磁性的测量_精品文档.pdf
- 文档编号:3216496
- 上传时间:2022-11-20
- 格式:PDF
- 页数:104
- 大小:1.53MB
磁性的测量_精品文档.pdf
《磁性的测量_精品文档.pdf》由会员分享,可在线阅读,更多相关《磁性的测量_精品文档.pdf(104页珍藏版)》请在冰豆网上搜索。
磁性测量中的几个问题第二部分:
参数磁化率的测量居里温度的测量饱和值的测量磁性测量讲座2007年磁学国家重点实验室磁化率2021TFHMHMH=?
磁化率的定义:
磁化强度M与磁场强度H的依赖关系初始磁化率磁化率质量(比)磁化率摩尔(克分子)磁化率张量磁化率H的大小M的计量单位H、M的空间分布磁化率MH=?
磁化率的量纲与单位:
磁场强度H的单位:
A/m的单位的量纲M的单位m3/molL3N1Am2/mol摩尔磁化率m3/kgL3M1Am2/kg质量磁化率11A/m磁化率磁化率MH=?
磁化率的数值:
闭合磁路开放磁路磁路励磁交流励磁直流励磁质量样品:
几何形状体积测量方法:
磁化率MH=?
磁化率的数值:
不要求精确数值:
略适用:
直流磁化率交流磁化率根据磁化率计算其它参数:
220
(1)3JBBNgJJCk+=必须注意:
H(样品内部的磁场)退磁效应退磁效应、退磁场、退磁因子HextMintextdHHH=+?
Hint样品内部磁场:
ddHNM=?
?
样品的磁化率:
intintMH=dNextMH=int1dddNNN=intint1ddNN=+int11dNdN=退磁效应的理论处理静磁学边值问题设空间充满磁导率为2的介质,在此空间存在一均匀的平行磁场H0,将某一磁导率为1的任意形状物体放置在此空间中,求解该物体内部感生的磁化强度和磁场强度。
退磁效应的理论处理求解依据:
t=+DHJ1、Maxwell方程:
0=H(J0,静磁学)()12-0=?
nBB2、唯一性边界条件:
0()=+BHHM3、磁化方程:
00=MH退磁效应的理论处理求解方法:
0=H分离变量法32210iiiiguhu=Laplace方程:
2222123,iiiixyzhghhhuuu=+=321()1()()44VSdd=+MrnMrrrrr-rr-r磁标势均匀磁化:
0退磁效应的理论处理求解方法:
0=H1、引力势:
Poisson:
旋转椭球体R.I.Joseph2、磁标势级数展开:
intintM?
HD.X.Chen3、电感方法:
A.S.Arrott4、能量方法:
MagnetostaticprinciplesinferromagnetismW.F.Brown,Jr.,1962,North-HollandPublishingCompany,Amsterdam退磁因子旋转椭球体:
精确解(解析解)bac1GGcGabNNN+=真空中:
定义椭率:
ccrab扁椭球(oblatespheroid)长椭球(prolatespheroid)(绕c轴旋转)()2211arccos11crNrrr=()2221ln1111crNrrrr=+r1r=()()()22archln1arsh1rrrr+=sh,ch22xxxxeeeexx+=()()22arshln1,archln1xxxxxx=+=+旋转椭球体的退磁因子0.10873.00.47580.61/31.00.75050.20.17362.00.52720.50.05585.00.43210.70.21871.60.58820.40.23301.50.66140.30.36180.90.86080.10.39440.81.0000.0NcrNcrccrab其它形状的退磁因子H=?
均匀磁化假设:
均匀退磁场假设:
通量退磁因子Nf(thefluxmetric(ballistic)demagnetizingfactor)xyzNf中心截面的平均磁化强度与平均退磁场强度之比Nm整个样品的平均磁化强度与平均退磁场强度之比强度退磁因子Nm(themagnetometricdemagnetizingfactor)圆柱体的退磁因子均匀磁化:
(h方向)h2a2hra定义长径比:
21()()fffrNKkEkk=22414fkr=+222411()
(1)()13mmmNrrKkrEkr=+22111mkr=+122222220011(),;1;,1222
(1)
(1)1sindxdyKkFkkxkxky=2212222200111()1sin,;1;,11222kxEkdxdykyFkkx=20时:
211FiorillofrNr=+r1(细长圆柱体)时22413251,1228fNrrrr+241,138mNrrrr1(短粗圆柱体)时281ln1,1frNrr2411ln,12mrNrr薄片状22211arctanlnln
(1),24mrrNrrbacrr=+()222223222221121211lnln21ln2111122arctan12
(1)2(21)132mrrrNrrrrrrrrrrrrr+=+craaac四方体长方体的退磁因子退化情况下:
如果:
ab()()()2222222222428arctan2482ln28424frrrNrrrrrrr+=+四方体的退磁因子简化公式:
aac四方体craab112SatomNr=+21arcsin1FiorillomNr=+cra四方体的退磁因子0.02360.05860.11090.15090.16390.25870.28620.3178Nf0.35440.39710.44730.50730.58030.67170.79331.000Nf0.14043.00.45250.61/31.00.69420.20.19832.00.49590.50.08835.00.41570.70.23711.60.54820.40.24921.50.61240.30.35710.90.80510.10.38430.81.0000.0NmrNmr正确处理退磁效应退磁效应的影响程度如何确定退磁因子规则形状的退磁因子非规则形状的退磁因子退磁效应对什么量有影响(Hext,M)所有与Hint有关的量!
