• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    INTERNAL BATTERY RESISTANCE MEASURING DEVICE ON LAYERS. This layered internal battery resistance meter is supplied with: an AC power supply unit to send an AC current to an internal resistance measurement device connected to the AC power supply unit, the internal resistance meter including at least one layered battery comprising a plurality of generating elements: an AC adjustment unit for adjusting the AC current so that a positive pole side AC potential difference which is a potential difference determined by subtracting a potential of an intermediate part of a potential in a part of the measured object of internal resistance that is connected to a charging device on one side of the positive pole, corresponds to a potential difference AC of the negative pole side which is a potential difference determined by subtracting the potential of the intermediate part of a potential in a part of the measured object of internal resistance that is connected to the charging device on one side of the negative pole; and a resistance calculation unit to calculate the resistance of the battery (...).
    公开号:BR112013014482B1
    申请号:R112013014482-3
    申请日:2011-11-09
    公开日:2020-12-22
    发明作者:Tetsuya Kamihara；Masanobu Sakai
    申请人:Nissan Motor Co., Ltd.；
    IPC主号:
    专利说明:

    Technical Field
    [001] The present description refers to a device and a method for measuring the internal resistance of a stacked battery in which a plurality of power generation elements are stacked. Fundamental Technique
    [002] In a layered battery in which a plurality of power generation elements are stacked, it is desirable to detect the internal resistance as precisely as possible. For example, in a fuel cell, the wetting capacity of an electrolytic membrane can be determined by understanding the internal resistance. High internal resistance is associated with low wetting capacity of an electrolytic membrane with a tendency to dry out. Low internal resistance is associated with high wetting capacity of an electrolytic membrane. The operating efficiency of the fuel cell varies depending on the wetting capacity of an electrolytic membrane. Therefore, an ideal wet state of an electrolytic membrane can be maintained constantly by the control operation according to the wetting capacity of the electrolytic membrane as estimated based on the internal resistance.
    [003] A device for measuring the internal resistance of a fuel cell is described in JP-2009-109375-A. summary
    [004] However, the device according to JP-2009-109375-A requires a charging current (DC) flowing from the cell during the measurement so that measurement is not possible unless the cell is in operation. In addition, even an AC current is controlled (or the current supply is limited) by an electronic charging device that controls a large DC current, where an extremely large dynamic range is required. Therefore, the components and circuit specification to be used are expensive.
    [005] The present description has been achieved by focusing attention on such conventional problems. The present description aims to provide a cheap internal resistance measurement device and a cheap internal resistance measurement method capable of measuring internal resistance even when a battery is not in operation.
    [006] An internal resistance measurement device for a stacked battery according to an embodiment of the present invention includes an AC power supply part that sends an AC current to an internal resistance measurement object comprising a stacked battery containing a plurality of stacked power generation elements being connected to the internal resistance measurement object. Then, the internal resistance measuring device additionally includes a positive portion connected to a positive electrode of the internal resistance measuring object, a negative portion connected to a negative electrode of the internal resistance measuring object, an intermediate portion connected to a part intermediate of the internal resistance measurement object, an AC adjustment part to adjust an output AC current for the positive electrode and the negative electrode of the internal resistance measurement object, and a resistance calculation part to calculate the resistance of the battery stacked based on the adjusted AC current and the AC potential difference.
    [007] The modalities of the present invention and the advantages of the present invention will be explained below in detail together with the attached drawings. Brief Description of the Drawings - Figure 1A is an external perspective view to explain a fuel cell serving as an example of a stacked battery to which an internal resistance measurement device according to the present invention is applied; Figure 1B is an exploded view illustrating a fuel cell power generation cell structure serving as an example of the stacked battery to which the internal resistance measurement device according to the present invention is applied; Figure 2 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to a first embodiment of the present invention; Figure 3 is a view to explain the details of a positive electrode DC interruption part 511, a negative electrode DC interruption part 512, a midpoint DC interruption part 513, a difference detection part positive electrode AC potential 521 and a negative electrode AC potential difference detection part 522; Figure 4 is a view to explain the details of a positive electrode power supply part 531 and a negative electrode power supply part 532; - Figure 5 is a view to explain the details of an adjustment part CA 540; - Figure 6 is a view to explain the details of a resistance calculation part 550; Figure 7 is a control flow chart to be performed by a controller on the internal resistance measurement device for stacked batteries according to the first embodiment of the present invention; - Figure 8 is a graph of time obtained when a control is made by the controller in the internal resistance measurement device for the stacked battery according to the present invention; - Figure 9 is a view to explain an action effect of the first modality; Figure 10A is a view to explain the mechanism of an action effect of an internal resistance measurement device for the stacked battery according to a second embodiment of the present invention; Figure 10B is a view to explain a mechanism of an action effect of the internal resistance measuring device for the stacked battery according to the second embodiment of the present invention; - Figure 11 illustrates a concrete structure of the second modality; Figure 12 is a circuit diagram illustrating the internal resistance measurement device for the stacked battery according to the second embodiment of the present invention; Figure 13 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to a third embodiment of the present invention; Figure 14 is a control flow chart to be performed by a controller on the internal resistance measurement device for the stacked battery according to the third embodiment of the present invention; Figure 15 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to a fourth embodiment of the present invention; Figure 16 illustrates an internal resistance measurement device for the stacked battery according to a fifth embodiment of the present invention; Figure 17 illustrates an internal resistance measurement device for the stacked battery according to a sixth embodiment of the present invention; - Figure 18 is a concrete circuit diagram of the sixth modality; Figure 19 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to a seventh embodiment of the present invention; Figure 20 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to an eighth embodiment of the present invention; - Figure 21A illustrates a first modified modality; - Figure 21B illustrates a second modified modality. Modalities First Mode
    [008] Figure 1A is an external perspective view to explain a fuel cell as an example of a stacked battery to which an internal resistance measurement device according to the present invention is applied. Figure 1B is an exploded view to explain the fuel cell power generation cells serving as an example of the stacked battery to which the internal resistance measurement device according to the present invention is applied.
    [009] As illustrated in figure 1A, a fuel cell stack 1 is provided with a plurality of stacked power generation cells 10, current collection plates 20, insulating plates 30, end plates 40 and four tension rods 50 .
    [0010] The power generation cells 10 are unit cells of the fuel cell. Each of the power generation cells 10 generates an electromotive voltage of about 1 volt. A detailed structure of each of the power generation cells 10 will be explained later.
    [0011] The current collection plates 20 are arranged on the outside of the plurality of stacked power generation cells 10. The current collection plates 20 are formed by a conductive gas impermeable element such as, for example, compact carbon . Current collection plates 20 include a positive electrode terminal 211 and a negative electrode terminal 212. There is also an intermediate terminal 213 provided between the positive electrode terminal 211 and the negative electrode terminal 212. In the fuel cell stack 1 , an electron is generated in each of the power generation cells 10 is extracted and sent by the positive electrode terminal 211 and the negative electrode terminal 212.
    [0012] The insulating plates 30 are arranged on the outside of the current collection plates 20. The insulating plates 30 are formed by an insulating element such as, for example, rubber.
    [0013] The end plates 40 are arranged on the outside of the insulating plates 30. The end plates 40 are formed by a rigid metallic material, such as, for example, steel.
    [0014] Arranged on one of the end plates 40 (that is, the end plate 40 on the left side facing forward in figure 1A) are an anode supply port 41a, an anode discharge port 41b, an cathode supply port 42a, cathode discharge port 42b, cooling water supply port 43a, and cooling water discharge port 43b. In the present embodiment, the anode discharge port 41b, the cooling water discharge port 43b and the cathode supply port 42a are arranged on the right side in figure 1A. The cathode discharge port 42b, the cooling water supply port 43a and the anode supply port 41a are also arranged on the right side in figure 1A.
    [0015] The tension rods 50 are arranged close to the four corners of the end plate 40. The fuel cell stack 1 is formed with holes (not shown) penetrating through the interior of the same. The tension rods 50 are inserted into the hollow holes. The tension rods 50 are formed of a rigid metal material such as, for example, steel. The insulating treatment is applied to the surface of the tension rods 50 in order to avoid an electrical short circuit between the power generation cells 10. The tension rods 50 are bolted with nuts (not illustrated because they are located inside). The fuel cell stack 1 is tightened in a stacking direction by tension rods 50 and nuts.
