁢           ⁢   x         ·       Ihr   2     2       +       v     m   ⁢           ⁢   i   ⁢           ⁢   n       ·   Ihr               (   11   )               
Cell Capacity Needed to Provide Specified Energy Content
 
     Assume, for example, that a battery pack includes a string of cells each with a different Amp-hr capacity due to manufacturing tolerances, age, temperature, etc. The same current would pass through all of the cells during a subsequent discharge of the series string. From (7), the cells with lesser Amp-hr capacity at the start of discharge would have greater cell voltages compared to those with greater Amp-hr capacity when charged to the same Amp-hrs. From (11), it can be seen that given two cells with the same number of Amp-hrs stored (the first with greater Amp-hrs maximum capability compared with the second), the second will deliver more energy if both are discharged. 
     Now assume, for example, that a given battery pack having 20 cells needs to store at least 30 kW·hrs of energy to support a drive range of 100 miles. That is, the sum of energies stored by the cells of the battery pack should be at least equal to 30 kW·hrs. (11) may then be evaluated for each of the cells. An initial value (e.g., 1 A·hr) for Ihr may be assumed, v max  and v min  are known by design, and Ihr max  can be determined from (1). If the sum of the cell energies is less than, in this example, 30 kW·hrs, the value for Ihr may be incremented by, for example, 1 A·hr and (11) evaluated again for each of the cells iteratively until the sum of the cell energies is at least equal to 30 kW·hrs. The capacity value resulting in the sum of the cell energies being at least equal to 30 kW·hrs is the target cell capacity value. 
     Total Battery Pack Charge Time 
     Ihr from (11) may be written as
 
 Ihr=ΔIhr+Ihr   initial   (12)
 
where Ihr initial  is the initial capacity in the cell (before cell balancing/charging) and Ihr is the difference in capacity in the cell before cell balancing/charging and after cell balancing/charging (to the target Ihr value). Ihr initial  is proportional to the measured voltage of the cell. Hence, a look-up table mapping values of cell voltage to Ihr may be used to determine Ihr initial  based on the initial measured cell voltage. ((7) may also be used to find the initial capacity by solving for i·t (cell capacity) and setting Lv equal to the measured voltage of a particular cell). Ihr for each cell may thus be found from (12).
 
     The total charge time, t c , (or time during which the cells are to receive current) for a battery pack may be found according to 
                     t   c     =       Δ   ⁢           ⁢     Ihr     ma   ⁢           ⁢   x           i   chg               (   13   )               
where ΔIhr max  is the maximum of the ΔIhr values determined from (12) and i chg  is the charge current of the pack.
 
Cell Resistive Circuitry Activation Time
 
     The duration of time, t R     —     act , during which a cell&#39;s resistive circuitry may be activated to cause the cell to supply a cell load current while the cell is receiving current (assuming t c  is greater than t R     —     act ) to achieve the target capacity may be found from the following sets of equations 
                     i     hr   ⁢     -     ⁢   bleed       =     ∫         v   cell     R     ·     ⅆ   t                 (   14   )               
where i hr-bleed  is the discharge Amp-hrs associated with the cell&#39;s resistive circuitry when activated, v cell  is the cell voltage, and R is the resistance of the cell&#39;s resistive circuitry. v cell  may be written as
 
                     v   cell     =           v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr     ma   ⁢           ⁢   x         ·   Ihr             (   15   )               
where v max  is the voltage of the cell at full state of charge, v min  is the voltage of the cell at 0% state of charge, Ihr max  is the cell&#39;s maximum capacity, and Ihr is the capacity in the cell. Substituting (15) into (14) and integrating yields
 
                     i     hr   ⁢     -     ⁢   bleed       =               v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr       ma   ⁢           ⁢   x     ⁢                 ·   Ihr     R     ·     t     R   ⁢           ⁢   _   ⁢           ⁢   act                 (   16   )               
Rearranging (16) yields
 
                     t     R   ⁢           ⁢   _   ⁢           ⁢   act       =         i     hr   ⁢     -     ⁢   bleed       ·   R             v     ma   ⁢           ⁢   x       -     v     m   ⁢           ⁢   i   ⁢           ⁢   n           Ihr     ma   ⁢           ⁢   x         ·   Ihr               (   17   )               
i hr-bleed , R, v max  and v min  are known by design, Ihr max  can be determined for each cell from (1), and Ihr can be found from (11) as discussed above.
 
