Verfahren zum Plausibilisieren einer elektronischen Schaltung zur Zeitmessung eines elektrochemischen Energiespeichersystems

Abstract

Method for checking the plausibility of an electronic circuit for time measurement of an electrochemical energy storage system by means of a cooling behavior of at least one electrochemical energy store during non-use of the electrochemical energy store.

Description

BACKGROUND OF THE INVENTION

The invention proceeds from a method for checking the plausibility of an electronic circuit for time measurement of an electrochemical energy storage system, an electrochemical energy storage system and use of an electrochemical energy storage system.

Document U.S. Pat. No. 5,955,869 discloses a method for monitoring the remaining capacity of a rechargeable battery pack. In said method, two different processes are used to estimate the remaining capacity. In a first process, the data generated on the rechargeable battery pack are used to estimate the remaining rechargeable battery capacity; and in the second procedure, data transmitted from a host device to the battery pack are used to estimate the remaining battery capacity. The rechargeable battery alternates between said two processes under defined conditions and, in the preferred embodiment, which is described in detail in the present description, the battery block alternates from the first procedure to the second procedure when the battery current falls below a threshold value.

Document US 2018/183252 discloses a method and provides an apparatus for detecting a battery state of an electronic apparatus. The electronic apparatus comprises a battery, a charging circuit for charging the battery, a measurement circuit for testing a state of the battery and a processor, which is configured to charge the battery using the charging circuit in order to determine whether the charging process fulfils a preset condition.

SUMMARY OF THE INVENTION

The approach according to the invention in contrast has the advantage that the check for plausibility is effected by means of a cooling behavior of at least one electrochemical energy store during non-use of the electrochemical energy store, comprising the following steps:

a) detecting an ambient temperature T_Env of the electrochemical energy store;

b) detecting a temperature T_t0 of the electrochemical energy store at the beginning of the non-use of the electrochemical energy store;

c) detecting a temperature T_t1 of the electrochemical energy store at the beginning of a restart of the electrochemical energy store;

d) calculating a period toff of the non-use of the electrochemical energy store in accordance with the formula

$t_{\mathrm{off}}=-\tau *\ln \left(\frac{T_{t1}-T_{\mathrm{Env}}}{T_{t0}-T_{\mathrm{Env}}}\right),$

wherein τ is a system constant, which comprises material properties of the electrochemical energy store in accordance with

$\tau =\frac{m*c_p}{\alpha *A},$

wherein m is a mass, A is a contact area, α is a thermal conductivity and c_p is a specific thermal capacity of the electrochemical energy store;

e) determining an overall error in the calculation of the period t_off of the non-use of the electrochemical energy store in accordance with the formula Δt_off^err=Δt₁+Δt₂+Δt₃, wherein

• • Δt1 is a temperature measurement error during the restart of the electrochemical energy store,

Δt2 is a temperature measurement error at the beginning of the non-use of the electrochemical energy store and

Δt3 is a temperature measurement error of the ambient temperature;

f) checking the plausibility of the electronic circuit for time measurement by comparing a period t_off^Clock of the non-use of the electrochemical energy store, which period is measured by the electronic circuit for time measurement, with the calculated period t_off of the non-use of the electrochemical energy store; and

g) identifying an error in the electronic circuit for time measurement when Δt_off^err<|t_off^Clock−t_off|.

The method for checking the plausibility of an electronic circuit for time measurement further can also comprise the following step:

h) generating an electrical, optical, acoustic and/or haptic signal when an error is identified in the electronic circuit for time measurement.

As a result thereof, for example, when an error is identified in the electronic circuit for time measurement, a user of the electrochemical energy storage system can be warned and/or the error can be stored for servicing purposes.

An electrochemical energy storage system advantageously comprises at least one electrochemical energy store, at least one sensor for detecting a temperature of the electrochemical energy store and/or an ambient temperature of the electrochemical energy store, an electronic circuit for time measurement and at least one means, in particular an electronic battery management control device, which is configured to carry out the steps of the method according to the invention.

A computer program advantageously comprises commands, which, when the computer program is executed by an electronic battery management control device, cause same to execute the method according to the invention.

The computer program is advantageously stored on a machine-readable storage medium.