    [0016] Examples of a method for supplying hydrogen serving as an anode gas for anode supply port 41a include a method for directly supplying a hydrogen gas from a hydrogen storage device and a method of supply of a hydrogen-containing gas reformed by reforming a hydrogen-containing fuel. Note that the hydrogen storage device is carried out by a high pressure gas tank, liquefied hydrogen tank and hydrogen storage alloy tank or other tanks. Hydrogen-containing fuel includes natural gas, methanol, gasoline and the like. Air is also used in general as a cathode gas supplied to the cathode supply port 42a.
    [0017] As illustrated in figure 1B, each of the power generation cells 10 is structured by the arrangement of an anode separator (or bipolar anode plate) 12a and a cathode separator (or bipolar cathode plate) 12b in both the surfaces of a MEA (Membrane Electrode Assembly) 11.
    [0018] MEA 11 is supplied with electrode catalyst layers 112 on both sides of an electrolytic membrane 111 made of an ion exchange membrane. GDL (gas diffusion layer) 113 is formed in each of the electrode catalyst layers 112.
    [0019] The electrode catalyst layers 112 are formed, for example, by carbon black particles bearing platinum.
    [0020] GDLs 113 are formed by an element with sufficient diffusion capacity and gas conduction such as, for example, carbon fibers.
    [0021] An anode gas supplied from anode supply port 41a flows through GDL 113a and reacts to the anode electrode catalyst layer 112 (i.e., 112a), followed by discharge from the discharge port anode 41b.
    [0022] A cathode gas supplied from cathode supply port 42a flows through GDL 113b and reacts with the cathode electrode catalyst layer 112 (i.e., 112b), followed by discharge from the discharge port cathode 42b.
    [0023] The anode separator 12a is stacked on one side of the MEA 11 (that is, the rear side of it in figure 1B) through GDL 113a and a seal 14a. The cathode separator 12b is stacked on one side of the MEA 11 (i.e., the front side of it in figure 1B) through GDL 113b and a seal 14b. The seals 14 (i.e., 14a and 14b) are made of an elastic rubber material such as, for example, silicone, rubber, EPDM (ethylene propylene diene monomer) and fluoroborch. Each of the anode separators 12a and cathode 12b is formed by pressure molding a separating substrate made of metal such as, for example, stainless metal and including a reactive gas flow path formed on one side and an air flow path. cooling water formed on the opposite side of it in order to run in parallel with the flow path of the reaction gas. As illustrated in figure 1B, anode separator 12a and cathode separator 12b are stacked together to form a cooling water flow path.
    [0024] Each of MEA 11, anode separator 12a and cathode separator 12b is formed with holes 41a, 41b, 42a, 42b, 43a and 43b and these holes are stacked together to form the anode supply port ( or anode supply pipe) 41a, anode discharge port (anode discharge pipe) 41b, cathode supply port (cathode supply pipe) 42a, cathode discharge port (or cathode discharge pipe) 42b, the cooling water supply port (or cooling water supply pipe) 43a and the cooling water discharge port (or cooling water discharge pipe) 43b.
    [0025] Figure 2 is a circuit illustrating an internal resistance measurement device for the stacked battery according to a first embodiment of the present invention.
    [0026] An internal resistance measuring device 5 includes a positive electrode DC break part 511, a negative electrode DC break part 512, a midpoint DC break part 513, a power difference detection part Positive electrode AC 521, a negative electrode potential difference detection part 522, a positive electrode power supply part 531, a negative electrode power supply part 532, an AC adjustment part 540 and a resistance calculation part 550.
    [0027] Details of the positive electrode DC interrupting part 511, negative electrode DC interrupting part 512, intermediate point DC interruption part 513, positive electrode AC potential difference detection part 521, and part detection difference in AC potential of negative electrode 522 will be explained with reference to figure 3.
    [0028] Fuel cell 1 is the object for measuring internal resistance. The positive electrode DC break part 511 is connected to a positive electrode terminal 211 of a fuel cell 1. In addition, the positive electrode terminal 211 is connected to a positive electrode of a charging device 3 via a connection on the line 4. The negative electrode DC break part 512 is connected to a negative electrode terminal 212 of the fuel cell 1. In addition, the negative electrode terminal 212 is connected to a negative electrode of a charging device 3 via a connection on line 4. Intermediate DC interruption part 513 is connected to an intermediate terminal 213 of the fuel cell 1. Note that the intermediate DC interruption part 513 may not be provided as illustrated by an interrupted line on the figure 2. These DC interrupt parts interrupt DC, but allow AC to flow. The DC interruption parts are made, for example, by capacitors and transformers.
    [0029] The positive electrode difference detection part of the positive electrode 521 sends a difference in AC power by receiving the AC potential Va at the positive electrode terminal 211 of the fuel cell 1 and the AC potential Vc at the intermediate terminal 213. The part Negative electrode AC potential difference detection method 522 sends an AC potential difference by receiving the AC potential Vb at the negative terminal 212 of the fuel cell 1 and the AC potential Vc from the intermediate terminal 213 thereof. The positive electrode AC potential difference detection part 521 and the negative electrode AC potential difference detection part 522 are performed, for example, by differential amplifiers (or instrumentation amplifiers).
    [0030] Details of the positive electrode power supply part 531 and the negative electrode power supply part 532 will be explained with reference to figure 4.
    [0031] The positive electrode 531 power supply part can be performed, for example, by a voltage / current conversion circuit made of operational amplifiers (OP amplifiers) as illustrated in figure 4. According to this circuit, a current Io that is proportional to an input voltage Vi is sent. Note that Io is obtained by dividing Vi by Rs which is a current sensor resistor. That is, this circuit is a variable AC current source that is able to adjust the output current Io by the input voltage Vi.
    [0032] It is possible with the use of this circuit to obtain the output current Io by dividing the input voltage Vi by the proportionality factor Rs without actual measurement of the output current Io. Furthermore, even if an element that generates a different phase angle such as a capacitor is interleaved in a current path, an AC current flowing through the stacked cell groups is brought into the same phase as an output from the current source since a chain is sent. In addition, the current is also brought into the same phase as the input voltage Vi. Accordingly, the circuit is simplified without the need to consider a phase difference when calculating resistance in a next stage. In addition, even if a capacitor arranged in the current path has a variable impedance, it is not affected by a phase change. Due to these reasons, the circuit as illustrated in figure 4 is preferably used as the positive electrode power supply part 531. The same must apply to the negative electrode power supply part 532.
    [0033] Details of the CA 540 adjustment part will be explained with reference to figure 5.
    [0034] The CA 540 adjustment part can be performed, for example, by a PI control circuit as illustrated in figure 5. The CA 540 adjustment part includes a positive electrode detector circuit 5411, a positive electrode subtraction element 5421, a positive electrode integration circuit 5431, a positive electrode multiplier 5451, a negative electrode detector circuit 5412, a negative electrode subtraction element 5422, a negative electrode integration circuit 5432, a negative electrode multiplier 5452 , a reference voltage 544 and an AC signal source 546.
    [0035] The positive electrode detector circuit 5411 removes an unnecessary signal from the AC potential Va in a wiring of the positive electrode power supply part 531 connected to the positive electrode terminal 211 of the stacked battery 1, and converts it into a signal CC.
    [0036] The positive electrode subtraction element 5421 detects a difference between the DC signal and the reference voltage 544. The positive electrode integration circuit 5431 equalizes a signal sent from the positive electrode subtraction element 5421 or adjust the signal sensitivity.
    [0037] The positive electrode multiplier 5451 modulates the amplitude of the signal source AC 546 by an output of the positive electrode integration circuit 5431.
    [0038] The AC 540 adjustment part thus generates a command signal sent to the positive electrode power supply part 531. The AC 540 adjustment part also generates a command signal sent to the supply electrode part. negative electrode energy 532 in the same way. According to the command signals generated in this way, the outputs of the positive electrode power supply part 531 and the negative electrode power supply part 532 are increased / reduced to control both the AC potential Va and Vb to a level predetermined. Therefore, each of the potential CA Va and Vb becomes equipotential.
    [0039] Note that the circuit configuration illustrated in this example by using an analog arithmetic integrated circuit as an example can also be composed of a digital control circuit after the digital conversion of the potential CA Va (or Vb) by a converter AD.
    [0040] Details of the resistance calculation part 550 will be explained with reference to figure 6.
    [0041] The resistance calculation part 550 includes an AD 551 converter and a 552 micro computer chip.
    [0042] The AD 551 converter converts AC currents (I1, I2) and AC voltages (V1, V2), each of which is an analog signal, into digital numerical value signals to be transferred to the micro computer chip . 552.
