CN106501740B - Superconducting magnet quench detection method and device - Google Patents

Superconducting magnet quench detection method and device Download PDF

Info

Publication number
CN106501740B
CN106501740B CN201610843208.9A CN201610843208A CN106501740B CN 106501740 B CN106501740 B CN 106501740B CN 201610843208 A CN201610843208 A CN 201610843208A CN 106501740 B CN106501740 B CN 106501740B
Authority
CN
China
Prior art keywords
quench
coil
voltage
temperature
unit
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201610843208.9A
Other languages
Chinese (zh)
Other versions
CN106501740A (en
Inventor
陈盼盼
诸嘉慧
丘明
张宏杰
刘二伟
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
State Grid Corp of China SGCC
China Electric Power Research Institute Co Ltd CEPRI
Electric Power Research Institute of State Grid Liaoning Electric Power Co Ltd
Original Assignee
State Grid Corp of China SGCC
China Electric Power Research Institute Co Ltd CEPRI
Electric Power Research Institute of State Grid Liaoning Electric Power Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by State Grid Corp of China SGCC, China Electric Power Research Institute Co Ltd CEPRI, Electric Power Research Institute of State Grid Liaoning Electric Power Co Ltd filed Critical State Grid Corp of China SGCC
Priority to CN201610843208.9A priority Critical patent/CN106501740B/en
Publication of CN106501740A publication Critical patent/CN106501740A/en
Application granted granted Critical
Publication of CN106501740B publication Critical patent/CN106501740B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/12Measuring magnetic properties of articles or specimens of solids or fluids
    • G01R33/1238Measuring superconductive properties

Abstract

The invention provides a superconducting magnet quench detection method and device, the method includes detecting the voltage and current of each unit coil in real time; calculating the power difference between two adjacent unit coils, and solving the absolute value of the power difference between the unit coil and the two adjacent unit coils; and if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, judging that the unit coil is in a power quench state. The invention detects the power quench state of the unit coil, and accurately positions the position of the unit coil in the power quench state through comparison; respectively detecting voltage and temperature quench states of the single coils, and accurately positioning the positions of the single coils in the voltage and temperature quench states step by step through comparison; the invention integrates the detection of the electric quantity and the non-electric quantity, and overcomes the defect of a single quench detection method. And meanwhile, a voltage correction coefficient is introduced, so that the reliability of superconducting magnet quench detection is greatly improved.