An electrochemical energy storage system according to the invention is advantageously used for electric vehicles, hybrid vehicles, aircraft, plug-in hybrid vehicles, pedelecs or E-bikes, for portable telecommunications or data processing devices, for electrical hand tools or food processors, and in stationary stores for storing in particular regeneratively obtained electrical energy.

BRIEF DESCRIPTION OF THE DRAWINGS

Exemplary embodiments of the invention are illustrated in the drawing and explained in more detail in the following description.

In the drawing:

FIG. 1 shows a schematic illustration of a temperature profile of an electrochemical energy store during non-use; and

FIG. 2 shows a schematic illustration of a temperature-dependent period of the non-use of an electrochemical energy store.

Identical reference signs denote identical apparatus components in all of the figures.

DETAILED DESCRIPTION

FIG. 1 shows a schematic illustration of a temperature profile of an electrochemical energy store during non-use. Development of heat in an electrochemical energy store, in particular a high-voltage or low-voltage system, can be described by means of the following differential equation:

$m*c_p*\frac{dT_{\mathrm{cell}}}{\mathrm{dt}}={\stackrel{.}{Q}}_{\mathrm{heat}}+\alpha *A*\left(T_{\mathrm{Env}}-T_{\mathrm{cell}}\right)$

During use, for example during a charging or discharging process, of the electrochemical energy store, a power loss {dot over (Q)}_heat is produced on account of an internal resistance of the electrochemical energy store and the electrochemical energy store assumes a somewhat higher temperature than the environment T_Env. During non-use, the power loss {dot over (Q)}_heat is essentially zero and a temperature profile is dependent on a heat exchange with an environment of the electrochemical energy store and on a mechanical design of the electrochemical energy store with specific material properties, for example a mass m, a contact area A, a thermal conductivity α and a specific thermal capacity c_p of the electrochemical energy store.

A period of non-use of the electrochemical energy store can be calculated by means of a cooling behavior of the electrochemical energy store during non-use.

FIG. 1 shows a temperature profile of an electrochemical energy store, for example a 48 volt battery pack. The electrochemical energy store has been heated at an ambient temperature T_Env of 20° C. through use, for example through a discharging process, to a temperature T_t0 of 50° C. Non-use of the electrochemical energy store begins at a time t₀. The temperature profile illustrated corresponds to a cooling curve during non-use of the electrochemical energy store up to a time t₁ at which the electrochemical energy store is set in operation again. The electrochemical energy store is cooled at the time t₁ to a temperature Ta of 30° C.

The period t_off of non-use of the electrochemical energy store can be calculated in accordance with the formula

$t_{\mathrm{off}}=-\tau *\ln \left(\frac{T_{t1}-T_{\mathrm{Env}}}{T_{t0}-T_{\mathrm{Env}}}\right),$

wherein τ is a system constant, which comprises the material properties of the electrochemical energy store in accordance with

$\tau =\frac{m*c_p}{\alpha *A}.$

The system constant T_off can be determined, for example, analytically or experimentally. In the case of the experimental determination, the electrochemical energy store at a given ambient temperature TEnv can thus be brought to a higher temperature. By means of observing and measuring a temperature profile at a plurality of times during non-use of the electrochemical energy store, the system constant T can be identified by way of a standard method, for example least square. Ideally, the experimental parameter determination is carried out after the electrochemical energy store has been installed, for example in a vehicle. This can minimize measurement and model inaccuracies.

An accuracy of the identified period t_off of non-use can be identified by means of methods for error propagation. A first partial error

$\Delta t_1=\left|\frac{-\tau }{T_{t0}-T_{\mathrm{Env}}}\right|*\Delta T_{t1}$

is caused by a temperature measurement error upon restart of the electrochemical energy store, a second partial error

$\Delta t_2=\left|\frac{\tau }{T_{t0}-T_{\mathrm{Env}}}\right|*\Delta T_{t0}$

is caused by a temperature measurement error at the beginning of non-use of the electrochemical energy store and a third partial error

$\Delta t_3=\left|\frac{-\tau *\left(T_{t1}-T_{t0}\right)}{\left(T_{t1}-T_{\mathrm{Env}}\right)*\left(T_{t0}-T_{\mathrm{Env}}\right)}\right|*\Delta T_{\mathrm{En\nu }}$

is caused by a temperature measurement error of an ambient temperature of the electrochemical energy store. An overall error Δ_off^err in the calculation of the period t_off of non-use of the electrochemical energy store results from a sum of all of the partial errors t_off=Δt₁+Δt₂+Δt₃.