    [0043] The 552 micro computer chip pre-stores programs to calculate the internal resistance Rn and the total internal resistance R of the stacked battery. The 552 micro computer chip performs sequential operations at predetermined micro time intervals or sends operating results in response to a request from a controller 6. Note that the internal resistance Rn and all internal resistance R of the stacked battery are calculated by formulas to follow: formula 1 Arithmetic expression for resistance

    [0044] The resistance calculation part 550 can also be performed by an analog arithmetic circuit using an analog arithmetic integrated circuit. According to an analog arithmetic circuit, changes in continuous resistance value in terms of time can be sent.
    [0045] Figure 7 is a control flow chart to be performed by the controller on the internal resistance measurement device for the stacked battery according to the first embodiment of the present invention.
    [0046] In step S1, the controller determines whether or not the positive electrode AC potential Va is greater than a predetermined value. The controller allows the process to move to step S2 when the determination result is negative and allows the process to move to step S3 when the determination result is positive.
    [0047] In step S2, the controller determines whether or not the positive electrode AC potential Va is less than a predetermined value. The controller allows the process to move to step S4 when the determination result is negative or allows the process to move to step S5 when the determination result is positive.
    [0048] In step S3, the controller causes the positive electrode 531 power supply to reduce an output. Therefore, the AC potential of positive Va electrode decreases.
    [0049] In step S4, the controller causes the positive electrode power supply part 531 to maintain an output. Therefore, the positive electrode AC potential Va is maintained.
    [0050] In step S5, the controller causes the positive electrode power supply part 531 to increase an output. Therefore, the positive electrode AC potential Va goes up.
    [0051] In step S6, the controller determines whether or not the negative electrode AC potential Vb is greater than a predetermined value. The controller allows the process to move to step S7 when the determination result is negative or allows the process to move to step S8 when the determination result is positive.
    [0052] In step S7, the controller determines whether or not the negative electrode AC potential Vb is less than a predetermined value. The controller allows the process to move to step S9 when the determination result is negative or allows the process to move to step S10 when the determination result is positive.
    [0053] In step S8, the controller causes the negative electrode 532 power supply to reduce an output. Therefore, the negative electrode AC potential Vb decreases.
    [0054] In step S9, the controller allows the negative electrode power supply part 532 to maintain an output. Therefore, the negative electrode AC potential Vb is maintained.
    [0055] In step S10, the controller causes the negative electrode power supply part 532 to increase an output. Therefore, the negative electrode AC potential Vb goes up.
    [0056] In step S11, the controller determines whether or not the positive electrode AC potential Va and the negative electrode AC potential VB are a predetermined value. The controller allows the process to move to step S12 when the determination result is positive or exits the process when the determination result is negative.
    [0057] In step S12, the controller calculates the resistance values based on the formulas (1-1) and (1-2) above.
    [0058] Figure 8 is a graph of time obtained when the controller performs a control on the internal resistance measurement device for stacked batteries according to the present invention.
    [0059] Note that it will be illustrated together with the step number to facilitate understanding corresponding to the flowchart.
    [0060] In an earlier stage in figure 8, an internal resistance value R1 on the positive electrode side is high and an internal resistance value R2 on the negative electrode side is low (see figure 8A). The controller starts control under this condition.
    [0061] At time t0, neither the positive electrode AC potential Va nor the negative electrode AC potential Vb reaches a control level (see figure 8C). Under this condition, the controller repeats the processing of steps S1 -> S2 -> S5 -> S6 -> S7 -> S10 -> S11. Therefore, the positive electrode AC current I1 and the negative electrode AC current I2 increase (see figure 8B).
    [0062] When the positive electrode AC potential Va reaches the control level at time t1 (see figure 8C), the controller repeats the steps S1 -> S2 -> S4 -> S6 -> S7 -> S10 -> S11. Therefore, the AC current of the positive electrode I1 is maintained and the AC current of the negative electrode I2 increases (see figure 8B).
    [0063] When the negative electrode AC potential Vb also reaches the control level to be equal to the positive electrode AC potential Va at time t2 (see figure 8C), the controller processes steps S1 -> S2 -> S4 -> S6 -> S7 -> S9 -> S11 -> S12. Therefore, the AC current of the positive electrode I1 and the AC current of the negative electrode I2 are maintained. Then, based on formula (1-1), the internal resistance value of the positive electrode R1 and the internal resistance value of the negative electrode R2 are calculated. Then, the internal resistance value of positive electrode R1 and the internal resistance value of negative electrode R2 are combined to obtain the entire internal resistance R.
    [0064] At time t3, and after it, the internal resistance value of negative electrode R2 is rising due to a change in the wetting state of the fuel cell and other factors (see figure 8A). In this case, the controller repeats the steps S1 -> S2 -> S4 -> S6 -> S8 -> S11 -> S12. Due to such a process, the negative electrode AC current 12 decreases according to the increase in the internal resistance value of the negative electrode R2, where the negative electrode AC potential is maintained to be at the same level as the positive electrode AC potential. Accordingly, the internal resistance can be calculated even in this state.
    [0065] At time t4 and after it, the negative electrode internal resistance value matches the positive electrode internal resistance value (see figure 8A). In this case, the controller repeats steps S1 -> S2 -> S4 -> S6 -> S7 -> S9 -> S11 -> S12. Due to such processing, the positive electrode AC potential is maintained to be at the same level as the negative electrode AC potential (see figure 8C) and the internal resistance is calculated.
    [0066] Figure 9 is a diagram to explain an action effect of the first modality.
    [0067] During an output of the stacked battery (that is, fuel cell), there is a potential difference between the positive electrode and the negative electrode (that is, DC Vdc potential difference). Then, in the present embodiment, the AC currents are sent from the positive electrode power supply part 531 and the negative electrode power supply part 532 in response to a command from the AC adjustment part 540.
    [0068] The AC current sent from the positive electrode power supply part 531 is sent to the positive electrode of the stacked battery (ie fuel cell) through the positive electrode DC break part 511 and flows to the detection part of positive electrode AC potential difference 521 through intermediate terminal 213 and intermediate point DC interrupting part 513. At that moment, the AC potential difference V1 (V1 = Va - Vc) occurs corresponding to the internal resistance and a current supplied . The AC V1 potential difference is detected by the positive electrode 521 detection potential difference.
    [0069] The AC current sent from the negative electrode power supply part 532 is sent to the negative battery electrode of the stacked battery (or fuel cell) through the negative electrode DC break part 512 and flows to the detection part negative electrode AC voltage difference 522 through intermediate terminal 213 and intermediate point DC interrupting part 513. At that moment, the AC voltage difference V2 (V2 = Vb - Vc) occurs corresponding to the internal resistance and a current supplied . The AC potential difference V2 is detected by the negative potential detection part of the negative electrode 522.
    [0070] The AC 540 adjustment part adjusts the positive electrode power supply part 531 and the negative electrode power supply part 532 in order to constantly create the difference between the positive electrode AC potential difference V1 and the negative electrode AC potential difference V2 (V1 - V2, equal to Va - Vb) small in the stacked battery (ie fuel cell).
    [0071] Note that the AC components are superimposed on the DC potential of the positive electrode and the negative electrode during a stacked battery output (ie fuel cell) as illustrated in figure 9, where the AC components are adjusted to remain the same by the AC 540 adjustment part and therefore the DC Vcd potential difference is constant without fluctuations.
    [0072] So, Ohm's law is applied in the resistance calculation part 550 to output V1 of the positive electrode AC potential difference detection part 521, the V2 output of the negative electrode AC potential difference detection part 522, the AC current I1 of the positive electrode power supply part 531 and the AC current I2 of the negative electrode power supply part 532 in order to calculate the internal resistance R1 on the positive electrode side and the internal resistance R2 on the negative electrode side on fuel cell 1.
    [0073] Thus, the positive electrode terminal 211 and the negative electrode terminal 212 share the same AC potential according to the present modality. Therefore, even if a charging device (such as the traction motor) is connected to the positive electrode terminal 211 and the negative electrode terminal 212, leakage of an AC current to the charging device can be suppressed.
    [0074] As a result, the value of AC currents flowing through the internal resistance measurement object (ie fuel cell) combines the value of AC currents sent from the power supply parts and therefore the AC currents flowing to the measurement object can be accurately detected. Since the internal resistance value of the positive electrode R1 and the internal resistance value of the negative electrode R2 in the stacked battery are obtained based on the AC currents, the internal resistance value of the positive electrode R1 and the internal resistance value of the negative electrode R2 on the stacked battery under operation can be accurately measured without being affected by a condition of the charging device, additionally allowing accurate measurement of the entire internal resistance value R of the stacked battery.
