CN112255453A - V2G-oriented electric automobile bidirectional electric energy metering method - Google Patents

V2G-oriented electric automobile bidirectional electric energy metering method Download PDF

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CN112255453A
CN112255453A CN202010984065.XA CN202010984065A CN112255453A CN 112255453 A CN112255453 A CN 112255453A CN 202010984065 A CN202010984065 A CN 202010984065A CN 112255453 A CN112255453 A CN 112255453A
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discharge
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崔家瑞
张宁宁
杨旭
张帅
李擎
王嘉玮
阎群
周静怡
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University of Science and Technology Beijing USTB
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    • G01MEASURING; TESTING
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Abstract

The invention provides a V2G-oriented bidirectional electric energy metering method for an electric automobile, and belongs to the field of electric energy metering of electric automobiles. The method comprises the following steps: establishing a bidirectional interaction model of the electric automobile connected to a power grid; wherein the two-way interaction model comprises: grid voltage u (t), grid line load Zl1、Zl2、Zl3Other loads Z in the power grid, electric automobile bidirectional inverter, electric automobile battery electromotive force E and electric automobile internal load Zev(ii) a Network voltage series connection Zl2、Zl3Then, the two-way inverter of the electric automobile is connected, ZevE is connected in series and then connected in parallel with two ends of a bidirectional inverter of the electric automobile, Z and Zl1After being connected in series, the two ends of the grid voltage are connected in parallel; and determining the electric energy measured during charging and the electric energy measured during discharging of the electric automobile under the distortion signal according to the established two-way interaction model. By adopting the invention, the aberration of the electric automobile can be realizedAnd bidirectional electric energy metering during charging and discharging under variable signals.

Description

V2G-oriented electric automobile bidirectional electric energy metering method
Technical Field
The invention relates to the field of electric automobile electric energy metering, in particular to a V2G-oriented electric automobile bidirectional electric energy metering method.
Background
The environmental and resource problems generated by the traditional fuel oil automobile are increasingly prominent, the fuel oil automobile is limited by successive strict measures in each country, and the new energy automobile plays an important role in relieving the pressure of oil shortage, reducing the emission of automobile tail gas, and promoting the transformation and upgrading of the automobile manufacturing industry and the sustainable development of the transportation industry. However, large-scale electric vehicle access to the grid also presents several challenges to the operation of the grid.
The electric Vehicle networking technology (V2G) describes a system in which an electric Vehicle is connected to a power Grid for bidirectional charging and discharging. The electric automobile can be used as a load to influence the power grid on one hand, and can be used as distributed energy storage equipment to provide electric energy for other users of the power grid during power utilization peak on the other hand. At present, the V2G technology has been widely concerned by scholars at home and abroad, and has achieved a series of achievements. Most researchers focus on intelligent scheduling, battery life, charging and discharging strategies and the like, and few documents relate to the problem of electric energy metering of V2G charging and discharging. Due to the nonlinear characteristic of a charging and discharging system of the electric automobile, the current electric energy metering method has unreasonable problems, and according to statistics of an electric power department, each charging pile has about 5% -30% of electric energy loss (the electric meter count is inconsistent with the charging amount of the electric automobile), and the reason is that the current electric energy meter metering principle is based on sine signal hypothesis. However, a large number of nonlinear loads are connected to the power grid nowadays, so that distorted signals exist in the power grid. The fundamental wave meter has not been able to meet the power metering in the current grid environment. Harmonic power is negative and is fed back to the power grid to become power grid garbage, the part of electric energy is converted from fundamental wave electric energy which is extracted from the power grid by the nonlinear load, the part of electric energy is useless and harmful, and the current electric energy metering method deducts the part of electric energy from the fundamental wave electric energy which is extracted from the power grid by the nonlinear load. At present, most electric vehicle charging models established by vast scholars at home and abroad are used for analyzing the influence of electric vehicles on a power grid or the aspects of optimized dispatching, economic benefit and the like of the power grid. These models are all built from a system perspective and cannot be used directly for power metering.
The signal types in the current power grid are very complex due to the access of a large number of nonlinear loads. Besides harmonic signals and simple harmonic signals, distortion signals of other forms exist in the power grid, and especially unstable distortion signals such as impact signals cannot be described by a harmonic model at all. Typical unsteady distortion signals in the grid are surge signals and ripple signals, assuming that for the kth surge or ripple, the current i in the grid circuitk(t) is
ik(t)=(1+αk(t))Imk sin(ω0t+φk) (1)
In the formula, alphak(t) is the kth impact function, Imk、φkCurrent amplitude and current phase, omega, respectively0And t represents the time, which is the standard power frequency angular frequency. For the convenience of metering, the zero point of the metering time is alphakThe time at which (t) occurs is standard. If the signal is an impulsive signal, alphak(t) can be approximately represented as
Figure BDA0002688534890000021
Wherein M isk>0 (2)
In the formula, MkThe amplitude of the k-th impact signal is obtained; t is tkThe duration of the kth impact signal;
if the signal is a wobble signal, αk(t) can be approximately represented as
Figure BDA0002688534890000022
In the formula, MkIs the amplitude of the kth fluctuation signal; t is tkThe kth wobble signal duration.