Description

Superconducting magnet quench detection method and device
Technical Field
The invention relates to a quench detection method, in particular to a quench detection method and a quench detection device for a superconducting magnet.
Background
The superconducting energy storage system can be used for improving the stability of the system, improving the power supply quality, storing electric energy in a dispersed power supply system containing new energy such as solar energy, wind energy and the like and improving the power output characteristic in a power system, and can also be used for an emergency power supply of important devices. These excellent properties of superconducting energy storage systems would bring immeasurable technical and economic benefits in power systems. When the superconducting energy storage system is applied to a power system, problems which need to be solved are brought, wherein quench of the superconducting magnet is one of key problems influencing safe and stable operation of the superconducting energy storage system.
Superconductors can exhibit superconducting characteristics only when specific conditions are satisfied. Once the conditions are broken, the magnet will quench. Because the superconducting energy storage device operating in the power system encounters various dynamic processes such as system short-circuit fault, and is subjected to the impact of large short-circuit current and unbalanced current and the effects of electromagnetic, mechanical stress and heat generated thereby, the superconducting magnet may be quenched. The superconducting magnet quench is accompanied by magnet overcurrent and heating, the magnet can be damaged by serious local temperature rise, if measures are not taken in time, a large amount of energy is dissipated in the form of heat energy through the coil, the magnet can be burnt, and the safe, stable and economic operation of a superconducting power system is further influenced.
As a core component of the superconducting energy storage system, the superconducting energy storage magnet can be in the structural form of a ring-shaped superconducting energy storage magnet, a parallel multi-solenoid-shaped superconducting energy storage magnet and a simple single solenoid-shaped superconducting energy storage magnet. The superconducting annular magnet is formed by arranging a plurality of unit coils along the circumferential direction, wherein each unit coil is used as a coil module of the magnet and is formed by connecting a plurality of single coils in series. The ring magnet involves unit coils, single coils, the number of coils being very large, up to hundreds, and quench detection being also much more complex than a single coil. How to timely and effectively detect the quench of the superconducting magnet and protect the quench becomes an important aspect of superconducting application, and has important practical significance.
Disclosure of Invention
When the superconducting magnet normally runs in a superconducting state, the superconducting magnet basically has no resistance, does not generate heat, and does not change voltage and temperature; when the system is in failure, the superconducting condition is damaged, the superconducting magnet enters a non-superconducting state, and the superconducting magnet generates heat, and the voltage and the temperature rise rapidly. Based on the above, in order to solve the problem of quench detection of the superconducting magnet, the invention provides a superconducting magnet quench detection method and device, which are used for detecting the power quench state of a unit coil and the voltage quench state and the temperature quench state of a single coil.
In order to achieve the purpose of the invention, the invention adopts the following technical scheme:
the invention provides a superconducting magnet quench detection method, which comprises the following steps:
detecting the voltage and current of each unit coil in real time;
calculating the power difference of two adjacent unit coils according to the voltage and the current of each unit coil, and solving the absolute value of the power difference between the unit coil and the two adjacent unit coils;
and if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, judging that the unit coil is in a power quench state.
The superconducting magnet is formed by annularly arranging N unit coils, and each unit coil is formed by M single coils which are connected in series and provided with a temperature probe and a lead.
The calculating the power difference of the two adjacent unit coils according to the voltage and the current of each unit coil and the solving of the absolute value of the power difference between the unit coil and the two adjacent unit coils comprises:
P1=(u1-u2)i1
P2=(u2-u3)i2
Pn=(un-un+1)in
PN=(uN-u1)iN
wherein u isnIs the voltage of the nth unit coil, and N is 1,2nIs the current of the nth unit coil, and i1=i2=...=in=...=iN
Calculating the absolute value | P of the power difference between the unit coil and two adjacent unit coils1|、|P2|、...、|Pn|、...、|PN|。
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, the step of judging that the unit coil is in the power quench state comprises the following steps:
setting the power quench threshold to PquenchThe absolute value P of the power difference between the unit coil and two adjacent unit coils1|、|P2|、...、|Pn|、...、|PNL is respectively associated with PquenchComparing, if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than PquenchIt indicates that the unit coil is in a power quench state.
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, indicating that the unit coil is in the power quench state includes:
setting the power delay constant value to NPWhen the absolute value of the power difference between a certain unit coil and two adjacent coils exceeds PquenchSustained NPAnd when the sampling point is detected, the unit coil is in a power quench state.
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, the step of judging that the unit coil is in the power quench state comprises the following steps:
and respectively detecting the voltage quench state and/or the temperature quench state of the single coil.
The detecting of the voltage quench state of the single coil comprises the following steps:
let the collection time interval of voltage and current be Deltat1Detecting the current and the voltage of each single coil in real time, taking each H sampling points as a group, solving the average value of the current of each group, and calculating the induction voltage u of a certain single coil according to the inductance value L of the single coilLThe method comprises the following steps:
Figure BDA0001118932500000031
wherein ilThe current of the l sampling point;
calculating the average value u of two adjacent groups of voltages at the same time, including:
Figure BDA0001118932500000032
wherein u islIs the voltage at the ith sample point;
according to u and uLCalculating the resistance voltage u of the single coilRThe method comprises the following steps:
uR=u-uL
introducing a voltage correction coefficient alpha, comprising:
u′R=u-αuL
wherein u isR' to the resistance voltage of the cell coil after introducing the voltage correction coefficient alpha,
Figure BDA0001118932500000033
u ' is the average voltage value u ' when the single coil is not in the voltage quenching state 'LThe induction voltage is the induction voltage when the single coil is not in the voltage quenching state;
setting the voltage quench threshold to uquenchWill uR' and uquenchComparison, if uR' greater than uquenchAnd indicating that the single coil is in a voltage quenching state.
Detecting a temperature quench condition of the cell coil includes:
the temperature probes arranged on the single coils detect the temperature of the single coils in real time, and the temperature acquisition time interval for acquiring the temperature of a certain single coil by the temperature probes is delta t2Calculating the temperature change rate v of a single coilTThe method comprises the following steps:
Figure BDA0001118932500000041
wherein, TkTemperature, T, of the monoblock coil acquired for the kth time of the temperature probek-1The temperature of the single coil collected by the temperature probe at the k-1 st time;
let the temperature quench threshold be vquenchThe rate of change v of the temperature of a single body coilTAnd vquenchBy comparison, if vTGreater than vquenchAnd indicating that the single coil is in a temperature quenching state.
The detecting of the temperature quench state of the single coil comprises:
setting the temperature rise delay constant value to NTV is to beTAnd vquenchMaking a comparison when vTOver vquenchSustained NTAfter sampling points, the single coil is in a temperature quenching state.
The invention also provides a superconducting magnet quench detection device, comprising:
means for detecting voltage and current of each unit coil in real time;
means for calculating a power difference between two adjacent element coils according to the voltage and current of each element coil, and solving an absolute value of the power difference between the element coil and the two adjacent element coils;
means for setting a power quench threshold; and
and the device is used for judging that the absolute values of the power differences between the unit coil and the two adjacent coils are larger than the power quench threshold value, and indicating that the unit coil is in a power quench state.
The superconducting magnet is formed by annularly arranging N unit coils, and each unit coil is formed by M single coils which are connected in series and provided with a temperature probe and a lead.
The device for calculating the power difference between two adjacent unit coils according to the voltage and the current of each unit coil and solving the power difference absolute value between the unit coil and the two adjacent unit coils comprises the following steps:
means for calculating the power difference between two adjacent element coils according to the following formula:
P1=(u1-u2)i1
P2=(u2-u3)i2
Pn=(un-un+1)in
PN=(uN-u1)iN
wherein u isnIs the voltage of the nth unit coil, and N is 1,2nIs the current of the nth unit coil, and i1=i2=...=in=...=iN(ii) a And
and the device is used for solving the power difference absolute value between the unit coil and two adjacent unit coils.
The quench detection apparatus further includes:
for setting power delay timing value NPThe apparatus of (1); and
used for judging whether the absolute value of the power difference between a certain unit coil and two adjacent coils exceeds PquenchSustained NPAnd when the sampling point is detected, the unit coil is in a power quench state.
The quench detection apparatus further includes:
and the device is used for detecting the voltage quench state and the temperature quench state of the single coil.
The device for detecting the voltage quench state and the temperature quench state of the single coil comprises:
and a device for detecting the voltage quench state of the single coil.
The device for detecting the voltage quench state of the single coil comprises:
means for setting acquisition time intervals for the voltage and current;
means for detecting in real time the voltage and current of each cell coil;
means for setting a voltage quench threshold;
the device is used for introducing a voltage correction coefficient to calculate the resistance voltage of the single coil after the voltage correction coefficient is introduced; and
and the device is used for judging that the resistance voltage of the single coil is greater than the voltage quench threshold value after the voltage correction coefficient is introduced, and indicating that the single coil is in a voltage quench state.
The device for introducing the voltage correction coefficient to calculate the resistance voltage of the single coil after the voltage correction coefficient is introduced comprises the following steps:
and a device for taking each H sampling points as a group, solving the average value of the current of each group, and calculating the induction voltage of a single coil according to the inductance value L of the single coil by the following formula:
Figure BDA0001118932500000051
wherein, Δ t1For the acquisition time interval of voltage and current, ilIs the current at the l-th sampling point, uLThe induced voltage of a certain single coil;
means for calculating an average of two sets of voltages adjacent at the same time by:
Figure BDA0001118932500000061
wherein u islIs the voltage of the l sampling point, u is the average value of two adjacent groups of voltages at the same time;
for according to u and uLMeans for calculating the resistance voltage of the cell coil by:
uR=u-uL
wherein u isRIs the resistance voltage of the cell coil.
The device for introducing the voltage correction coefficient calculates the resistance voltage of the single coil after the voltage correction coefficient is introduced according to the following formula:
u′R=u-αuL
wherein, alpha is a voltage correction coefficient,
Figure BDA0001118932500000063
uR'is the resistance voltage of the cell coil after the voltage correction coefficient is introduced, u' is the average voltage value, u 'when the cell coil is not in the voltage quenching state'LThe induced voltage is the induced voltage when the single coil is not in the voltage quenching state.
The device for detecting the voltage quench state and the temperature quench state of the single coil comprises:
and a device for detecting the temperature quench state of the single coil.
The apparatus for detecting a temperature quench state of the cell coil includes:
the temperature probe is arranged on the single coil and used for detecting the temperature of the single coil in real time;
a device for setting a temperature acquisition time interval for acquiring the temperature of a certain single coil by the temperature probe;
means for calculating a rate of temperature change of a certain cell coil by the following formula;
Figure BDA0001118932500000062