    [0075] Additionally, due to the power supply parts used in this modality, the internal resistance can be measured even when the stacked battery (that is, fuel cell) is suspended. Second Mode
    [0076] Figures 10A and 10B are diagrams for explaining an action effect mechanisms of an internal resistance measurement device for the stacked battery according to a second embodiment of the present invention.
    [0077] Although each of the potential difference detection parts AC 521 and 522 and each of the power supply parts 531 and 532 are connected to fuel cell 1 by using a route in the first mode, they are connected fuel cell 1 by different routes in the present modality. This connection will improve the detection accuracy of the internal resistance. The reason will be explained below.
    [0078] When the AC potential difference detection part and the power supply part are connected by a route as shown in figure 10A, the fuel cell potential Vx 1 is expressed by the following formula: formula 2

    [0079] Meanwhile, a voltage Vi detected by the potential difference detection part AC 521 is expressed by the following formula. formula 3

    [0080] Thus, the voltage Vi detected by the potential difference detection part AC 521 is obtained by adding the resistance of the wiring Rw, resistance to contact Rc at a connection point, and an error voltage corresponding to an AC current. for the potential Vx whose detection is originally desired. Accordingly, an err measurement error is expressed by the following formula. formula 4

    [0081] Since the resistance of the measuring object Rx is large in small or similar batteries in general, the contact resistance Rc and the resistance of the wiring Rw can be ignored and do not cause any problems in practical use, whereas large batteries they are generally associated with a ratio so that the resistance of the Rw wiring is greater than the resistance of the measuring object Rx. In this case, each of the stacked cell groups must be connected by the four-terminal method.
    [0082] Therefore, the present modality involves the connection of each of the AC potential difference detection parts and each of the energy sources by a separate route as illustrated in figure 10B. In such a configuration, the contact resistance Rc and the wiring resistance Rw in a voltage detection line AC 501a act to divide the voltage Vx whose detection is desired by the input resistance Ri of the potential difference detection part AC 521. In general, the input resistance Ri of the potential difference detection part CA 521 is extremely large compared to the wiring resistance Rw and the contact resistance Rc (Ri >> (Rw + Rc)). Accordingly, in such a configuration, the measurement error err can be expressed by the following formula and must be minimal, where Vi can be considered Vx. Formula 5

    [0083] Figure 11 illustrates a concrete structure of the second modality.
    [0084] The separators (or bipolar plates) 12 of the power generation cells 10 to constitute the fuel cell 1 are partially extended to provide connecting parts.
    [0085] Figure 12 is a circuit diagram illustrating the internal resistance measurement device for the stacked battery according to the second embodiment of the present invention.
    [0086] The positive electrode difference detection part of the positive electrode 521 is connected to a separator (or bipolar plate) on the positive electrode side of the fuel cell 1 through a capacitor 511a. The positive electrode power supply part 531 is connected to, via capacitor 511, the same separator (or bipolar plate) as one connected to the positive AC potential difference detection part 521 by a route 501 different from the route 501a used by the positive electrode difference detection part of the 521 positive electrode.
    [0087] The negative potential detection part AC of negative electrode 522 is connected to a separator (or bipolar plate) on the negative electrode side of fuel cell 1 through a capacitor 512a. The negative electrode power supply part 532 is connected to, through capacitor 512, the same separator (or bipolar plate) as one connected to the negative potential AC detection part of negative electrode 522 by a 502 route other than a route 502a used by the negative electrode difference detection part of electrode 522.
    [0088] A grounding line 503 is connected to a separator (or bipolar plate) at the intermediate point of the fuel cell 1 through capacitor 513. The positive potential AC difference detection part of the 521 electrode and the difference detection part of negative electrode AC potential 522 are connected to, through a capacitor 513a, the same separator (or bipolar plate) as one connected to the ground line 503 by a route 503a different from the ground line 503.
    [0089] The present modality also focuses attention on a proportional relationship between a command signal from the AC 540 adjustment part and output signals from the positive electrode power supply part 531 and the negative electrode power supply part 532 , where AC current values (I1, I2) are obtained based on the command signal.
    [0090] According to the present modality, it is possible to substantially reduce the effects of resistance fluctuations caused by the size of the wiring resistance and contact resistance, the temperature and surface oxidation of the terminals or other factors. As a result, high versatility in the design of signal wiring with respect to the stacked battery can be achieved while allowing the accurate detection of the internal resistance in each cell of the stacked cell group at low costs.
    [0091] The circuit can also be simplified since the current measurement of the AC current values (I1, I2) is not required. Third Mode
    [0092] Figure 13 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to a third embodiment of the present invention.
    [0093] In the present modality, a part of the AC power supply 570 is connected to a separator (or bipolar plate) disposed in the intermediate part of the fuel cell 1 through capacitor 513. The part of detection of potential difference of electrode AC positive 521 is also connected, via capacitor 513a, to the same separator (or bipolar plate) as one connected to the AC power supply part 570 by route 503a different from the route 503 used by the AC power supply part 570.
    [0094] A positive current detection part of electrode 531a is connected, through a variable resistor Ra, to a variable capacitor Ca and to capacitor 511, the same separator (or bipolar plate) as the one connected to the detection part of positive electrode AC potential difference 521 through route 501 different from route 501a used by positive electrode AC potential difference detection part 521.
    [0095] A negative current detection part of negative electrode 532a is connected, via a fixed resistor Rf and capacitor 512, to the same separator (or bipolar plate) as the one connected to capacitor 612a by route 502 which differs from route 502a used by capacitor 512a. Note that a current / voltage conversion circuit made from the operational amplifier and an AC current sensor from the CT system (current transformer) or other devices can be used for the AC current detection parts 531a and 532a.
    [0096] One AC adjustment part 540a has one end connected between capacitor 511a and the positive potential AC difference detection part 521. The other end of the AC adjustment part 540a is also connected to capacitor 512a. Therefore, the AC 540a adjustment part can receive the positive electrode AC potential Va and the negative electrode AC potential Vb of the fuel cell 1. Then, the AC 540a adjustment part adjusts the variable resistor Ra and the variable capacitor Ca.
    [0097] Figure 14 is a flow chart of control to be performed by the controller on the internal resistance measurement device for the stacked battery according to the third embodiment of the present invention.
    [0098] The controller determines in step S1 whether or not the initial configuration of the value is completed. The controller allows the process to move to step S2 when the determination result is negative (that is, initial value setting not completed) or allows the process to move to step S4 when the determination result is positive (that is, initial setting is completed).
    [0099] In step S2, the controller configures an adjustment amount N for the variable resistor Ra and an adjustment amount M for the variable capacitor Ca. Here, one is determined for each of them as an example.
    [00100] In step S3, the controller calculates a difference of comparative potential Vp by subtracting the negative AC potential Vb from the positive AC potential Va.
    [00101] In step S4, the controller determines whether or not the variable resistor Ra must be adjusted. The controller allows the process to move to step S5 when the determination result is positive or allows the process to move to step S11 when the determination result is negative.
    [00102] In step S5, the controller adds the adjustment amount N to the resistance value Ra of the variable resistor in order to update the value of the variable resistance Ra.
    [00103] In step S6, the controller calculates a potential difference Vn by subtracting the negative AC potential Vb from the positive AC potential Va.
    [00104] In step S7, the controller determines whether or not the potential difference Vn becomes less than the difference in comparative potential Vp. The controller allows the process to move to step S8 when the determination result is negative or allows the process to move to step S9 when the determination result is positive.
    [00105] In step S8, the controller reverses the polarity of the adjustment amount N and exits the process.
    [00106] In step S9, the controller determines whether or not the potential difference Vn has been determined to the minimum. The controller allows the process to move to step S10 when the determination result is positive or exits processing when the determination result is negative.
    [00107] In step S10, the controller updates the comparative potential difference Vp by the difference in potential Vn obtained at that point.
    [00108] In step S11, the controller adds the adjustment amount M to the variable capacitor's Ca capacity in order to update the capacity of the Ca variable capacitor.
    [00109] In step S12, the controller calculates the difference in potential Vn by subtracting the negative AC potential Vb from the positive AC potential Va.
    [00110] In step S13, the controller determines whether or not the potential difference Vn becomes less than the difference in comparative potential Vp. The controller allows the process to move to step S14 when the determination result is negative or allows the process to move to step S15 when the determination result is positive.