Since the time at which the fluctuations occur is uncertain, the duration tkIs random. When M iskWhen the voltage is more than 1, the amplitude of the fluctuation current is more than that of the fundamental wave current, and the voltage drops; when M isk<At 1, the amplitude of the ripple current is smaller than that of the fundamental current, and the voltage rises.
Under the condition of distorted signals, the voltage u (t) at a certain metering point in the power grid and the current i (t) flowing into the metering point can be expressed by the following formula:
u(t)=uI(t)+uS(t) (4)
i(t)=iI(t)+iS(t) (5)
in the formula uI(t)、uS(t) fundamental voltage and distortion voltage at the measurement point, iI(t)、iS(t) are the fundamental current and the distortion current at the metering point, respectively.
On the basis, scholars establish a charging model and a discharging model of the electric automobile in a power grid, and provide an electric energy metering formula during charging or discharging.
Taking the charging of the electric vehicle in the power grid as an example, fig. 1 is a charging model of the electric vehicle in the power grid. As shown in fig. 1, the left side of the circuit is a Power grid (Power grid) simplified model. u (t) is the grid instantaneous voltage; i (t) is the instantaneous current in the line; zlAs a line load on the grid side during charging; on the right side of the circuit, an electric vehicle (electric vehicle) simplified model is provided, and the electric vehicle is equivalent to a pure load Z during charging. The design time is T, and for the sake of discussion, T is assumed to be N.T0,T0The fundamental wave period is N, which represents the number of impacts/undulations and is an integer. At the kth impact or surge, the instantaneous power p at point a is measuredak(t) is
pak(t)=uak(t)·ik(t) (6)
In the formula uak(t) represents the point voltage at metering point a at the kth bump or surge; u. ofak(t) represents the voltage at the kth shock or fluctuation metering point a;
combining the formulas (4) and (5), one can obtain
Figure BDA0002688534890000033
Wherein, UakI(t) is the fundamental voltage at the metering point a at the time of the kth surge or fluctuation, ikI(t) is the fundamental current at the kth surge or surge, uakS(t) is the distortion voltage at the metering point a at the kth impact or fluctuation, ikS(t) is a distortion current at the time of the kth impact or fluctuation.
So the average power (active power) P at the metering point a at the kth surge or fluctuationakComprises the following steps:
Figure BDA0002688534890000031
in the formula, PakI、PakIs、PaksI、PaksThe fundamental wave power at the point a, the power generated by the action of the fundamental wave voltage and the distortion current, the power generated by the action of the distortion voltage and the fundamental wave current and the distortion power are measured when the shock or the fluctuation occurs at the kth time respectively.
Assuming that there are N impacts or fluctuations within the power metering time T, where N is a random positive integer, the average power P at the metering point aaComprises the following steps:
Figure BDA0002688534890000032
in the formula, PI、PIS、PSI、PSAnd respectively measuring the fundamental wave power at the point a, the power generated by the action of the fundamental wave voltage and the distortion current, the power generated by the action of the distortion voltage and the fundamental wave current and the distortion power.
Various researches are integrated, and the conclusion that the electric automobile is connected in the power grid for charging is obtained:
PIgreater than 0, fundamental waveThe power generated by the voltage and the fundamental wave current is positive, that is, the fundamental wave power is positive, which indicates that the electric energy generated by the fundamental wave power belongs to the electric energy absorbed by the electric vehicle from the power grid during the charging time of the electric vehicle in the power grid.
PISNot less than 0, the power generated by the fundamental voltage and the distortion current is not negative (only containing the harmonic wave is 0), namely the electric energy absorbed by the electric automobile from the power grid.
PSIThe power generated by the distortion voltage and the fundamental wave current is not positive (0 when only the harmonic wave is contained), which indicates that the part of electric energy flows into the power grid, but is fed back to the power grid in a mode of the fundamental wave current, and the power grid is not polluted.
PS<0, the distortion power is negative, and the part of electric energy also flows into the power grid and is fed back to the power grid in a distortion current mode to pollute the power grid. The part of electric energy is not ignored, and is charged by the user of the electric automobile without metering.
In combination with the above analysis, the power to be measured when the electric vehicle is charged in the power grid is as follows:
P=PI+PIS+PSI (10)
=(PI+PIS+PSI+PS)-PS
=Pa-PS
where P represents the total power that should be metered;
in fact, the process of discharging the electric vehicle on the power grid is opposite to that of charging the electric vehicle, and the influence of the distorted signal on the circuit needs to be considered. However, the above-mentioned energy metering formula is only applicable to the case where the electric vehicle is only charged or only discharged in the grid. The charging and discharging behaviors of the electric automobile connected in the power grid have higher randomness, and the establishment of a uniform two-way interaction model has more practical significance for V2G electric energy metering.