Cell Energy Content Balancing/Charging
 
     Referring to  FIG. 2 , an embodiment of a plug-in hybrid electric vehicle (PHEV)  10  may include an engine  12 , a plurality of cells  8  forming a traction battery  14 , battery charger  15  and electric machine  16 . The PHEV  10  may also include a transmission  18 , wheels  20 , controller(s)  22 , and electrical port  24 . 
     The engine  12 , electric machine  16  and wheels  20  are mechanically connected with the transmission  18  (as indicated by thick lines) in any suitable/known fashion such that the engine  12  and/or electric machine  16  may drive the wheels  20 , the engine  12  and/or wheels  20  may drive the electric machine  16 , and the electric machine  16  may drive the engine  12 . Other configurations, such as a battery electric vehicle (BEV) configuration, etc., are also possible. 
     The battery  14  may provide energy to or receive energy from the electric machine  16  (as indicated by dashed line). The battery  14  may also receive energy from a utility grid or other electrical source (not shown) via the electrical port  24  and battery charger  15  (as indicated by dashed line). 
     The controller(s)  22  are in communication with and/or control the engine  12 , battery  14 , battery charger  15 , electric machine  16 , and transmission  18  (as indicated by thin lines). 
     Referring to  FIGS. 2 and 3 , the controller(s)  22  may determine (e.g., measure, read, etc.) the voltages of each of the cells  8  at operation  28 . At operation  30 , the controllers  22  may determine the maximum capacity of each of the cells  8  using, for example, the techniques described with respect to (1). At operation  32 , the controller(s)  22  may determine the Amp-hrs needed in each of the cells to support a target drive range using, for example, the techniques described with respect to (11). At operation  34 , the controller(s)  22  may determine the charge time for the battery pack  14  using, for example, the techniques described with respect to (13). At operation  36 , the controller(s)  22  may determine each of the cell&#39;s resistive circuitry activation time using, for example, the techniques described with respect to (17). 
     Referring to  FIGS. 2 and 4A , the controller(s)  22  may determine, at operation  38  whether the pack charge time determined at operation  34  ( FIG. 3 ) is greater than the maximum of the resistive circuitry activation times determined at operation  36  ( FIG. 3 ). If no, the controller(s)  22  may first balance and then charge the cells  8  of the battery pack  14  at operation  40  using any suitable/known technique. If yes, referring to  FIGS. 2 and 4B , the controller(s)  22  may activate, for each of the cells  8 , the resistive circuitry and enable the battery charger  15  at operation  42 . At operation  44 , the controller(s)  22  may determine whether, for each of the cells  8 , the cell&#39;s resistive circuitry activation time has expired. If no, the algorithm returns to operation  44 . That is, for any of the cells  8  whose resistive circuitry activation time has yet to expire, the algorithm returns to operation  44 . If yes, the controller(s)  22  may deactivate the cell resistive circuitry at operation  46 . That is, for any of the cells  8  whose resistive circuitry activation time has expired, the controller(s)  22  may deactivate their resistive circuitry. 
     Once the resistive circuitry for all of the cells  8  has been deactivated, the controller(s)  22 , at operation  48 , may determine whether the battery pack charge time has expired. If no, the algorithm returns to operation  48 . If yes, the algorithm may disable the battery charger  15  at operation  50 . The cells  8  of the battery pack  14  have thus been balanced/charged to a target capacity sufficient to support a desired drive range. 
     The algorithms disclosed herein may be deliverable to/implemented by a processing device, such as the battery charger  15  or controller(s)  22 , which may include any existing electronic control unit or dedicated electronic control unit, in many forms including, but not limited to, information permanently stored on non-writable storage media such as ROM devices and information alterably stored on writeable storage media such as floppy disks, magnetic tapes, CDs, RAM devices, and other magnetic and optical media. The algorithms may also be implemented in a software executable object. Alternatively, the algorithms may be embodied in whole or in part using suitable hardware components, such as Application Specific Integrated Circuits (ASICs), Field-Programmable Gate Arrays (FPGAs), state machines, or other hardware components or devices, or a combination of hardware, software and firmware components. 
     While embodiments of the invention have been illustrated and described, it is not intended that these embodiments illustrate and describe all possible forms of the invention. The words used in the specification are words of description rather than limitation, and it is understood that various changes may be made without departing from the spirit and scope of the invention.