    [00111] In step S14, the controller inverts the polarity of the adjustment amount M and exits the process.
    [00112] In step S15, the controller determines whether or not the potential difference Vn is determined to the minimum. The controller allows the process to move to step S16 when the determination result is positive or exits processing when the determination result is negative.
    [00113] In step S16, the controller updates the comparative potential difference Vp by the potential difference Vn obtained at that point.
    [00114] In step S17, the controller calculates the resistance values based on the formulas mentioned above (1-1) and (1-2).
    [00115] The execution of the flowchart above is accompanied by the following operation.
    [00116] First, an initial value is determined (S1 -> S2 -> S3).
    [00117] In the next cycle, the variable resistor Ra is adjusted first. The variable resistance value Ra is adjusted (S4) to calculate the potential difference Vn (S5) followed by reversing the polarity of the adjustment quantity N if the potential difference is not reduced (S8) and determining whether or not the difference in potential that has been reduced is a minimum value (S9). The same process (S1 -> S4 -> S5 -> S6 -> S7 -> S8 or S9) is repeated until the potential difference Vp is updated by the potential difference Vn obtained at that point (S10).
    [00118] In the next cycle, the capacity of the variable capacitor Ca is adjusted. The capacity of the variable capacitor Ca is adjusted (S11) to calculate the potential difference Vn (S12), followed by the inversion of the polarity of the adjustment quantity M if the potential difference is not reduced (S14) and determining whether or not the difference of potential that has been reduced is a minimum value (S15). The same process (S1 -> S4 -> S11 -> S12 -> S13 -> S14 or S15) is repeated until the potential difference is a minimum value, where the capacity of the variable capacitor Ca is adjusted to a minimum value. Then, when the capacity of the variable capacitor Ca is adjusted to a minimum value, the difference in comparative potential Vp is updated by the difference in potential Vn obtained at that point (S16).
    [00119] Then, the resistance values are calculated based on the formulas mentioned above (1-1) and (1-2) (S17).
    [00120] The configuration as illustrated in the present modality necessarily provides the same amplitude of AC voltage between both ends of each of the stacked cell groups. It is, therefore, possible to obtain the same effects as the first modality and the second modality. That is, the value of an AC current flowing through the internal resistance measurement object (ie, fuel cell) matches the value of AC currents sent from the power supplies and therefore AC currents flowing through the object of measurement can be accurately detected. Then, the internal resistance in the stacked battery is obtained based on the AC currents, where the accurate measurement of the internal resistance of the stacked battery under operation can be performed without being affected by a condition of the charging device.
    [00121] Additionally, since both ends of each of the stacked cell groups necessarily have the same AC voltage amplitude according to the present modality, the AC potential difference detection part can be arranged on the positive electrode side or on the negative electrode side. Note that the present modality is provided with the potential difference detection part AC 521 on the positive electrode side. Accordingly, the circuit can be simplified. Fourth Mode
    [00122] Figure 15 is a circuit diagram illustrating an internal resistance measurement device for the stacked battery according to a fourth embodiment of the present invention.
    [00123] In the present modality, similar to the third modality, the AC 570 power supply part is connected to a separator (or bipolar plate) disposed at the intermediate point of the fuel cell 1 through capacitor 513. The difference detection part of positive electrode AC potential 521 and the negative potential difference detection part of negative electrode 522 are connected, via capacitor 513a, to the same separator (or bipolar plate) as one connected to the AC power supply part 570 via route 503a different from route 503 used by the AC 570 power supply part.
    [00124] A positive electrode reverse polarity amplifier 540b is connected, through capacitor 511, to the same separator (or bipolar plate) as the one connected to the positive potential AC difference detection part of positive electrode 521 by route 501 different from route 501a used by the positive electrode difference detection part of positive electrode 521.
    [00125] A 540c negative electrode polarity inversion amplifier is connected, via capacitor 512, to the same separator (or bipolar plate) as the one connected to the negative potential AC detection part of negative electrode 522 by route 502 different from route 502a used by the negative electrode difference detection part of electrode 522. Note that circuits such as an inversion amplifier circuit made of the operational amplifier, boot strap circuit and active noise cancellation circuit are applicable to amplifiers reverse polarity 540b and 540c.
    [00126] Due to such a configuration, the polarity of the AC voltages detected at the output ends of the stacked battery is reversed and returned to the output terminals of the stacked battery, where the amplitude of the AC voltages at the output ends of the stacked battery is forcibly eliminated (or set to zero). Therefore, the amplitude of both AC voltages at both ends of the stacked battery is made zero and equipotentialized.
    [00127] AC currents flowing through each of the stacked cell groups are detected by the AC current detection parts 531a and 532a and AC voltages at both ends of the stacked cell group are detected by the potential difference detection parts AC 521 and 522 connected to the AC voltage detection lines.
    [00128] Accordingly, the present modality makes it possible to simplify the circuit since a voltage comparison function performed by the adjustment part AC 540 becomes unnecessary. Fifth Mode
    [00129] Figure 16 illustrates an internal resistance measurement device for stacked batteries according to a fifth embodiment of the present invention.
    [00130] Each of the above modalities involves the connection of an intermediate point. In contrast, the present modality switches the intermediate point sequentially. That is, a 580 connection switch is used to switch the waypoint sequentially.
    [00131] Due to such a configuration, the resistance of a currently connected cell can be calculated by comparing a currently measured value with a previously measured value. Accordingly, the internal resistance can be measured for each cell. It is, therefore, possible to monitor the distribution of internal resistance in a direction of stacking and deterioration of local cell or similar. Sixth Mode
    [00132] Figure 17 illustrates an internal resistance measurement device for the stacked battery according to a sixth embodiment of the present invention.
    [00133] In each of the above modalities, each of the AC potential difference detection parts and each of the power supply parts (or AC current detection parts) is connected to the common separator (or bipolar board). In contrast, the present modality involves connecting each of the components to a bipolar plate separated by at least another bipolar plate. The concrete circuit diagram is as illustrated in figure 18.
    [00134] The positive electrode power supply part 531 is connected to bipolar plate 501 on the positive electrode side of fuel cell 1 through capacitor 511. The positive potential AC difference detection part of positive electrode 521 is connected to the plate bipolar 501a different from bipolar plate 501 through capacitor 511a. The positive electrode difference detection part of positive electrode 521 is also connected, through a capacitor 5131a, to a bipolar plate 5031a different from the bipolar plate 503 that is connected to a grounding line.
    [00135] The negative electrode power supply part 532 is connected to the bipolar plate 502 on the negative electrode side of fuel cell 1 through capacitor 512. The negative potential AC detection part of negative electrode 522 is connected to the plate bipolar 502a different from the bipolar plate 502 through capacitors 512a. The negative potential AC detection part of negative electrode 522 is also connected, via a capacitor 5132a, to a bipolar plate 5032a different from the bipolar plate 503 connected to the ground line.
    [00136] The same action effect as the second modality can also be obtained by the present modality. Miniaturization can be performed since the space occupied by the connection terminals can be narrowed. Note that it is impossible in the present mode to detect the cell resistance between the bipolar plate 501 and the bipolar plate 501a, the cell resistance between the bipolar plate 502 and the bipolar plate 502a, the cell resistance between the bipolar plate 503 and the bipolar plate 5031a and the cell resistance between the bipolar plate 503 and the bipolar plate 5032a as they are outside the AC voltage detection range. However, it is not a problem in such cases that the number of cells stacked is large as illustrated in large stacked batteries and / or resistance variations are aligned between the cells, since the average cell resistance per cell can be obtained by using the number of cells in the detection range and spliced. Seventh Mode
    [00137] Figure 19 is a circuit diagram illustrating an internal resistance measurement device for stacked batteries according to a seventh embodiment of the present invention.
    [00138] The present modality is the same as the third modality (illustrated in figure 13) in terms of circuit diagram. However, in contrast to the third modality in which the AC potential difference detection part and the power supply part (or AC current detection part) are connected to the common separator (or bipolar board), the present modality involves the connection to different bipolar plates separated by at least another bipolar plate. Note that the AC potential difference detection part is disposed only on the positive electrode side in the present modality and the AC potential difference detection part of the positive electrode is connected to the bipolar 5031a plate as shown in figure 17. No it is necessary to prepare an AC potential difference detection part connected to the 5032a bipolar plate illustrated in figure 17.