In the prior art, a charging model and a discharging model of an electric vehicle in a power grid are established, and an electric energy metering formula during charging or discharging is provided, but the electric energy metering modes have limitations and are only suitable for the situation that the electric vehicle is only charged or only discharged in the power grid. At present, a bidirectional interaction model aiming at electric automobile electric energy metering does not exist, and charging and discharging bidirectional electric energy metering cannot be realized.
Disclosure of Invention
The embodiment of the invention provides a V2G-oriented bidirectional electric energy metering method for an electric vehicle, which can realize bidirectional electric energy metering during charging and discharging of the electric vehicle under a distorted signal. The technical scheme is as follows:
the embodiment of the invention provides a V2G-oriented bidirectional electric energy metering method for an electric vehicle, which comprises the following steps:
establishing a bidirectional interaction model of the electric automobile connected to a power grid; wherein the two-way interaction model comprises: grid voltage u (t), grid line load Zl1、Zl2、Zl3Other loads Z in the power grid, electric automobile bidirectional inverter, electric automobile battery electromotive force E and electric automobile internal load Zev(ii) a Network voltage series connection Zl2、Zl3Then, the two-way inverter of the electric automobile is connected, ZevE is connected in series and then connected in parallel with two ends of a bidirectional inverter of the electric automobile, Z and Zl1After being connected in series, the two ends of the grid voltage are connected in parallel;
and determining the electric energy measured during charging and the electric energy measured during discharging of the electric automobile under the distortion signal according to the established two-way interaction model.
Further, under the condition of the distorted signal, the grid voltage u (t) is:
u(t)=Um sin(ω0t+ψk)
wherein, UmIs the grid voltage amplitude; omega0Is the standard power frequency angular frequency; psikVoltage phase for the kth surge or fluctuation; t is the time.
Furthermore, in the power grid, at Zl2、Zl3The point on the line between is the metering point a;
is provided with Zl2、Zl3Are all pure resistive loads RlWhen the electric automobile is charged in the power grid or the electric automobile is discharged into the power grid,the voltage at metering point a is:
ua(t)=u(t)-Rlia(t)
wherein u isa(t) is the voltage at metering point a; i.e. ia(t) is the current at metering point a;
with electric automobile charge direction as the positive direction, when electric automobile discharges to the electric wire netting, to k impact or undulant under the distortion signal condition, current is in metering point a:
iak(t)=-(1+αk(t))Imk sin(ω0t+φk)
wherein iak(t) represents the current at the kth impact or fluctuation metering point a; alpha is alphak(t) denotes the kth-time impact function; i ismk、φkThe current amplitude and the current phase of the kth impact or fluctuation are respectively.
Further, for the kth impact or fluctuation, the voltage at the metering point a is:
uak(t)=u(t)-Rliak(t)
=Um sin(ω0t+ψk)+Rl[1+αk(t)]Imk sin(ω0t+φk)
=Um sin(ω0t+ψk)+RlImk sin(ω0t+φk)+Rlαk(t)Imk sin(ω0t+φk)
=Um sinω0tcosψk+Um sinψk cosω0t+RlImk sinω0tcosφk
+RlImk sinφk cosω0t+RlImkak(t)sin(ω0t+φk)
=uakI(t)+uakS(t)
uakI(t)=Um sinω0tcosψk+Um sinψk cosω0t+RlImk sinω0tcosφk
+RlImk sinφk cosω0t
=(Um cosψk+RlImk cosφk)sinω0t
+(Um sinψk+RlImk sinφk)cosω0t
=UakIm sin(ω0t+θk)
Figure BDA0002688534890000051
Figure BDA0002688534890000052
uakS(t)=RlImkαk(t)sin(ω0t+φk)
wherein u isak(t) represents the voltage at the kth shock or fluctuation metering point a; u. ofakI(t)、uakS(t) the fundamental voltage and the distortion voltage at the k-th impact or fluctuation metering point a respectively; u shapeakImThe fundamental voltage amplitude at the k-th impact or fluctuation metering point a is obtained; thetakIs the fundamental voltage phase;
fundamental current i at k-th impact or fluctuation metering point aakI(t) is:
iakI(t)=-Imk sin(ω0t+φk)
distortion current i at k-th impact or fluctuation metering point aaks(t) is:
iakS(t)=-Imkαk(t)sin(ω0t+φk)。
further, the determining, according to the established bidirectional interaction model, the electric energy measured during charging and the electric energy measured during discharging of the electric vehicle under the distortion signal includes:
according to the established two-way interaction model, determining the average power at the metering point a in the metering time:
Figure BDA0002688534890000061
Figure BDA0002688534890000062
Figure BDA0002688534890000063