wherein v isTIs the rate of change of temperature, T, of a certain monolithic coilkTemperature, T, of the monoblock coil acquired for the kth time of the temperature probek-1Temperature of the single coil, delta t, acquired for the kth-1 th time of the temperature probe2Acquiring the temperature acquisition time interval of a certain single coil for the temperature probe;
for setting the temperature quench threshold vquenchThe apparatus of (1); and
for judging vTGreater than vquenchAnd then the single coil is in a temperature quenching state.
The apparatus for detecting a temperature quench state of the cell coil further includes:
for setting a constant value N of temperature rise delayTThe apparatus of (1);
for judging vTOver vquenchSustained NTAnd after sampling points, the device indicates that the single coil is in a temperature quenching state.
Compared with the closest prior art, the technical scheme provided by the invention has the following beneficial effects:
1) the method and the device carry out power quench state detection on the unit coils in the superconducting magnet, and determine the power quench state of the corresponding unit coils through comparison, so that the position of the unit coils in the power quench state can be accurately positioned;
2) the invention detects the voltage quench state of the single coil, and determines the voltage quench state of the corresponding single coil through step-by-step comparison, thereby accurately positioning the position of the single coil in the voltage quench state;
3) the invention detects the temperature quench state of the single coil, and determines the temperature quench state of the corresponding single coil through step-by-step comparison, thereby accurately positioning the position of the single coil in the temperature quench state;
4) the invention integrates the detection of the electric quantity and the non-electric quantity, and overcomes the defect of a single quench detection method. And meanwhile, a voltage correction coefficient is introduced, so that the reliability of voltage quench detection is greatly improved.
Drawings
Fig. 1 is a schematic view of a superconducting magnet according to an embodiment of the present invention;
fig. 2 is a flowchart of a superconducting magnet quench detection method in an embodiment of the invention.
Detailed Description
The present invention will be described in further detail with reference to the accompanying drawings.
The invention provides a superconducting magnet quench detection method, as shown in fig. 1, the superconducting magnet is formed by annularly arranging 16 unit coils, each unit coil is formed by connecting 2 single coils in series, and each single coil is provided with a temperature probe and a lead; as shown in fig. 2, the method includes:
the invention provides a superconducting magnet quench detection method, which comprises the following steps:
detecting the voltage and current of each unit coil in real time;
calculating the power difference of two adjacent unit coils according to the voltage and the current of each unit coil, and solving the absolute value of the power difference between the unit coil and the two adjacent unit coils;
and if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, judging that the unit coil is in a power quench state.
The calculating the power difference of the two adjacent unit coils according to the voltage and the current of each unit coil and the solving of the absolute value of the power difference between the unit coil and the two adjacent unit coils comprises:
P1=(u1-u2)i1
P2=(u2-u3)i2
Pn=(un-un+1)in
P16=(u16-u1)i16
wherein u isnIs the voltage of the nth unit coil, and n is 1,2nIs the current of the nth unit coil, and i1=i2=...=in=...=i16
Calculating the absolute value | P of the power difference between two adjacent unit coils1|、|P2|、...、|Pn|、...、|P16|;
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, indicating that the unit coil is in the power quench state includes:
setting the power quench threshold to PquenchThe absolute value | P of the power difference between the unit coil and the adjacent two unit coils1|、|P2|、...、|Pn|、...、|P16L is respectively associated with PquenchComparing, if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than PquenchIt indicates that the unit coil is in a power quench state.
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, the step of judging that the unit coil is in the power quench state comprises the following steps:
setting power delay timing NPWhen the absolute value of the power difference between a certain unit coil and two adjacent coils exceeds PquenchWhen the sampling time lasts for 3 sampling points, the sampling time is shownThe unit coil is in a power quench state. By setting the power delay timing NPCompared with the former method, the method reduces the misjudgment of the power quench state of the unit coil and improves the detection accuracy.
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, the step of judging that the unit coil is in the power quench state comprises the following steps:
and respectively detecting the voltage quench state and/or the temperature quench state of the single coil.
The detecting of the voltage quench state of the single coil comprises the following steps:
let the collection time interval of voltage and current be Deltat1Detecting the current and voltage of each single coil in real time, taking each 5 sampling points as one group, and calculating the average value I of the current of two adjacent groups1And I2And calculating the induced voltage u of a single coil according to the inductance L of the single coilLThe method comprises the following steps:
Figure BDA0001118932500000091
wherein ilThe current of the l sampling point;
calculating the average value u of two adjacent groups of voltages at the same time, including:
Figure BDA0001118932500000092
wherein u islIs the voltage at the ith sample point;
according to u and uLCalculating the resistance voltage u of the single coilRThe method comprises the following steps:
uR=u-uL
introducing a voltage correction coefficient alpha, comprising:
u′R=u-αuL
wherein u isR' to the resistance voltage of the cell coil after introducing the voltage correction coefficient alpha,
Figure BDA0001118932500000093
u ' is the average voltage value u ' when the single coil is not in the voltage quenching state 'LThe induction voltage is the induction voltage when the single coil is not in the voltage quenching state;
setting the voltage quench threshold to uquenchWill uR' and uquenchComparison, if uR' greater than uquenchAnd indicating that the single coil is in a voltage quenching state.
Detecting a temperature quench condition of the cell coil includes:
the temperature probes arranged on the single coils detect the temperature of the single coils in real time, and the temperature acquisition time interval for acquiring the temperature of a certain single coil by the temperature probes is delta t2Calculating the temperature change rate v of a single coilTThe method comprises the following steps:
Figure BDA0001118932500000094
wherein, TkTemperature, T, of the monoblock coil acquired for the kth time of the temperature probek-1The temperature of the single coil collected by the temperature probe at the k-1 st time;