    [00139] Due to such a configuration, similar to the third modality, the amplitude of AC voltage necessarily remains the same at both ends of each of the stacked cell groups. Therefore, the value of AC currents flowing through the internal resistance measurement object (or fuel cell) matches the value of AC currents sent from the power supplies, and therefore AC currents flowing through the measurement object can be accurately detected. . Then, the internal resistance of the stacked battery is obtained based on AC currents, where the accurate measurement of the internal resistance of the stacked battery under operation is unaffected by a condition of the charging device. It is also possible to achieve miniaturization since the space occupied by the connection terminals can be narrowed. Eighth Mode
    [00140] Figure 20 is a circuit diagram illustrating an internal resistance measurement device for stacked batteries according to an eighth embodiment of the present invention.
    [00141] The present modality is basically the same as the fourth modality (illustrated in figure 15). However, as opposed to the fourth modality (illustrated in figure 15) where each of the AC potential difference detection parts and each of the power supply parts (or AC current detection parts) are connected to the common separator ( or bipolar plate), the present modality involves connecting them to different bipolar plates separated by at least another bipolar plate. A concrete circuit diagram is as illustrated in figure 20.
    [00142] The positive electrode reverse polarity amplifier 540b is connected to the bipolar plate 501 on the positive electrode side of fuel cell 1 through capacitor 511. The positive potential AC difference detection part of the positive electrode 521 is connected to the plate bipolar 501a which differs from the bipolar plate 501 through capacitor 511a. The positive electrode difference detection portion of positive electrode 521 is also connected, via capacitor 5131a, to the bipolar plate 5031a which differs from the bipolar plate 503 connected to the ground line.
    [00143] The negative electrode polarity reversal amplifier 540c is connected to the bipolar plate 502 on the negative electrode side of fuel cell 1 through capacitor 512. The negative potential AC difference detection part of negative electrode 522 is connected to the bipolar 502a which differs from the bipolar plate 502 through capacitor 512a. The negative potential AC detection part of negative electrode 522 is also connected, via capacitor 5132a, to the bipolar plate 5032a which differs from the bipolar plate 503 connected to the ground line.
    [00144] Due to such a configuration, similar to the fourth modality, the polarity of the AC currents detected at the output ends of the stacked battery is inverted and returned to the output terminals of the stacked battery, where the amplitude of the AC voltages at the output ends of the stacked battery is forcibly eliminated (or zeroed). Therefore, the amplitude of both AC voltages at both ends of the stacked battery is zeroed and equipotentialized. In addition, AC currents flowing through each of the stacked cell groups are detected by the AC current detection parts 531a and 532a and AC voltages at both ends of the stacked cell group are detected by the AC potential difference detection part 521 and 522 connected to the AC voltage detection lines. As a result of this, the present modality makes it possible to simplify the circuit since a voltage comparison function performed by the AC 540 adjustment part is not necessary. Miniaturization can also be achieved since the space occupied by the connection terminals can be narrowed.
    [00145] Although the modalities of the present invention are as explained above, the modalities above exhibit merely a part of the application examples of the present invention and should not limit the technical scope of the present invention to the concrete configurations of the above modalities.
    [00146] For example, as illustrated in figure 21A, the internal resistance measurement object may additionally contain a resistor 2 connected in series to the stacked battery 1. In such a case, one end of resistor 2 illustrated in figure 21A is considered the electrode positive in the above modalities, the positive electrode of the stacked battery 1 shown in figure 21A is considered the intermediate point in the above modalities, and the negative electrode of the stacked battery 1 illustrated in figure 21A is considered the negative electrode of the above modalities. By recognizing each of the electrodes, a total internal resistance value of the stacked battery as illustrated in figure 21A can be obtained as R2. Even in such a configuration, it is possible to achieve the accurate measurement of a total internal resistance value in the stacked battery.
    [00147] Furthermore, the internal resistance measurement object can also be configured so that a stacked battery 1-2 is additionally connected in series to a stacked battery 101. In such a case, a positive electrode from the stacked battery 1-1 is considered the positive electrode in the above modalities, an intermediate point between the stacked battery 1-1 and the stacked battery 1-2 is considered the intermediate point in the above modalities, and a negative electrode in the stacked battery 1-2 is considered the negative electrode in the above modalities. above modalities. By recognizing each of the electrodes, a stacked battery internal resistance value 1-1 is obtained as R1 and a stacked battery internal resistance value 1-2 is obtained as R2. Even in such a configuration, it is possible to achieve an accurate measurement of the internal resistance values in the stacked battery 1-1 and the stacked battery 1-2.
    [00148] Additionally, the fuel cell used as an example of the battery stacked in the above mode can also be replaced by other batteries such as lithium ion battery. That is, the present invention is applicable to any batteries as long as a plurality of power generating elements are stacked. The measurement of internal resistance performed on such batteries allows efficient operation, which is desirable.
    [00149] Additionally, even in the configuration as illustrated in figure 17, the intermediate point can be switched sequentially as illustrated in the fifth modality. Even in such a configuration, the same action effect as the fifth modality can be obtained.
    [00150] The above modalities can also be combined with each other as appropriate.
    [00151] This application claims priority of Japanese patent application No. 2010- 275638 filed with the Japanese Patent Office on December 10, 2010. The contents of that application are incorporated herein by reference in their entirety.
    权利要求:
    Claims (13)
    [0001]
    1. Internal resistance measurement device (5) for stacked battery (1) comprising: an AC power supply part (531, 532) to send an AC current to an internal resistance measurement object including at least one stacked battery (1) made of a plurality of power generation elements stacked through connection to the internal resistance measurement object; and a resistance calculation part (550) for calculating stacked battery resistance (1), CHARACTERIZED by the fact that: the device (5) further comprises an AC adjustment part (540) to adjust an AC current so that a difference of positive electrode AC potential, being a potential difference obtained by subtracting potential in an intermediate part (503) of potential in a positive side part (501) connected to a charging device (3) on the positive electrode side of the internal resistance measurement object, combine with a negative electrode AC potential difference, being a potential difference obtained by subtracting the potential in the intermediate part (503) of the potential in a negative side part (502) connected to the charge (3) on the negative electrode side of the internal resistance measurement object; and the resistance calculation part (550) is configured to calculate the resistance of the stacked battery (1) based on the adjusted AC current and the AC potential difference.
    [0002]
    2. Internal resistance measurement device (5) for stacked battery (1), according to claim 1, CHARACTERIZED by the fact that: the object of internal resistance measurement is the stacked battery (1).
    [0003]
    3. Internal resistance measurement device (5) for stacked battery (1) according to either of claims 1 or 2, CHARACTERIZED by the fact that: the AC power supply part (531, 532) includes a part positive electrode power supply (531) to send an AC current to the internal resistance measurement object via connection to the positive side part (501) of the internal resistance measurement object via a DC interrupt part (511 ), and a negative electrode power supply part (532) to send an AC current to the internal resistance measurement object via the connection to the negative side part (502) of the internal resistance measurement object via a part DC break (512); and the AC adjustment part (540) adjusts the positive electrode power supply part (531) and the negative electrode power supply part (532) so that the positive electrode AC potential difference matches the difference negative electrode AC potential.
    [0004]
    4. Internal resistance measuring device (5) for stacked battery (1), according to claim 3, CHARACTERIZED by the fact that: the positive side part (501) is connected via the DC interrupting part (511 ), to a positive electrode AC voltage difference detector (521) to detect the positive electrode AC voltage difference by a route other than a route connected to the positive electrode power supply part (531); the negative side part (502) is connected, via the DC interrupting part (512), to a negative electrode AC potential difference detector (522) to detect the negative electrode AC potential difference by a route other than a route connected to the negative electrode power supply part (532); and the intermediate part (503) is connected to a grounding line through a DC interrupting part (511) and connected, via a DC interrupting part (511), to the positive electrode AC potential difference detector (521 ) and the negative electrode AC potential difference detector (522) by a different route than the route connected to the ground line.
    [0005]
    5. Internal resistance measuring device (5) for stacked battery (1), according to claim 4, CHARACTERIZED by the fact that: a positive electrode AC potential difference detector (521) to detect the potential difference Positive electrode AC is connected, via a DC interrupting part (511), to a separate part of the positive side part (501) by at least one power generating element; a negative electrode AC potential difference detector (522) to detect the negative electrode AC potential difference is connected, via a DC interrupting part (512), to a separate part of the negative side part (502) by at least one element of power generation; the intermediate part (503) is connected to a grounding line through a DC interrupting part (513); the positive side part (501) to be separated from the intermediate part (503) by at least one power generation element is connected to the positive electrode AC potential difference detector (521) via a DC interruption part (511 ); and the negative side part (502) to be separated from the intermediate part (503) by at least one power generating element is connected to the negative electrode AC potential difference detector (522) via a DC interrupting part ( 512).
