交流相对磁导率检测标准

交流相对磁导率检测标准相关信息

ASTM A772/A772M-00(2016) 使用正弦电流的材料的交流磁导率的标准测试方法
简介：
信息：ICS：29.030 CCS： 发布：2016-04-01 实施：

ASTM A772/A772M-00(2011) 使用正弦电流的材料的交流磁导率的标准测试方法
简介：
信息：ICS：29.030 CCS： 发布：2011-05-01 实施：

ASTM A772/A772M-00(2011)e1 使用正弦电流的材料的交流磁导率的标准测试方法
简介：
信息：ICS：29.030 CCS： 发布：2011-05-01 实施：

ASTM A772/A772M-00(2005) 使用正弦电流的材料的交流磁导率的标准测试方法
简介：
信息：ICS：29.030 CCS： 发布：2005-11-01 实施：

ASTM A772/A772M-00 使用正弦电流的材料的交流磁导率的标准测试方法
简介：
信息：ICS：29.030 CCS： 发布：2000-10-10 实施：

ASTM A772/A772M-2000(2011)e1 正弦电流用材料的交流磁导率的标准试验方法
简介：The permeability determined by this method is the impedance permeability. Impedance permeability is the ratio of the peak value of flux density (Bmax) to the assumed peak magnetic field strength (Hz) without regard to phase. As compared to testing under sinusoidal flux (sinusoidal B) conditions, the permeabilities determined by this method are numerically lower since, for a given test signal frequency, the rate of flux change (dB/dt) is higher. This test method is suitable for impedance permeability measurements at very low magnetic inductions at power frequencies (50 to 60 Hz) to moderate inductions below the point of maximum permeability of the material (the knee of the magnetization curve) or until there is visible distortion of the current waveform. The lower limit is a function of sample area, secondary turns, and the sensitivity of the flux-reading voltmeter used. At higher inductions, measurements of flux-generated voltages that are appreciably distorted mean that the flux has appreciable harmonic frequency components. The upper limit is given by the availability of pure sinusoidal current, which is a function of the power source. In addition, a large ratio (x2265;10) of the total series resistance of the primary circuit to the primary coil impedance is required. With proper test apparatus, this test method is suitable for use at frequencies up to 1 MHz. This test method is suitable for design, specification acceptance, service evaluation, quality control, and research use.1.1 This test method provides a means for determination of the impedance permeability (x03BC;z) of ferromagnetic materials under the condition of sinusoidal current (sinusoidal H) excitation. Test specimens in the form of laminated toroidal cores, tape-wound toroidal cores, and link-type laminated cores having uniform cross sections and closed flux paths (no air gaps) are used. The method is intended as a means for determining the magnetic performance of ferromagnetic strip having a thickness less than or equal to 0.025 in. [0.635 mm]. 1.2 This test method shall be used in conjunction with those applicable paragraphs in Practice A34/A34M. 1.3 The values and equations stated in customary (cgs-emu and inch-pound) or SI units are to be regarded separately as standard. Within this standard, SI units are shown in brackets except for the sections concerning calculations where there are separate sections for the respective unit systems. The values stated in each system may not be exact equivalents; therefore, each system shall be used independently of the other. Combining values from the two systems may result in nonconformance with this standard. 1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.
信息：ICS：29.030 (Magnetic materials) CCS：H21 发布：2000 实施：

ASTM A772/A772M-2000 使用正弦电流测定材料的交流磁导率的标准试验方法
简介：1.1 This test method provides a means for determination of the impedance permeability (181z) of ferromagnetic materials under the condition of sinusoidal current (sinusoidal H) excitation. Test specimens in the form of laminated toroidal cores, tape-wound toroidal cores, and link-type laminated cores having uniform cross sections and closed flux paths (no air gaps) are used. The method is intended as a means for determining the magnetic performance of ferromagnetic strip having a thickness less than or equal to 0.025 in. [0.635 mm].1.2 This test method shall be used in conjunction with those applicable paragraphs in Practice A34/A34M.1.3 The values and equations stated in customary (cgs-emu and inch-pound) or SI units are to be regarded separately as standard. Within this standard, SI units are shown in brackets except for the sections concerning calculations where there are separate sections for the respective unit systems. The values stated in each system may not be exact equivalents; therefore, each system shall be used independently of the other. Combining values from the two systems may result in nonconformance with this standard.1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.
信息：ICS：29.030 (Magnetic materials) CCS： 发布：2000 实施：