wherein, PaIs the average power at metering point a over the metering time T; pakThe average power at the metering point a in the time when the kth impact exists; p is a radical ofak(t) measuring the instantaneous power at the point a during the time when the kth impact exists; t is N.T0,T0The fundamental wave period is N represents the impact times; t is1=N1T0,T1Metering time for charging, N1Representing the number of times the impact occurred during the charging process; t is2=N2T0,T2For measuring time of discharge, N2Indicating the number of times the impact occurred during the discharge; pa_chargeThe average power at the metering point a in the charging metering time is; pa_dischargeIs the average power at metering point a during the discharge metering time; pI_charge、PIS_charge、PSI_charge、PS_chargeThe power generated by the action of the fundamental wave power, the fundamental wave voltage and the distortion current during charging, and the work and the distortion power generated by the action of the distortion voltage and the fundamental wave current are respectively; pI_discharge、PIS_discharge、PSI_discharge、PS_dischargeThe power generated by the action of the fundamental wave power, the fundamental wave voltage and the distortion current during discharging, the power generated by the action of the distortion voltage and the fundamental wave current and the distortion power are respectively;
according to the obtained Pa_chargeAnd PS_chargeDetermining the electric energy W measured during chargingcharge
According to the obtained Pa_dischargeAnd PS_dischargeDetermining the electric energy W measured during dischargedischarge
Further, PS_dischargeExpressed as:
Figure BDA0002688534890000071
further, WchargeExpressed as:
Wcharge=(PI_charge+PIS_charge+PSI_charge)T1
=(Pa_charge-PS_charge)T1
=Wa_charge-WS_charge
wherein, Wa_chargeMeasuring the charging power at point a, Wa_charge=Pa_charge*T1;WS_chargeDistortion of electric energy during charging, WS_charge=PS_charge*T1
Further, WdischargeExpressed as:
Wdischarge=(PI_discharge+PIS_discharge+PSI_discharge)T2
=(Pa_discharge-PS_discharge)T2
=Wa_discharge-WS_discharge
wherein, Wa_dischargeMeasuring the discharge power at point a, Wa_discharge=Pa_discharge*T2;WS_dischargeElectric energy distorted during discharge, WS_discharge=PS_discharge*T2
Further, the method further comprises:
and summing the determined electric energy measured during charging and the determined electric energy during discharging to obtain the total electric energy measured by bidirectional charging and discharging.
The technical scheme provided by the embodiment of the invention has the beneficial effects that at least:
in the embodiment of the invention, aiming at the fact that the charging and discharging behaviors of the electric automobile connected to the power grid have high randomness, a uniform two-way interaction model of the electric automobile connected to the power grid is established; and according to the established bidirectional interaction model, bidirectional electric energy metering of the electric automobile during charging and discharging under the distorted signal is realized.
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In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the drawings needed to be used in the description of the embodiments will be briefly introduced below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art to obtain other drawings based on these drawings without creative efforts.
FIG. 1 is a schematic diagram of a charging model of an electric vehicle in a power grid;
FIG. 2 is a schematic diagram of a bidirectional interaction model of an electric vehicle connected to a power grid according to an embodiment of the present invention;
fig. 3 is a schematic flow chart of a V2G-oriented electric vehicle bidirectional electric energy metering method according to an embodiment of the present invention.
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more apparent, embodiments of the present invention will be described in detail with reference to the accompanying drawings.
As shown in fig. 2 and fig. 3, an embodiment of the present invention provides a bidirectional electric energy metering method for a V2G-oriented electric vehicle, where the method includes:
s101, establishing a bidirectional interaction model of the electric automobile connected to a power grid; wherein the two-way interaction model comprises: grid voltage u (t), grid line load Zl1、Zl2、Zl3Other loads Z in the power grid, electric automobile bidirectional inverter, electric automobile battery electromotive force E and electricityInternal load Z of motor vehicleev(ii) a Network voltage series connection Zl2、Zl3Then, the two-way inverter of the electric automobile is connected, ZevE is connected in series and then connected in parallel with two ends of a bidirectional inverter of the electric automobile, Z and Zl1After being connected in series, the two ends of the grid voltage are connected in parallel;
and S102, determining the electric energy measured during charging and the electric energy measured during discharging of the electric automobile under the distortion signal according to the established two-way interaction model.
According to the V2G-oriented bidirectional electric energy metering method for the electric automobile, a uniform bidirectional interaction model of the electric automobile connected to a power grid is established aiming at the fact that the charging and discharging behaviors of the electric automobile connected to the power grid have high randomness; and according to the established bidirectional interaction model, bidirectional electric energy metering of the electric automobile during charging and discharging under the distorted signal is realized.
In this example, Zl1、Zl2、Zl3Both represent grid line loads, and other loads Z in the grid include: loads other than line loads and electric vehicles in the power grid, for example, lighting loads, household loads such as air conditioners and refrigerators, and loads such as industrial electric appliances.