    [0006]
    6. Internal resistance measurement device (5) for stacked battery (1), according to either of claims 1 or 2, CHARACTERIZED by the fact that it comprises: a variable resistor (Ra) and a variable capacitor (Ca) connected to one between the positive side part (501) and the negative side part (502) of the internal resistance measurement object through a DC interruption part (511, 512); a fixed resistor (Rf) connected to the other between the positive side part (501) and the negative side part (502) of the internal resistance measurement object through a DC interruption part (512, 511); and an AC potential difference detector (521, 522) to detect the positive electrode AC potential difference or the negative electrode AC potential difference by connecting to one of the positive side part (501) and the negative side (502) and the intermediate part (503) through the DC interrupting part (511, 512), where: the AC power supply part (531, 532) sends an AC current to the intermediate part (503) through the connection to the intermediate part (503) through a DC interruption part (513); and the AC adjustment part (540a) adjusts the variable resistor (Ra) and the variable capacitor (Ca) so that the positive electrode AC potential matches the negative electrode AC potential.
    [0007]
    7. Internal resistance measurement device (5) for stacked battery (1), according to claim 6, CHARACTERIZED by the fact that: the positive side part (501) is connected via the DC interrupting part (511 ), to a different route than a route connected to one between the variable resistor (Ra) and the fixed resistor (Rf) in order to send the positive electrode AC potential to the AC adjustment part (540); the negative side part (502) is connected, through the DC interruption part (512), to a different route from one connected to the other between the variable resistor (Ra) and the fixed resistor (Rf) in order to send the negative electrode AC potential for the AC adjustment part (540); and the intermediate part (503) is connected, via the DC interrupting part (513), to the AC potential difference detector (521) by a route other than a route connected to the AC power supply part (531, 532) .
    [0008]
    8. Internal resistance measurement device (5) for stacked battery (1), according to claim 6, CHARACTERIZED by the fact that: a part separated from the positive side part (501) by at least one generation element energy is connected, via a DC interrupting part (511), to a route to send the positive electrode AC potential to the AC adjustment part (540); a part separated from the negative side part (502) by at least one power generating element is connected, via a DC interrupting part (512), to a route to send the negative electrode AC potential to the adjustment part CA (540); and a part separated from the intermediate part (503) by at least one power generating element is connected to the AC potential difference detector (521, 522) via a DC interrupting part (513).
    [0009]
    9. Internal resistance measurement device (5) for stacked battery (1) according to either of claims 1 or 2, CHARACTERIZED by the fact that: the AC power supply part (531, 532) sends a current AC to the intermediate part (503) through the connection to the intermediate part (503) through a DC interruption part (511, 512); and the AC adjustment part (540) includes a positive electrode adjustment part (540b) to transform potential on the positive side part (501) of the internal resistance measurement object to zero through connection with the positive side part ( 501) of the internal resistance measurement object through a DC interruption part (511), and a negative electrode adjustment part (540c) to transform potential in the negative side part (502) of the internal resistance measurement object in zero through connection to the negative side part (502) of the internal resistance measurement object via a DC interruption part (512).
    [0010]
    10. Internal resistance measurement device (5) for stacked battery (1), according to claim 9, CHARACTERIZED by the fact that: the positive side part (501) is connected, via a DC interruption part ( 511a), to a positive electrode AC potential difference detector (521) to detect the positive electrode AC potential difference, by a route other than a route connected to the positive electrode adjustment part (540b); the negative side part (502) is connected, via a DC interrupting part (512a), to a negative electrode AC potential difference detector (522) to detect the negative electrode AC potential difference, by a route different from a route connected to the negative electrode adjustment part (540c); and the intermediate part (503) is connected, via a DC interrupting part (513a), to the positive electrode AC potential difference detector (521) and to the negative electrode AC potential difference detector (522) by a route other than a route connected to an AC power supply part (570).
    [0011]
    11. Internal resistance measuring device (5) for stacked battery (1), according to claim 9, CHARACTERIZED by the fact that: a part (501a) separated from the positive side part (501) by at least one element power generation is connected, via a DC interruption part (511a), to a positive electrode AC potential difference detector (521) to detect the positive electrode AC potential difference; a part (502a) separated from the negative side part (502) by at least one power generating element is connected, via a DC interrupting part (512a), to a negative electrode AC potential difference detector (522 ) to detect the negative electrode AC potential difference; a part (5031a) on the positive electrode side to be separated from the intermediate part (503) by at least one power generating element is connected to the positive electrode AC potential difference detector (521) via a DC interrupting part (511); and a part on the negative electrode side to be separated from the intermediate part (503) by at least one power generating element is connected, via a DC interrupting part (5132a), to the negative electrode AC potential difference detector (522).
    [0012]
    12. Internal resistance measuring device (5) for stacked battery (1), according to any one of claims 1 to 11, CHARACTERIZED by the fact that it additionally comprises: a connection switch (580) for switching the intermediate part (503 ) sequentially.
    [0013]
    13. Internal resistance measurement method for stacked battery (1) comprising: an AC output step (S3, S4, S5, S8, S9, S10) of sending an AC current to an internal resistance measurement object comprising a stacked battery (1) made of a plurality of stacked power generation elements through connection to the internal resistance measurement object; and a resistance calculation step (S12) to calculate stacked battery resistance (1), CHARACTERIZED by the fact that: the method also comprises an AC adjustment step (S1, S2, S3, S4, S5, S6, S7, S8, S9, S10, S11) to adjust an AC current so that a positive electrode AC potential difference, being a potential difference obtained by subtracting potential in an intermediate part (503) of potential in a positive side part (501) connected to a charging device (3) on the positive electrode side of the internal resistance measurement object, combine with a negative electrode AC potential difference, being a potential difference obtained by subtracting potential in the intermediate part ( 503) of potential on a negative side part (502) connected to the charging device (3) on the negative electrode side of the internal resistance measurement object; and the resistance calculation step (S12) is configured to calculate the stacked battery resistance (1) based on the adjusted AC current and the AC potential difference.