(Hint,M)MHextHdKittel公式旋转椭球体的一致进动本征频率:
()()000xzSyzSHNNMHNNM=+仅为教学使用10-310-210-110010110210310410510610-310-210-11001011021031.0000.1000.0100.00100102103104105106107108109110111112113114115116117118119120121122123124125126127128129130131132133134135136137138139140141142143144145146147148149150151152153154155156157158159160161162163164165166167168169170171172173174175176177178179180181182183184185186187188189190191192193194195196197198199200201202203204205206207208209210211212213214215216217218219220221222223224225226227228229230231232233234235236237238239240241242243244245246247248249250251252253254255256257258259260261262263264265266267268269270271272273274275276277278279280281282283284285286287288289290291292293294295296297298299300301302303304305306307308309310311312313314315316317318319320321322323324325323VWCXCYCZDADBDCDDDEDFDGDHDIDJDKDLDMDNDODPDQDRDSDTDUDVDWDXDYDZEAEBECEDEEEFEGEHEIEJEKELEMENEOEPEQERESETEUEVEWEXEYEZFAFBFCFDFEFFFGFHFIFJFKFLFMFNFOFPFQFRFSFTFUFVFWFXFYFZGAGBGCGDGEGFGGGHGIGJGKGLGMGNGOGPGQGRGSGTGUGVGWGXGYGZHAHBHCHDHEHFHGHHHIHJHKHLHMHNHOHPHQHRHSHTHUHVHWHXHYHZIAIBICIDIEIFIGIHIIIJIKILIMINIOIPIQIRISITIUIVIWIXIYIZJAJBJCJDJEJFJGJHJIJJJKJLJMJNJOJPJQJRJSJTJUJVJWJXJYJZKAKBKCKDKEKFKGKHKIKJKKKLKMKNKOKPKQKRKSKTKUKVKWKXKYKZLALBLCLDLELFLGLHLILJLKLLLMLNLwcxcyczdadbdcdddedfdgdhdidjdkdldmdndodpdqdrdsdtdudvdwdxdydzeaebecedeeefegeheiejekelemeneoepeqereseteuevewexeyezfafbfcfdfefffgfhfifjfkflfmfnfofpfqfrfsftfufvfwfxfyfzgagbgcgdgegfggghgigjgkglgmgngogpgqgrgsgtgugvgwgxgygzhahbhchdhehfhghhhihjhkhlhmhnhohphqhrhshthuhvhwhxhyhziaibicidieifigihiiijikiliminioipiqirisitiuiviwixiyizjajbjcjdjejfjgjhjijjjkjljmjnjojpjqjrjsjtjujvjwjxjyjzkakbkckdkekfkgkhkikjkkklkmknkokpkqkrksktkukvkwkxkykzlalblcldlelflglhliljlklllmlnNN=0.001N=0.002N=0.003N=0.004N=0.005N=0.006N=0.007N=0.008N=0.009N=0.010N=0.020N=0.030N=0.040N=0.050N=0.060N=0.0701N=0.080AN=0.090aN=0.100N=0.200N=0.293N=0.333N=0.500N=1.000DemagnetizationfactorN1+NN=修正未修正影响程度D1E-41E-30.010.111010010001E-71E-61E-51E-41E-30.010.11123456789100.010.1DemagnetizingfactorsN(Nf,Nm)AspectRatior(c/aorh/2a)N-Ellipsoid(-exact)Nf-Cylinder(-exact)Nm-Cylinder(-exact)Ndf-Cylinder(-Fiorillo)Nf-RectangularPrism(-exact)Nm-RectangularPrism(-exac)Ndm-RectangularPrism(-Fiorillo)Ndm-RectangularPrism(-Sato)规则形状非规则形状学习微磁学W.F.Brown,Jr.,Magnetostaticprinciplesinferromagnetism,1962,North-HollandPublishingCompany
- 配套讲稿:
如PPT文件的首页显示word图标,表示该PPT已包含配套word讲稿。双击word图标可打开word文档。
- 特殊限制:
部分文档作品中含有的国旗、国徽等图片,仅作为作品整体效果示例展示,禁止商用。设计者仅对作品中独创性部分享有著作权。
- 关 键 词:
- 磁性 测量 精品 文档
![提示](https://static.bdocx.com/images/bang_tan.gif)