In fig. 2, the simplified model of the power grid is shown on the left side of the circuit, and the electric vehicle is shown on the right side of the circuit. Taking the current direction shown in fig. 2 as the positive direction, when the electric vehicle is charged, the Bi-directional inverter (Bi-directional Converter) of the electric vehicle controls the current to flow into the electric vehicle from the point b; when the electric automobile discharges, the bidirectional inverter controls the current to flow out to the point b from the electric automobile, and the current and the grid voltage are the load (comprising: Z) in the gridl1、Zl2、Zl3And Z) power supply.
In FIG. 2, in the power grid, at Zl2、Zl3The points on the line between the points are metering points a, i (t) are network currents, ua(t) is the voltage at the measurement point a, ia(t) is the current at metering point a, uevAnd (t) is the output voltage of the electric automobile when discharging to the power grid.
Under distorted signal conditions, the grid voltage u (t) can be expressed as:
u(t)=Um sin(ω0t+ψk) (11)
wherein, UmIs the grid voltage amplitude; omega0Is the standard power frequency angular frequency; psikFor the phase of the voltage of the kth surge or surge, psikIs a random variable; t is the time.
Taking the current direction shown in fig. 2 as the positive direction, that is, the charging direction of the electric vehicle as the positive direction, the current flowing into the metering point a during the charging of the electric vehicle can be obtained according to the equation (1):
ia(t)=(1+α(t))Imsin(ω0t+φ) (12)
wherein ia(t) is the current at the metering point a, α (t) is the impulse function, ImPhi is the current amplitude and current phase, respectively.
In this embodiment, the expression of α (t) depends on whether the signal is an impulse signal or a ripple signal, as shown in equations (2) and (3).
Similarly, the current flowing into the metering point a during the discharge of the electric automobile is as follows:
ia(t)=-(1+α(t))Imsin(ω0t+φ) (13)
when the electric automobile is charged in a power grid, the voltage at the point a of the metering point is as follows:
ua(t)=u(t)-Zl2ia(t) (14)
wherein u isa(t) is the voltage at metering point a;
when the electric automobile discharges to the power grid, the voltage at the point a is measured
ua(t)=uev(t)-Zl3ia(t) (15)
Wherein u isev(t) is the output voltage of the electric vehicle discharging to the power grid;
in fact, the output voltage u of the electric vehicle when discharging into the gridev(t) is practically the same as the grid voltage u (t), which is a standard sinusoidal voltage, then:
uev(t)=u(t) (16)
suppose Zl2、Zl3Are all pure resistive loads RlMeasuring the voltage u at point a in the case of charging or discharging V2Ga(t) can be expressed in the form:
ua(t)=u(t)-Rlia(t) (17)
taking the electric vehicle discharge as an example for analysis, under the condition of distorted signals, for the kth impact or fluctuation, the current at the metering point a is as follows:
iak(t)=-(1+αk(t))Imk sin(ω0t+φk) (18)
wherein iak(t) represents the current at the kth impact or fluctuation metering point a; alpha is alphak(t) denotes the kth-time impact function; i ismk、φkThe current amplitude and the current phase of the kth impact or fluctuation are respectively;
for the kth bump or fluctuation, the voltage at metering point a is:
Figure BDA0002688534890000101
wherein u isak(t) represents the voltage at the kth shock or fluctuation metering point a; u. ofakI(t)、uakS(t) the fundamental voltage and the distortion voltage at the k-th impact or fluctuation metering point a respectively;
according to equation (19), the voltage at the metering point a can be divided into a fundamental voltage uakI(t) and distortion voltage uaks(t), wherein the fundamental voltage is:
Figure BDA0002688534890000104
Figure BDA0002688534890000102
Figure BDA0002688534890000103
wherein, UakImThe fundamental voltage amplitude at the k-th impact or fluctuation metering point a is obtained; thetakIs the fundamental voltage phase;
the distortion voltage at the measurement point a is:
uakS(t)=RlImkαk(t)sin(ω0t+φk) (23)
according to equation (23), the current at measurement point a can be divided into fundamental current iakI(t) and a distortion current iaks(t) wherein the fundamental current i at the kth impact or fluctuation metering point aakI(t) is:
iakI(t)=-Imk sin(ω0t+φk) (24)
distortion current i at k-th impact or fluctuation metering point aaks(t) is:
iakS(t)=-Imkαk(t)sin(ω0t+φk) (25)
for convenience of description, it is assumed that T is N · T during the measurement time T0,T0N represents the number of impacts, and essentially, N represents the sum of the number of impacts and undulations. The charging metering time of the electric automobile is T1Discharge metering time of T2. Theoretically, T1>T2For convenience of measurement, assume that within the measurement time T, N1When the secondary impact occurs in the charging process, the charging metering time is T1=N1T0;N2The sub-impact occurs in the discharge process, and the discharge metering time is T2=N2T0(ii) a The average power (active power) P at the metering point a during the metering time can be obtainedaComprises the following steps:
Figure BDA0002688534890000111
wherein, PaIs the average power at metering point a over the metering time; pakThe average power at the metering point a in the time when the kth impact exists; p is a radical ofak(t) is the time during which the kth impact is present, the meterThe instantaneous power at quantity point a;