let the temperature quench threshold be vquenchThe rate of change v of the temperature of a single body coilTAnd vquenchBy comparison, if vTGreater than vquenchAnd indicating that the single coil is in a temperature quenching state.
The detecting of the temperature quench state of the single coil comprises:
setting the temperature rise delay constant value to NTWhen v is equal to 3, v isTAnd vquenchMaking a comparison when vTOver vquenchAfter 3 sampling points are continuously carried out, the single coil is in a temperature quenching state. By setting the temperature rise delay constant value to be NTCompared with the former method, the method reduces misjudgment of the temperature quench state of the single coil and improves the accuracy of detection.
The invention also provides a superconducting magnet quench detection device, comprising:
means for detecting voltage and current of each unit coil in real time;
means for calculating a power difference between two adjacent element coils according to the voltage and current of each element coil, and solving an absolute value of the power difference between the element coil and the two adjacent element coils;
means for setting a power quench threshold; and
and the device is used for judging that the absolute values of the power differences between the unit coil and the two adjacent coils are larger than the power quench threshold value, and indicating that the unit coil is in a power quench state.
The device for calculating the power difference between two adjacent unit coils according to the voltage and the current of each unit coil and solving the power difference absolute value between the unit coil and the two adjacent unit coils comprises the following steps:
means for calculating the power difference between two adjacent element coils according to the following formula:
P1=(u1-u2)i1
P2=(u2-u3)i2
Pn=(un-un+1)in
P16=(u16-u1)i16
wherein u isnIs the voltage of the nth unit coil, and n is 1,2nIs the current of the nth unit coil, and i1=i2=...=in=...=i16(ii) a And
for calculating absolute value | P of power difference between unit coil and two adjacent unit coils1|、|P2|、...、|Pn|、...、|P16L of the device.
The quench detection apparatus further includes:
for setting power delay timing value NPA device of 3; and
used for judging whether the absolute value of the power difference between a certain unit coil and two adjacent coils exceeds PquenchAnd when 3 sampling points are continuously carried out, the unit coil is in a power quench state.
The quench detection apparatus further includes:
and the device is used for detecting the voltage quench state and the temperature quench state of the single coil.
The device for detecting the voltage quench state and the temperature quench state of the single coil comprises:
and a device for detecting the voltage quench state of the single coil.
The device for detecting the voltage quench state of the single coil comprises:
means for setting acquisition time intervals for the voltage and current;
means for detecting in real time the voltage and current of each cell coil;
means for setting a voltage quench threshold;
the device is used for introducing a voltage correction coefficient to calculate the resistance voltage of the single coil after the voltage correction coefficient is introduced; and
and the device is used for judging that the resistance voltage of the single coil is greater than the voltage quench threshold value after the voltage correction coefficient is introduced, and indicating that the single coil is in a voltage quench state.
The device for introducing the voltage correction coefficient to calculate the resistance voltage of the single coil after the voltage correction coefficient is introduced comprises the following steps:
for taking each 5 sampling points as one group, calculating the average value I of the current of two adjacent groups1And I2And means for calculating an induced voltage of a single coil from the inductance value L of the single coil by the following formula:
Figure BDA0001118932500000111
wherein ilThe current of the l sampling point;
means for calculating an average of two sets of voltages adjacent at the same time by:
Figure BDA0001118932500000112
wherein u islIs the voltage of the l sampling point, u is the average value of two adjacent groups of voltages at the same time;
for according to u and uLMeans for calculating the resistance voltage of the cell coil by:
uR=u-uL
wherein u isRIs the resistance voltage of the cell coil.
The device for introducing the voltage correction coefficient calculates the resistance voltage of the single coil after the voltage correction coefficient is introduced according to the following formula:
u′R=u-αuL
wherein, alpha is a voltage correction coefficient,
Figure BDA0001118932500000121
uR'is the resistance voltage of the cell coil after the voltage correction coefficient is introduced, u' is the average voltage value, u 'when the cell coil is not in the voltage quenching state'LThe induced voltage is the induced voltage when the single coil is not in the voltage quenching state.
The device for detecting the voltage quench state and the temperature quench state of the single coil comprises:
and a device for detecting the temperature quench state of the single coil.
The apparatus for detecting a temperature quench state of the cell coil includes:
the temperature probe is arranged on the single coil and used for detecting the temperature of the single coil in real time;
a device for setting a temperature acquisition time interval for acquiring the temperature of a certain single coil by the temperature probe;
means for calculating a rate of temperature change of a certain cell coil by the following formula;
Figure BDA0001118932500000122
wherein v isTIs the rate of change of temperature, T, of a certain monolithic coilkTemperature, T, of the monoblock coil acquired for the kth time of the temperature probek-1Temperature of the single coil, delta t, acquired for the kth-1 th time of the temperature probe2Acquiring the temperature acquisition time interval of a certain single coil for the temperature probe;
for setting the temperature quench threshold vquenchThe apparatus of (1); and
for judging vTGreater than vquenchAnd then the single coil is in a temperature quenching state.
The apparatus for detecting a temperature quench state of the cell coil further includes:
for setting a constant value N of temperature rise delayTA device of 3;
for judging vTOver vquenchAnd after 3 sampling points are continuously carried out, the device indicates that the single coil is in a temperature quenching state.
Finally, it should be noted that: the above embodiments are only intended to illustrate the technical solution of the present invention and not to limit the same, and a person of ordinary skill in the art can make modifications or equivalents to the specific embodiments of the present invention with reference to the above embodiments, and such modifications or equivalents without departing from the spirit and scope of the present invention are within the scope of the claims of the present invention as set forth in the claims.