ASTM A772/A772M-2000(2005) 正弦电流用材料的交流磁导率的标准试验方法
简介：The permeability determined by this method is the impedance permeability. Impedance permeability is the ratio of the peak value of flux density (Bmax) to the assumed peak magnetic field strength (Hz) without regard to phase. As compared to testing under sinusoidal flux (sinusoidal B) conditions, the permeabilities determined by this method are numerically lower since, for a given test signal frequency, the rate of flux change (dB/dt) is higher. This test method is suitable for impedance permeability measurements at very low magnetic inductions at power frequencies (50 to 60 Hz) to moderate inductions below the point of maximum permeability of the material (the knee of the magnetization curve) or until there is visible distortion of the current waveform. The lower limit is a function of sample area, secondary turns, and the sensitivity of the flux-reading voltmeter used. At higher inductions, measurements of flux-generated voltages that are appreciably distorted mean that the flux has appreciable harmonic frequency components. The upper limit is given by the availability of pure sinusoidal current, which is a function of the power source. In addition, a large ratio (x2265;10) of the total series resistance of the primary circuit to the primary coil impedance is required. With proper test apparatus, this test method is suitable for use at frequencies up to 1 MHz. This test method is suitable for design, specification acceptance, service evaluation, quality control, and research use.1.1 This test method provides a means for determination of the impedance permeability (181z) of ferromagnetic materials under the condition of sinusoidal current (sinusoidal H) excitation. Test specimens in the form of laminated toroidal cores, tape-wound toroidal cores, and link-type laminated cores having uniform cross sections and closed flux paths (no air gaps) are used. The method is intended as a means for determining the magnetic performance of ferromagnetic strip having a thickness less than or equal to 0.025 in. [0.635 mm].1.2 This test method shall be used in conjunction with those applicable paragraphs in Practice A34/A34M.1.3 The values and equations stated in customary (cgs-emu and inch-pound) or SI units are to be regarded separately as standard. Within this standard, SI units are shown in brackets except for the sections concerning calculations where there are separate sections for the respective unit systems. The values stated in each system may not be exact equivalents; therefore, each system shall be used independently of the other. Combining values from the two systems may result in nonconformance with this standard.1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.
信息：ICS：29.030 (Magnetic materials) CCS：H21 发布：2000 实施：

ASTM A772/A772M-2000(2011) 正弦电流用材料的交流磁导率的标准试验方法
简介：The permeability determined by this method is the impedance permeability. Impedance permeability is the ratio of the peak value of flux density (Bmax) to the assumed peak magnetic field strength (Hz) without regard to phase. As compared to testing under sinusoidal flux (sinusoidal B) conditions, the permeabilities determined by this method are numerically lower since, for a given test signal frequency, the rate of flux change (dB/dt) is higher. This test method is suitable for impedance permeability measurements at very low magnetic inductions at power frequencies (50 to 60 Hz) to moderate inductions below the point of maximum permeability of the material (the knee of the magnetization curve) or until there is visible distortion of the current waveform. The lower limit is a function of sample area, secondary turns, and the sensitivity of the flux-reading voltmeter used. At higher inductions, measurements of flux-generated voltages that are appreciably distorted mean that the flux has appreciable harmonic frequency components. The upper limit is given by the availability of pure sinusoidal current, which is a function of the power source. In addition, a large ratio (x2265;10) of the total series resistance of the primary circuit to the primary coil impedance is required. With proper test apparatus, this test method is suitable for use at frequencies up to 1 MHz. This test method is suitable for design, specification acceptance, service evaluation, quality control, and research use.1.1 This test method provides a means for determination of the impedance permeability (x03BC;z) of ferromagnetic materials under the condition of sinusoidal current (sinusoidal H) excitation. Test specimens in the form of laminated toroidal cores, tape-wound toroidal cores, and link-type laminated cores having uniform cross sections and closed flux paths (no air gaps) are used. The method is intended as a means for determining the magnetic performance of ferromagnetic strip having a thickness less than or equal to 0.025 in. [0.635 mm]. 1.2 This test method shall be used in conjunction with those applicable paragraphs in Practice A34/A34M. 1.3 The values and equations stated in customary (cgs-emu and inch-pound) or SI units are to be regarded separately as standard. Within this standard, SI units are shown in brackets except for the sections concerning calculations where there are separate sections for the respective unit systems. The values stated in each system may not be exact equivalents; therefore, each system shall be used independently of the other. Combining values from the two systems may result in nonconformance with this standard. 1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.
信息：ICS：29.030 CCS：H21 发布：2000 实施：