Figure BDA0002688534890000112
wherein, Pa_chargeIs the average power at metering point a over the charge metering time; pa_dischargeIs the average power at metering point a during the discharge metering time;
as can be seen from equation (27), the power at the metering point a can be divided into four parts in the charging metering time and the discharging metering time:
Figure BDA0002688534890000113
wherein, PI_charge、PIS_charge、PSI_charge、PS_chargeThe power generated by the action of the fundamental wave power, the fundamental wave voltage and the distortion current during charging, and the work and the distortion power generated by the action of the distortion voltage and the fundamental wave current are respectively; pI_discharge、PIS_discharge、PSI_discharge、PS_dischargeThe power generated by the action of the fundamental wave power, the fundamental wave voltage and the distortion current during discharging, the power generated by the action of the distortion voltage and the fundamental wave current and the distortion power are respectively;
take the discharging process of the electric vehicle as an example, P is sequentially pairedI_discharge、PIS_discharge、PSI_discharge、PS_dischargeThe four parts of power are analyzed:
1. fundamental power P during dischargeI_discharge
As can be seen from equations (20) and (24), the fundamental instantaneous power at the measurement point a is:
Figure BDA0002688534890000121
wherein, the first term is alternating current component, the mean value is zero, and represents power second harmonic; the second term is a direct current component, which indicates the average power of the fundamental voltage and the fundamental current, and must be positive.
Figure BDA0002688534890000122
2. Power P generated by action of wave voltage and distorted current during dischargeIS_discharge
As can be seen from equations (20) and (25), the instantaneous power generated by the action of the fundamental voltage and the distortion current at the measurement point a is:
Figure BDA0002688534890000123
for a surge signal or a surge signal, the energy accumulation time can be regarded as infinitely long, so that the total electrical energy E generated in the metering timeIS_dischargeComprises the following steps:
Figure BDA0002688534890000124
1) if the signal is a wobble signal, then
Figure BDA0002688534890000125
Wherein, ImkThe current amplitude of the kth fluctuation signal is obtained; t is tkFor the duration of the kth wobble signal
Then the formula (32) is
Figure BDA0002688534890000131
Wherein, the first term and the second term are random terms, and the sum of multiple fluctuations tends to zero. Third term cos (θ)kk) The one must be positive and is generally not very small, less than 0.5, not uncommon under current constraints on the power factor of the grid. The third term is therefore positive. Thus is provided with
EIS_diacharge≤0 (35)
2) If the signal is an impact signal, then:
Figure BDA0002688534890000141
wherein, γkIn a simplified form, the method specifically comprises the following steps:
Figure BDA0002688534890000142
therefore, formula (32) can be written as
Figure BDA0002688534890000151
When t iskOn a time scale of → 0,
EIS_discharge→0 (39)
when t isk>T0When the temperature of the water is higher than the set temperature,
Figure BDA0002688534890000152
0tkis greater than 1, so
Figure BDA0002688534890000153
Where the first term is a positive value and the second term is a random variable, the sum of multiple hits will tend to zero. Therefore, it is not only easy to use
Figure BDA0002688534890000154
Combine formula (35) and (41) to know
EIS_discharge≤0 (42)
Energy E generated by action of fundamental voltage and distortion currentIS_dischargeMust not be greater than zero, and because,
Figure BDA0002688534890000155
so the average power PIS_dischargeMust also be no greater than 0, so there is:
PIS_discharge≤0 (43)
3. power P generated by action of distortion voltage and fundamental current during dischargeSI_discharge
As is clear from the equations (23) and (24), the instantaneous power generated by the action of the distortion voltage and the fundamental current at the measurement point a is
Figure BDA0002688534890000156
The average power is:
Figure BDA0002688534890000161
thus, the sum of the first term and the second term is not greater than 0, i.e.
PSI_discharge≤0 (46)
4. Distortion power P at dischargeS_discharge
As is clear from the expressions (23) and (25), the distortion instantaneous power at the measurement point a is
Figure BDA0002688534890000162
Average power:
Figure BDA0002688534890000163
thus, the sum of the first term and the second term is less than 0, i.e.
PS_discharge<0 (49)
In combination with the above analysis, the electric vehicle has the following conclusions during the discharging process:
PI_discharge<0, the fundamental power is negative, and the electric automobile supplies power to a power grid and needs to be measured.
PIS_dischargeLess than or equal to 0, the power generated by the action of the fundamental voltage and the distortion current is not positive (0 when only the harmonic is contained), and the electric automobile provides electric quantity and needs to be measured.
PSI_dischargeLess than or equal to 0, the power generated by the action of the distortion voltage and the fundamental wave current is not positive (0 when only the harmonic wave is contained), and the power grid absorbs energy and needs to be measured.