    类似技术:
    公开号 | 公开日 | 专利标题
    BR112013014482B1|2020-12-22|internal resistance measurement device and internal resistance measurement method for stacked battery
    JP5867615B2|2016-02-24|Multilayer battery impedance measurement device
    JP6075442B2|2017-02-08|Impedance measuring device and control method of impedance measuring device
    CA2943932C|2019-02-19|Diagnosis device and diagnosis method
    EP3168629B1|2018-06-20|Apparatus for measuring an impedance of fuel cell and method of measuring an impedance of fuel cell
    WO2016006114A1|2016-01-14|Fuel cell impedance measurement device and fuel cell impedance measurement method
    JP6036836B2|2016-11-30|Multilayer battery internal resistance measurement circuit
    KR102221208B1|2021-03-02|Apparatus and method for measuring an average power of fuel cell
    JP2016050858A|2016-04-11|Layer-built cell impedance measuring apparatus
    JP6675725B1|2020-04-01|Impedance spectrum estimation method
    JP2658502B2|1997-09-30|Lead-acid battery internal impedance measurement device
    CN112748281A|2021-05-04|Average power measuring device and method for fuel cell, and voltage measuring device
    同族专利:
    公开号 | 公开日
    WO2012077450A1|2012-06-14|
    EP2650689B1|2019-09-18|
    RU2536780C1|2014-12-27|
    JP5708658B2|2015-04-30|
    EP2650689A1|2013-10-16|
    JPWO2012077450A1|2014-05-19|
    KR20130102106A|2013-09-16|
    CN103261898A|2013-08-21|
    KR101481359B1|2015-01-09|
    CN104614680A|2015-05-13|
    EP2650689A4|2017-10-18|
    MX2013006438A|2013-06-28|
    BR112013014482A2|2016-09-20|
    RU2013131786A|2015-01-20|
    MY173025A|2019-12-19|
    US20130249562A1|2013-09-26|
    CN104614680B|2018-04-20|
    US9366731B2|2016-06-14|
    CN103261898B|2015-04-08|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US3753094A|1969-07-01|1973-08-14|Matsushita Electric Ind Co Ltd|Ohmmeter for measuring the internal resistance of a battery and directly reading the measured resistance value|
    US5047722A|1989-04-17|1991-09-10|Ssmc Inc.|Apparatus for measuring internal resistance of wet cell storage batteries having non-removable cell caps|
    JPH033659U|1989-05-31|1991-01-16|
    JPH03226688A|1990-01-31|1991-10-07|Yuasa Battery Co Ltd|Method for judging life of lead storage battery|
    JP3003659U|1994-04-28|1994-10-25|アデックス株式会社|Impedance measuring device|
    US5862515A|1996-02-16|1999-01-19|Hioki Denki Kabushiki Kaisha|Battery tester|
    JPH09297165A|1996-03-04|1997-11-18|Hioki Ee Corp|Battery tester|
    JP3713828B2|1996-08-12|2005-11-09|ソニー株式会社|Charging method, charging device and charging control circuit|
    JP3720555B2|1997-12-15|2005-11-30|ソニー株式会社|Battery cell inspection method and battery cell inspection apparatus|
    JP3598873B2|1998-08-10|2004-12-08|トヨタ自動車株式会社|Secondary battery state determination method and state determination device, and secondary battery regeneration method|
    JP2001351696A|2000-06-02|2001-12-21|Hitachi Ltd|Charging and discharging device of secondary cell|
    JP2002267704A|2001-03-14|2002-09-18|Hioki Ee Corp|Method and instrument for measuring internal resistance of layer built cell|
    JP4360052B2|2001-06-27|2009-11-11|株式会社ジーエス・ユアサコーポレーション|Secondary battery lifetime determination device, lifetime determination method, and lifetime determination program|
    JP2003121516A|2001-10-09|2003-04-23|Furukawa Battery Co Ltd:The|Measurement device for internal resistance of storage battery|
    JP3904875B2|2001-10-09|2007-04-11|古河電池株式会社|Method for measuring internal impedance of storage battery|
    JP2003121513A|2001-10-09|2003-04-23|Furukawa Battery Co Ltd:The|Measuring method for internal resistance of storage battery|
    JP4407874B2|2001-10-09|2010-02-03|古河電池株式会社|Storage battery internal resistance measurement circuit|
    US7208914B2|2002-12-31|2007-04-24|Midtronics, Inc.|Apparatus and method for predicting the remaining discharge time of a battery|
    US7642786B2|2004-06-01|2010-01-05|Midtronics, Inc.|Battery tester capable of identifying faulty battery post adapters|
    US7545146B2|2004-12-09|2009-06-09|Midtronics, Inc.|Apparatus and method for predicting battery capacity and fitness for service from a battery dynamic parameter and a recovery voltage differential|
    DE102005029096A1|2005-06-23|2007-01-04|Robert Bosch Gmbh|Battery condition detection for car batteries|
    JP2007181365A|2005-12-28|2007-07-12|Ntt Data Ex Techno Corp|Ac voltage applying circuit and method to battery group|
    JP2007188767A|2006-01-13|2007-07-26|Fujitsu Ten Ltd|Battery condition monitoring device, battery condition monitoring system and battery condition monitoring method|
    US20070194791A1|2006-02-17|2007-08-23|Bppower Inc.|Method and apparatus for monitoring the condition of a battery by measuring its internal resistance|
    JP5563734B2|2007-10-31|2014-07-30|日置電機株式会社|Electronic load device and battery internal resistance measuring device|
    CN201156079Y|2007-12-27|2008-11-26|武汉理工大学|Single slice battery essential resistance and voltage on-line testing system for fuel cell pile|
    JP5228759B2|2008-09-29|2013-07-03|日産自動車株式会社|Resistance distribution detection device and fuel cell system using the same|
    CN101477179A|2009-01-15|2009-07-08|艾默生网络能源有限公司|On-line AC detection method and system for internal resistance of accumulator|
    CN201548669U|2009-11-24|2010-08-11|南京鼎尔特科技有限公司|Storage battery fault early-warning device|
    CN201594116U|2009-11-30|2010-09-29|比亚迪股份有限公司|Measuring device of battery internal resistance|
    CN101806865B|2010-03-29|2013-04-17|深圳睿立方智能科技有限公司|Detection device of internal resistance of cell|US9529055B2|2012-10-09|2016-12-27|Nissan Motor Co., Ltd.|Impedance measuring device for laminated battery|
    WO2014141752A1|2013-03-12|2014-09-18|日産自動車株式会社|Impedance measuring device and control method for impedance measuring device|
    EP3040728B1|2013-08-29|2020-05-27|Nissan Motor Co., Ltd|Stacked battery impedance measurement device and measurement method|
    JP2015154593A|2014-02-14|2015-08-24|ソニー株式会社|Charge/discharge control device, battery pack, electronic apparatus, electric motor vehicle and charge/discharge control method|
    CN106030324B|2014-02-19|2019-02-22|日产自动车株式会社|The control method of impedance measuring instrument and impedance measuring instrument|
    US9791518B2|2014-02-19|2017-10-17|Nissan Motor Co., Ltd.|Impedance measuring device and control method for impedance measuring device|
    EP3124987B1|2014-03-26|2018-11-21|Nissan Motor Co., Ltd|Impedance measurement device and impedance measurement method|
    WO2015145755A1|2014-03-28|2015-10-01|日産自動車株式会社|Cell stack, separator, and method for connecting internal resistance measurement device|
    JP6318883B2|2014-06-09|2018-05-09|日産自動車株式会社|Impedance measuring device|
    JP6458375B2|2014-07-03|2019-01-30|日産自動車株式会社|Impedance measuring device|
    JP6413402B2|2014-07-03|2018-10-31|日産自動車株式会社|Impedance measuring device|
    WO2016006114A1|2014-07-11|2016-01-14|日産自動車株式会社|Fuel cell impedance measurement device and fuel cell impedance measurement method|
    US10290885B2|2014-07-11|2019-05-14|Nissan Motor Co., Ltd.|Apparatus for measuring an impedance of fuel cell and method of measuring an impedance of fuel cell|
    US20160020618A1|2014-07-21|2016-01-21|Ford Global Technologies, Llc|Fast Charge Algorithms for Lithium-Ion Batteries|
    JP6446920B2|2014-08-29|2019-01-09|日産自動車株式会社|Multilayer battery impedance measurement device|
    WO2016092618A1|2014-12-08|2016-06-16|日産自動車株式会社|Impedance measurement device and impedance measurement method|
    KR101859419B1|2014-12-26|2018-05-23|엘지디스플레이 주식회사|Touch screen device and method for driving the same|
    WO2016125231A1|2015-02-02|2016-08-11|日産自動車株式会社|Fuel battery system and fuel battery system control method|
    CN107615544B|2015-05-21|2018-11-27|日产自动车株式会社|Power regulation system and its control method|
    JP6485746B2|2015-06-16|2019-03-20|パナソニックＩｐマネジメント株式会社|Fuel cell system and operation method thereof|
    CN109142872A|2017-06-16|2019-01-04|日本贵弥功株式会社|The measuring method and measurement device of the resistance of charge storage element|
    法律状态:
    2016-09-27| B08E| Application fees: payment of additional fee required [chapter 8.5 patent gazette]|Free format text: COMPLEMENTAR A RETRIBUICAO DA(S) 5A. ANUIDADE(S), DE ACORDO COM TABELA VIGENTE, REFERENTE A(S) GUIA(S) DE RECOLHIMENTO 92160101872-9. |
    2016-12-13| B08F| Application dismissed because of non-payment of annual fees [chapter 8.6 patent gazette]|Free format text: NAO APRESENTADA A GUIA DE CUMPRIMENTO DE EXIGENCIA. |
    2017-04-11| B08G| Application fees: restoration [chapter 8.7 patent gazette]|
    2018-12-18| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
    2019-08-06| B06U| Preliminary requirement: requests with searches performed by other patent offices: procedure suspended [chapter 6.21 patent gazette]|
    2020-04-07| B07A| Application suspended after technical examination (opinion) [chapter 7.1 patent gazette]|
    2020-09-01| B06A| Patent application procedure suspended [chapter 6.1 patent gazette]|
    2020-11-03| B09A| Decision: intention to grant [chapter 9.1 patent gazette]|
    2020-12-22| B16A| Patent or certificate of addition of invention granted [chapter 16.1 patent gazette]|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 09/11/2011, OBSERVADAS AS CONDICOES LEGAIS. |
    优先权:
    申请号 | 申请日 | 专利标题
    JP2010-275638|2010-12-10|
    JP2010275638|2010-12-10|
    PCT/JP2011/075792|WO2012077450A1|2010-12-10|2011-11-09|Layered battery internal resistance measuring apparatus|
    [返回顶部]