ASTM A772/A772M-2000(2016) 采用正弦电流的材料交流磁导率标准试验方法
简介： 4.1x00a0;The permeability determined by this method is the impedance permeability. Impedance permeability is the ratio of the peak value of flux density (Bmax) to the assumed peak magnetic field strength (Hz) without regard to phase. As compared to testing under sinusoidal flux (sinusoidal B) conditions, the permeabilities determined by this method are numerically lower since, for a given test signal frequency, the rate of flux change (dB/dt) is higher. 4.2x00a0;This test method is suitable for impedance permeability measurements at very low magnetic inductions at power frequencies (50 to 60 Hz) to moderate inductions below the point of maximum permeability of the material (the knee of the magnetization curve) or until there is visible distortion of the current waveform. The lower limit is a function of sample area, secondary turns, and the sensitivity of the flux-reading voltmeter used. At higher inductions, measurements of flux-generated voltages that are appreciably distorted mean that the flux has appreciable harmonic frequency components. The upper limit is given by the availability of pure sinusoidal current, which is a function of the power source. In addition, a large ratio (x2265;10) of the total series resistance of the primary circuit to the primary coil impedance is required. With proper test apparatus, this test method is suitable for use at frequencies up to 1 MHz. 4.3x00a0;This test method is suitable for design, specification acceptance, service evaluation, quality control, and research use. 1.1x00a0;This test method provides a means for determination of the impedance permeability (x03bc;z) of ferromagnetic materials under the condition of sinusoidal current (sinusoidal H) excitation. Test specimens in the form of laminated toroidal cores, tape-wound toroidal cores, and link-type laminated cores having uniform cross sections and closed flux paths (no air gaps) are used. The method is intended as a means for determining the magnetic performance of ferromagnetic strip having a thickness less than or equal to 0.025 in. [0.635 mm]. 1.2x00a0;This test method shall be used in conjunction with those applicable paragraphs in Practice A34/A34M. 1.3x00a0;The values and equations stated in customary (cgs-emu and inch-pound) or SI units are to be regarded separately as standard. Within this standard, SI units are shown in brackets except for the sections concerning calculations where there are separate sections for the respective unit systems. The values stated in each system may not be exact equivalents; therefore, each system shall be used independently of the other. Combining values from the two systems may result in nonconformance with this standard. 1.4x00a0;This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of ......
信息：ICS：29.030 CCS： 发布：2000 实施：

GOST 12119.6-1998 电工钢.磁性能及电性能测定法;相对磁导率及交流电桥测定磁损率的方法
简介：Настоящий стандарт устанавливает метод определения действительной и мнимой составляющих комплексной относительной магнитной проницаем
信息：ICS：77.040.20 CCS： 发布：1998 实施：1999-07-01

AECMA PREN 2591-513-1997 航空航天系列.光电连接件元件 试验方法.第513部分:交流磁导率
简介：This standard specifies the characteristics of tee union, equal in titanium alloy intended for use in aircraft fluid system pipe lines.
信息：ICS：67.080.20 CCS：V40 发布：1997-04-01 实施：

JJG 493-1987 软磁材料音频磁特性标准样品(交流磁化曲线及幅值磁导率)检定规程
简介：
信息：ICS： CCS：A55 发布：1987 实施：1988-01-09

北检院部分仪器展示