PS_discharge<0, the distortion power is negative, and the electric automobile supplies power to the power grid, but flows into the power grid in a distortion current mode, so that the power grid is polluted and is not measured.
Therefore, a reasonable formula for electricity metering at discharge should be:
Figure BDA0002688534890000172
wherein, WdischargeThe electric energy is measured during discharging; wa_dischargeTo measure the discharge power at point a, Wa_discharge=Pa_discharge*T2;WS_dischargeFor distorting electric energy during discharge, WS_discharge=PS_discharge*T2
The formula derivation of the charging process of the electric vehicle is similar to the discharging process, and only the current direction needs to be noticed to be opposite, and the description is omitted here. Therefore, it can be concluded when the electric vehicle is charged:
PI_chargeand if the power is more than 0, the fundamental wave power is positive, and the power grid supplies power to the electric automobile and needs to measure.
PIS_chargeNot less than 0, the power generated by the action of the fundamental voltage and the distortion current is not negative (only containing the harmonic wave, the power is 0), and the power grid supplies power to the electric automobile and needs to be measured.
PSI_chargeLess than or equal to 0, the power generated by the action of the distortion voltage and the fundamental wave current is not positive (0 when only the harmonic wave is contained), but the power is fed back to the power grid in a mode of the fundamental wave current, and the power grid is not polluted.
PS_charge<And 0, the distortion power is negative and is fed back to the power grid in a distortion current mode, and although the part feeds back electric energy to the power grid, the part pollutes the power grid and is not measured.
In this example, PS_chargeExpressed as:
Figure BDA0002688534890000171
therefore, a reasonable formula for measuring the electric quantity during charging is
Figure BDA0002688534890000173
Wherein, WchargeElectric energy measured during charging; wa_chargeFor measuring the charging power at point a, Wa_charge=Pa_charge*T1;WS_chargeFor distorting electric energy during charging, WS_charge=PS_charge*T1
In the metering time T, the electricity metering formula at the metering point a is as follows:
Figure BDA0002688534890000183
Figure BDA0002688534890000181
wherein, WaTo measure the quantity of electricity at point a, WIAs fundamental electric energy, WISElectric energy produced for fundamental voltage and distortion current action, WISElectric energy produced for the action of distorted voltage and fundamental current, WSIs distortion power;
in the foregoing embodiment of the V2G-oriented bidirectional electric energy metering method for the electric vehicle, further, the method further includes:
and summing the determined electric energy measured during charging and the determined electric energy during discharging to obtain the total electric energy measured by bidirectional charging and discharging.
In this embodiment, in combination with equations (50) and (51), the rational measure equation should be:
Figure BDA0002688534890000182
wherein W represents the total electric energy measured by bidirectional charge and discharge, and Wa=Pa_chargeT1+Pa_dischargeT2,WS=Pa_chargeT1+Pa_dischargeT2
The above description is only for the purpose of illustrating the preferred embodiments of the present invention and is not to be construed as limiting the invention, and any modifications, equivalents, improvements and the like that fall within the spirit and principle of the present invention are intended to be included therein.

Claims (9)

1. A V2G-oriented bidirectional electric energy metering method for an electric automobile is characterized by comprising the following steps:
establishing a bidirectional interaction model of the electric automobile connected to a power grid; wherein the two-way interaction model comprises: grid voltage u (t), grid line load Zl1、Zl2、Zl3Other loads Z in the power grid, electric automobile bidirectional inverter, electric automobile battery electromotive force E and electric automobile internal load Zev(ii) a Network voltage series connection Zl2、Zl3Then, the two-way inverter of the electric automobile is connected, ZevE is connected in series and then connected in parallel with two ends of a bidirectional inverter of the electric automobile, Z and Zl1After being connected in series, the two ends of the grid voltage are connected in parallel;
and determining the electric energy measured during charging and the electric energy measured during discharging of the electric automobile under the distortion signal according to the established two-way interaction model.
2. The V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 1, wherein under the condition of distorted signals, the grid voltage u (t) is:
u(t)=Um sin(ω0t+ψk)
wherein, UmIs the grid voltage amplitude; omega0Is the standard power frequency angular frequency; psikVoltage phase for the kth surge or fluctuation; t is the time.
3. The V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 2, wherein the power grid is located at Zl2、Zl3The point on the line between is the metering point a;
is provided with Zl2、Zl3Are all pure resistive loads RlWhen the electric automobile is charged in the power grid or discharged into the power grid, the voltage at the metering point a is as follows:
ua(t)=u(t)-Rlia(t)
wherein u isa(t) is the voltage at metering point a; i.e. ia(t) is the current at metering point a;
with electric automobile charge direction as the positive direction, when electric automobile discharges to the electric wire netting, to k impact or undulant under the distortion signal condition, current is in metering point a:
iak(t)=-(1+αk(t))Imk sin(ω0t+φk)
wherein iak(t) represents the current at the kth impact or fluctuation metering point a; alpha is alphak(t) denotes the kth-time impact function; i ismk、φkThe current amplitude and the current phase of the kth impact or fluctuation are respectively.