Claims (11)

1. A method of superconducting magnet quench detection, the method comprising:
detecting the voltage and current of each unit coil in real time;
calculating the power difference of two adjacent unit coils according to the voltage and the current of each unit coil, and solving the absolute value of the power difference between the unit coil and the two adjacent unit coils;
if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, judging that the unit coil is in a power quench state;
the superconducting magnet is formed by annularly arranging N unit coils, and each unit coil consists of M single coils which are connected in series and provided with a temperature probe and a lead;
the calculating the power difference of the two adjacent unit coils according to the voltage and the current of each unit coil and the solving of the absolute value of the power difference between the unit coil and the two adjacent unit coils comprises:
Figure FDA0002621405770000011
wherein u isnIs the voltage of the nth unit coil, and N is 1,2nIs the current of the nth unit coil, and i1=i2=...=in=...=iN
Calculating the absolute value | P of the power difference between the unit coil and two adjacent unit coils1|、|P2|、...、|Pn|、...、|PN|;
If the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold, the step of judging that the unit coil is in the power quench state comprises the following steps:
respectively detecting the voltage quench state and/or the temperature quench state of the single coil;
the detecting of the voltage quench state of the single coil comprises the following steps:
let the collection time interval of voltage and current be Deltat1Detecting the current and the voltage of each single coil in real time, taking each H sampling points as a group, solving the average value of the current of each group, and calculating the induction voltage u of a certain single coil according to the inductance value L of the single coilLThe method comprises the following steps:
Figure FDA0002621405770000021
wherein ilThe current of the l sampling point;
calculating the average value u of two adjacent groups of voltages at the same time, including:
Figure FDA0002621405770000022
wherein u islIs the voltage at the ith sample point;
according to u and uLCalculating the resistance voltage u of the single coilRThe method comprises the following steps:
uR=u-uL
introducing a voltage correction coefficient alpha, comprising:
uR′=u-αuL
wherein u isR' to the resistance voltage of the cell coil after introducing the voltage correction coefficient alpha,
Figure FDA0002621405770000023
u ' is the average voltage value u ' when the single coil is not in the voltage quenching state 'LThe induction voltage is the induction voltage when the single coil is not in the voltage quenching state;
setting the voltage quench threshold to uquenchWill uR' and uquenchComparison, if uR' greater than uquenchAnd indicating that the single coil is in a voltage quenching state.
2. The superconducting magnet quench detection method according to claim 1, wherein the determining that the unit coil is in the power quench state if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold value comprises:
setting the power quench threshold to PquenchThe absolute value | P of the power difference between the unit coil and the adjacent two unit coils1|、|P2|、...、|Pn|、...、|PNL is respectively associated with PquenchComparing, if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than PquenchIt indicates that the unit coil is in a power quench state.
3. The superconducting magnet quench detection method according to claim 2, wherein the determining that the unit coil is in the power quench state if the absolute value of the power difference between the unit coil and the two adjacent coils is greater than the power quench threshold value comprises:
setting the power delay constant value to NPWhen the absolute value of the power difference between a certain unit coil and two adjacent coils exceeds PquenchSustained NPAnd when the sampling point is detected, the unit coil is in a power quench state.
4. The superconducting magnet quench detection method of claim 1, wherein the detecting the temperature quench state of the monoblock coil comprises:
the temperature probes arranged on the single coils detect the temperature of the single coils in real time, and the temperature acquisition time interval for acquiring the temperature of a certain single coil by the temperature probes is delta t2Calculating the temperature change rate v of a single coilTThe method comprises the following steps:
Figure FDA0002621405770000031
wherein, TkTemperature, T, of the monoblock coil acquired for the kth time of the temperature probek-1The temperature of the single coil collected by the temperature probe at the k-1 st time;
let the temperature quench threshold be vquenchThe rate of change v of the temperature of a single body coilTAnd vquenchBy comparison, if vTGreater than vquenchAnd indicating that the single coil is in a temperature quenching state.
5. The superconducting magnet quench detection method of claim 1, wherein the detecting the temperature quench state of the monoblock coil comprises:
setting the temperature rise delay constant value to NTV is to beTAnd vquenchMaking a comparison when vTOver vquenchSustained NTAfter sampling points, the single coil is in a temperature quenching state.
6. A superconducting magnet quench detection apparatus, the quench detection apparatus comprising:
means for detecting voltage and current of each unit coil in real time;
means for calculating a power difference between two adjacent element coils according to the voltage and current of each element coil, and solving an absolute value of the power difference between the element coil and the two adjacent element coils;
means for setting a power quench threshold; and