The inaccuracies of the individual input variables ΔT_t3, ΔT_t0, ΔT_Env can be determined experimentally, for example in a vehicle, since the measurement inaccuracy of a temperature of the electrochemical energy store increases when no power loss is produced in the electrochemical energy store in a short period of time, usually a few minutes, and a homogenous temperature distribution in the electrochemical energy store can be assumed.

A check for the plausibility of an electronic circuit for time measurement of an electrochemical energy storage system is effected by means of a cooling behavior of at least one electrochemical energy store during non-use of the electrochemical energy store in one advantageous embodiment by means of comparing a period t_off^Clock of non-use of the electrochemical energy store, which period is measured by the electronic circuit, with the calculated period t_off of non-use of the electrochemical energy store.

A difference between the measured period t_off^clock and the calculated period t_off must be within a tolerance range of the overall error Δt_off^err, otherwise the electronic circuit for time measurement has an error.

electronic circuit for time measurement functions in a fault free manner:

Δt_off^err≥|t_off^Clock−t_off|

electronic circuit for time measurement is faulty:

Δt_off^err<|t_off^Clock−t_off|

FIG. 2 shows a schematic illustration of a temperature-dependent period of the non-use of an electrochemical energy store. A difference T_t1−T_Env between a temperature T_t1 of the electrochemical energy store at the beginning of a restart of the electrochemical energy store and an ambient temperature T_Env of the electrochemical energy store is plotted on the abscissa. A difference T_t0−T_Env, between a temperature To of the electrochemical energy store at the beginning of non-use of the electrochemical energy store and an ambient temperature T_Env of the electrochemical energy store is plotted on the ordinate. For the illustration of the period of non-use calculated in accordance with the invention, as values for example 4 hours is assumed for the system constant τ and ΔT_t1=3 kelvins, ΔT_t2=6 kelvins and ΔT_Env=1.5 kelvins are assumed for the temperature measurement accuracies.

In a first example, a temperature difference T_t0−T_Env is 40 kelvins at a time of non-use of the electrochemical energy store. Upon restart, a temperature difference T_t1−T_Env is 10 kelvins. A temperature-dependent period 201 of non-use of the electrochemical energy store is approximately 5 hours.

In a second example, a temperature difference T_t0−T_Env is 30 kelvins at a time of non-use of the electrochemical energy store. Upon restart, a temperature difference T_N— Tg-_n, is 20 kelvins. A temperature-dependent period 202 of non-use of the electrochemical energy store is approximately 3 hours.

Claims

1. A method for checking the plausibility of an electronic circuit for time measurement of an electrochemical energy storage system by means of a cooling behavior of at least one electrochemical energy store during non-use of the electrochemical energy store, the method comprising the following steps: a) detecting an ambient temperature TEnv of the electrochemical energy store;b) detecting a temperature Tt0 of the electrochemical energy store at the beginning of the non-use of the electrochemical energy store;c) detecting a temperature Tt1 of the electrochemical energy store at the beginning of a restart of the electrochemical energy store;d) calculating a period toff of the non-use of the electrochemical energy store in accordance with the formula

2. The method for checking the plausibility of an electronic circuit for time measurement according to claim 1, further comprising the following step: h) generating an electrical, optical, acoustic and/or haptic signal when an error is identified in the electronic circuit for time measurement.

3. An electrochemical energy storage system comprising at least one electrochemical energy store, at least one sensor for detecting a temperature of the electrochemical energy store and/or an ambient temperature of the electrochemical energy store, an electronic circuit for time measurement and at least one means configured to carry out the steps of the method according to claim 1.

4. A computer program, comprising commands, which, when the computer program is executed by an electronic battery management control device, cause the device to execute the method according to claim 1.

5. A non-transitory, machine-readable storage medium, on which a computer program is stored, and which, if the computer program is executed by an electronic battery management control device, causes the electronic battery management control device to execute the method according to claim 1.

6. (canceled)

7. An electrochemical energy storage system comprising at least one electrochemical energy store, at least one sensor for detecting a temperature of the electrochemical energy store and/or an ambient temperature of the electrochemical energy store, an electronic circuit for time measurement and an electronic battery management control device configured to carry out the steps of the method according to claim 1.