4. The V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 3, wherein for the kth impact or fluctuation, the voltage at the metering point a is:
uak(t)=u(t)-Rliak(t)
=Um sin(ω0t+ψk)+Rl[1+αk(t)]Imk sin(ω0t+φk)
=Um sin(ω0t+ψk)+RlImk sin(ω0t+φk)+Rlαk(t)Imk sin(ω0t+φk)
=Um sinω0tcosψk+Um sinψk cosω0t+RlImk sinω0tcosφk+RlImk sinφk cosω0t+RlImkαk(t)sin(ω0t+φk)
=uakI(t)+uakS(t)
uakI(t)=Um sinω0tcosψk+Um sinψk cosω0t+RlImk sinω0tcosφk+RlImk sinφk cosω0t
=(Um cosψk+RlImk cosφk)sinω0t+(Um sinψk+RlImk sinφk)cosω0t
=UakIm sin(ω0t+θk)
Figure FDA0002688534880000021
Figure FDA0002688534880000022
uakS(t)=RlImkαk(t)sin(ω0t+φk)
wherein u isak(t) represents the voltage at the kth shock or fluctuation metering point a; u. ofakI(t)、uakS(t) the fundamental voltage and the distortion voltage at the k-th impact or fluctuation metering point a respectively; u shapeakImIs as followsThe fundamental voltage amplitude at the k times of impact or fluctuation metering point a; thetakIs the fundamental voltage phase;
fundamental current i at k-th impact or fluctuation metering point aakI(t) is:
iakI(t)=-Imk sin(ω0t+φk)
distortion current i at k-th impact or fluctuation metering point aaks(t) is:
iakS(t)=-Imkαk(t)sin(ω0t+φk)。
5. the V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 4, wherein the determining of the electric vehicle under the distorted signal, the electric energy metered during charging and the electric energy metered during discharging according to the established bidirectional interaction model comprises:
according to the established two-way interaction model, determining the average power at the metering point a in the metering time:
Figure FDA0002688534880000023
Figure FDA0002688534880000031
Figure FDA0002688534880000032
wherein, PaIs the average power at metering point a over the metering time T; pakThe average power at the metering point a in the time when the kth impact exists; p is a radical ofak(t) measuring the instantaneous power at the point a during the time when the kth impact exists; t is N.T0,T0The fundamental wave period is N represents the impact times; t is1=N1T0,T1The time is measured for the purpose of charging,N1representing the number of times the impact occurred during the charging process; t is2=N2T0,T2For measuring time of discharge, N2Indicating the number of times the impact occurred during the discharge; pa_chargeThe average power at the metering point a in the charging metering time is; pa_dischargeIs the average power at metering point a during the discharge metering time; pI_charge、PIS_charge、PSI_charge、PS_chargeThe power generated by the action of the fundamental wave power, the fundamental wave voltage and the distortion current during charging, and the work and the distortion power generated by the action of the distortion voltage and the fundamental wave current are respectively; pI_discharge、PIS_discharge、PSI_discharge、PS_dischargeThe power generated by the action of the fundamental wave power, the fundamental wave voltage and the distortion current during discharging, the power generated by the action of the distortion voltage and the fundamental wave current and the distortion power are respectively;
according to the obtained Pa_chargeAnd PS_chargeDetermining the electric energy W measured during chargingcharge
According to the obtained Pa_dischargeAnd PS_dischargeDetermining the electric energy W measured during dischargedischarge
6. The V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 5, wherein P is PS_dischargeExpressed as:
Figure FDA0002688534880000033
7. the V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 5, wherein W is WchargeExpressed as:
Wcharge=(PI_charge+PIS_charge+PSI_charge)T1
=(Pa_charge-PS_charge)T1
=Wa_charge-WS_charge
wherein, Wa_chargeMeasuring the charging power at point a, Wa_charge=Pa_charge*T1;WS_chargeDistortion of electric energy during charging, WS_charge=PS_charge*T1
8. The V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 5, wherein W is WdischargeExpressed as:
Wdischarge=(PI_discharge+PIS_discharge+PSI_discharge)T2
=(Pa_discharge-PS_discharge)T2
=Wa_discharge-WS_discharge
wherein, Wa_dischargeMeasuring the discharge power at point a, Wa_discharge=Pa_discharge*T2;WS_dischargeElectric energy distorted during discharge, WS_discharge=PS_discharge*T2
9. The V2G-oriented electric vehicle bidirectional electric energy metering method according to claim 1, characterized in that the method further comprises:
and summing the determined electric energy measured during charging and the determined electric energy during discharging to obtain the total electric energy measured by bidirectional charging and discharging.
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