the device is used for judging whether the absolute values of the power difference between the unit coil and the two adjacent coils are larger than a power quench threshold value, and indicating that the unit coil is in a power quench state;
the superconducting magnet is formed by annularly arranging N unit coils, and each unit coil consists of M single coils which are connected in series and provided with a temperature probe and a lead;
the device for calculating the power difference between two adjacent unit coils according to the voltage and the current of each unit coil and solving the power difference absolute value between the unit coil and the two adjacent unit coils comprises the following steps:
means for calculating the power difference between two adjacent element coils according to the following formula:
Figure FDA0002621405770000032
Figure FDA0002621405770000041
wherein u isnIs the voltage of the nth unit coil, and N is 1,2nIs the current of the nth unit coil, and i1=i2=...=in=...=iN(ii) a And
the device is used for solving the power difference absolute value between the unit coil and two adjacent unit coils;
the quench detection apparatus further includes:
means for detecting a voltage quench condition and a temperature quench condition of the cell coil;
the device for detecting the voltage quench state of the single coil comprises:
means for setting acquisition time intervals for the voltage and current;
means for detecting in real time the voltage and current of each cell coil;
means for setting a voltage quench threshold;
the device is used for introducing a voltage correction coefficient to calculate the resistance voltage of the single coil after the voltage correction coefficient is introduced; and
and the device is used for judging that the resistance voltage of the single coil is greater than the voltage quench threshold value after the voltage correction coefficient is introduced, and indicating that the single coil is in a voltage quench state.
7. The superconducting magnet quench detection apparatus of claim 6, further comprising:
for setting power delay timing value NPThe apparatus of (1); and
used for judging whether the absolute value of the power difference between a certain unit coil and two adjacent coils exceeds PquenchSustained NPAnd when the sampling point is detected, the unit coil is in a power quench state.
8. The superconducting magnet quench detection apparatus according to claim 6, wherein the means for introducing the voltage correction factor to calculate the resistance voltage of the monolithic coil after introducing the voltage correction factor comprises:
and a device for taking each H sampling points as a group, solving the average value of the current of each group, and calculating the induction voltage of a single coil according to the inductance value L of the single coil by the following formula:
Figure FDA0002621405770000042
wherein, Δ t1For the acquisition time interval of voltage and current, ilIs the current at the l-th sampling point, uLThe induced voltage of a certain single coil;
means for calculating an average of two sets of voltages adjacent at the same time by:
Figure FDA0002621405770000051
wherein u islIs the voltage of the l sampling point, u is the average value of two adjacent groups of voltages at the same time;
for according to u and uLMeans for calculating the resistance voltage of the cell coil by:
uR=u-uL
wherein u isRIs the resistance voltage of the cell coil.
9. The superconducting magnet quench detection apparatus of claim 8, wherein the means for introducing the voltage correction factor calculates the resistance voltage of the monolithic coil after introducing the voltage correction factor by:
uR′=u-αuL
wherein, alpha is a voltage correction coefficient,
Figure FDA0002621405770000052
uR'is the resistance voltage of the cell coil after the voltage correction coefficient is introduced, u' is the average voltage value, u 'when the cell coil is not in the voltage quenching state'LThe induced voltage is the induced voltage when the single coil is not in the voltage quenching state.
10. The superconducting magnet quench detection apparatus of claim 6 wherein the means for detecting a temperature quench condition of the monoblock coil comprises:
the temperature probe is arranged on the single coil and used for detecting the temperature of the single coil in real time;
a device for setting a temperature acquisition time interval for acquiring the temperature of a certain single coil by the temperature probe;
means for calculating a rate of temperature change of a certain cell coil by the following formula;
Figure FDA0002621405770000053
wherein v isTIs the rate of change of temperature, T, of a certain monolithic coilkTemperature, T, of the monoblock coil acquired for the kth time of the temperature probek-1Temperature of the single coil, delta t, acquired for the kth-1 th time of the temperature probe2Acquiring the temperature acquisition time interval of a certain single coil for the temperature probe;
for setting the temperature quench threshold vquenchThe apparatus of (1); and
for judging vTGreater than vquenchAnd then the single coil is in a temperature quenching state.
11. The superconducting magnet quench detection apparatus of claim 10, wherein the means for detecting a temperature quench state of the monolithic coil further comprises:
for setting a constant value N of temperature rise delayTThe apparatus of (1);
for judging vTOver vquenchSustained NTAnd after sampling points, the device indicates that the single coil is in a temperature quenching state.
CN201610843208.9A 2016-09-22 2016-09-22 Superconducting magnet quench detection method and device Active CN106501740B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610843208.9A CN106501740B (en) 2016-09-22 2016-09-22 Superconducting magnet quench detection method and device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610843208.9A CN106501740B (en) 2016-09-22 2016-09-22 Superconducting magnet quench detection method and device

Publications (2)

Publication Number Publication Date
CN106501740A CN106501740A (en) 2017-03-15
CN106501740B true CN106501740B (en) 2021-02-23

Family

ID=58290437

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610843208.9A Active CN106501740B (en) 2016-09-22 2016-09-22 Superconducting magnet quench detection method and device

Country Status (1)

Country Link
CN (1) CN106501740B (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109342504B (en) * 2018-11-20 2022-09-20 中国电力科学研究院有限公司 Device and method for measuring quench recovery characteristic of superconducting tape
CN111812562B (en) * 2020-06-01 2024-01-30 国网辽宁省电力有限公司电力科学研究院 Quench detection method and quench detection device for high-temperature superconductive ring magnet
CN111707978B (en) * 2020-07-09 2021-09-10 华中科技大学 Quench detection method, device and equipment for superconducting magnet and storage medium
CN113954678B (en) * 2021-10-28 2024-03-12 上海海事大学 Charging system and method for high-temperature superconducting module battery for hybrid energy storage of automobile battery

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0205924A3 (en) * 1985-05-20 1988-04-06 Kabushiki Kaisha Toshiba Monitoring system for detecting quench of superconductive coils
CN101126787B (en) * 2007-09-28 2010-06-09 中国科学院电工研究所 Superconducting coil quench detection method
CN101446610B (en) * 2008-11-25 2011-08-17 中国电力科学研究院 Quench-detection circuit of high-temperature superconducting magnet
CN101975900A (en) * 2010-10-08 2011-02-16 天津理工大学 Superconducting magnet quenching detection system based on active power
CN201897633U (en) * 2010-10-08 2011-07-13 天津理工大学 Superconducting magnet quench detection device based on active power
CN102346239B (en) * 2011-04-18 2014-09-10 中国科学院等离子体物理研究所 Quenching detection system used in superconducting magnet under pulsed field and method thereof
CN104181821B (en) * 2014-08-08 2017-01-25 东南大学 Comprehensive real-time monitoring and early warning method applicable to superconducting magnets or superconducting equipment

Also Published As

Publication number Publication date
CN106501740A (en) 2017-03-15

Similar Documents

Publication Publication Date Title
CN106501740B (en) Superconducting magnet quench detection method and device
CN107102278B (en) Quench detection device and method for superconducting magnet under alternating current working condition
EP2680017A1 (en) A method of early detection of feeder lines with a high-ohm ground fault in compensated power networks
CN102607643A (en) Overheat fault diagnosis and early warning system and method for electrical equipment of traction substation of electrified railway
CN102346239B (en) Quenching detection system used in superconducting magnet under pulsed field and method thereof
CN107870286A (en) A kind of DC Line Fault arc method for measuring and device
CN102495328B (en) Differential power reactor fault on-line monitoring instrument
CN106291226A (en) Residual current transformer failure detector circuit and electrical fire-detector
CN101551442B (en) A generator rotor insulation on-line monitoring grounding locating method and device
Baldini et al. Quench performance of the first pre-series AUP cryo-assembly
CN110579661B (en) Method and system for detecting quench of superconducting cable
CN107731328A (en) A kind of Gray code double precision control rod location detection methods
RU2437109C2 (en) Control method of electrical resistance of insulation and protective disconnection of electrical equipment
CN107728002B (en) Distribution network fault online positioning method considering distributed power access
CN206649097U (en) More battery detection circuit for access and electronic equipment
Sheng et al. Recovery time of high temperature superconducting tapes exposed in liquid nitrogen
CN113702875B (en) Gas switch self-discharge positioning method of fast pulse linear transformer driving source
CN109239437A (en) A kind of current sensor of the redundancy feature containing self-test
CN104391145A (en) Online low voltage detection device for electric leakage and electric energy steal and implement method thereof
RU2609277C1 (en) Method of monitoring insulation resistance of extensive dc networks
FI129549B (en) Electric vehicle charging monitoring device and method
Chu et al. Performance of the quench detection system for the KSTAR CS magnet system
CN109541345B (en) Half-wave detection method and half-wave detection system
Zhu et al. Research and application of on-line monitoring device for dry-type air-core reactor
CN106154121A (en) A kind of cable system insulating fault diagnosis method

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant