不(bu)銹鋼管穿(chuan)過磁(ci)化線圈時會發生(sheng)如(ru)下(xia)兩種電磁(ci)感應(ying)現象:
1. 鋼管在橫向漏磁檢測磁化器內運動時,不(bu)銹鋼管切割磁力線而在其內部形成感生渦流。
2. 不銹鋼管(guan)磁(ci)(ci)(ci)介(jie)質在管(guan)頭進入磁(ci)(ci)(ci)化(hua)線(xian)(xian)圈(quan)(quan)和管(guan)尾離開磁(ci)(ci)(ci)化(hua)線(xian)(xian)圈(quan)(quan)時,由于(yu)磁(ci)(ci)(ci)化(hua)線(xian)(xian)圈(quan)(quan)的(de)磁(ci)(ci)(ci)通總量發生(sheng)(sheng)急劇變化(hua),線(xian)(xian)圈(quan)(quan)中會產(chan)生(sheng)(sheng)感生(sheng)(sheng)電流。
一(yi)、鋼管內產生的感生渦流
不銹鋼(gang)管橫向(xiang)缺陷漏(lou)磁檢(jian)測方(fang)法(fa)采用穿過式線圈產生軸向(xiang)磁化(hua)場(chang),并在(zai)磁化(hua)線圈內布置(zhi)檢(jian)測傳感器。當鋼(gang)管沿(yan)著軸向(xiang)移(yi)動時,處于磁化(hua)線圈內的不銹鋼(gang)管段被(bei)磁化(hua)至近飽和狀態(tai),如存在(zai)缺陷將在(zai)鋼(gang)管表面(mian)產生泄漏(lou)磁場(chang),然后被(bei)磁敏感元件(jian)拾取并依次轉換為模擬信號(hao)和數(shu)字信號(hao),最終(zhong)由計算機信號(hao)處理系統實施報警和分類(lei)。
如(ru)圖5-1所示,以鋼管軸線為(wei)(wei)中(zhong)心建(jian)立圓柱(zhu)坐標系。沿著鋼管運動方向,以磁(ci)化(hua)線圈(quan)(quan)為(wei)(wei)中(zhong)心將鋼管劃分為(wei)(wei)進入區和離(li)開區,在(zai)磁(ci)化(hua)線圈(quan)(quan)中(zhong)施(shi)加如(ru)圖所示的磁(ci)化(hua)電流,磁(ci)力(li)線分布特征為(wei)(wei):在(zai)進入區磁(ci)力(li)線從(cong)空氣中(zhong)進入鋼管,并在(zai)磁(ci)化(hua)線圈(quan)(quan)中(zhong)部匯聚,然后在(zai)離(li)開區折射入空氣中(zhong)。

如圖5-1所示,將(jiang)磁(ci)感應強度矢量B(r,z)分(fen)(fen)解為軸向分(fen)(fen)量和徑向分(fen)(fen)量,即(ji) B(r,z)=B2(r,z)+B,(r,z)
從圖5-1中可以看(kan)出,軸向(xiang)(xiang)分量(liang)B2(r,z)在(zai)(zai)(zai)(zai)(zai)進(jin)入區(qu)和離(li)開(kai)區(qu)方向(xiang)(xiang)一致,沿著鋼(gang)(gang)管(guan)前進(jin)方向(xiang)(xiang),其強(qiang)度在(zai)(zai)(zai)(zai)(zai)進(jin)入區(qu)逐漸增大(da),并(bing)在(zai)(zai)(zai)(zai)(zai)磁化線(xian)圈中部(bu)達到極大(da)值,之后在(zai)(zai)(zai)(zai)(zai)離(li)開(kai)區(qu)逐漸減小。徑向(xiang)(xiang)分量(liang)B,(r,z)在(zai)(zai)(zai)(zai)(zai)進(jin)入區(qu)方向(xiang)(xiang)指(zhi)向(xiang)(xiang)鋼(gang)(gang)管(guan)內(nei)部(bu),并(bing)在(zai)(zai)(zai)(zai)(zai)磁化線(xian)圈中部(bu)發生轉變(bian),在(zai)(zai)(zai)(zai)(zai)離(li)開(kai)區(qu)方向(xiang)(xiang)指(zhi)向(xiang)(xiang)鋼(gang)(gang)管(guan)外部(bu)。
為(wei)(wei)(wei)了研究(jiu)與鋼管同軸圓(yuan)環(huan)l(ro ,zo)的渦(wo)流(liu)分布(bu),設圓(yuan)環(huan)半徑(jing)為(wei)(wei)(wei)ro,軸向位置為(wei)(wei)(wei)200根據楞次定律,當(dang)圓(yuan)環(huan)移動時,軸向分量B,(r,z)的強(qiang)度(du)變化(hua)導致圓(yuan)環(huan)磁通量也發生(sheng)改(gai)變,從而(er)在圓(yuan)環(huan)中產(chan)生(sheng)感生(sheng)電(dian)(dian)動勢。因(yin)磁化(hua)場為(wei)(wei)(wei)軸對稱,建立圓(yuan)環(huan)感應電(dian)(dian)動勢方(fang)程(cheng)為(wei)(wei)(wei)
根據式(shi)(5-3),沿鋼管前進(jin)方向,在進(jin)入區,軸向分(fen)量強(qiang)度逐(zhu)漸增強(qiang),感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)方向與原磁(ci)化(hua)(hua)電(dian)流(liu)(liu)方向相(xiang)反;在磁(ci)化(hua)(hua)線(xian)圈中間位置,由于軸向分(fen)量變化(hua)(hua)率為零,故此部(bu)位無(wu)感(gan)(gan)(gan)生(sheng)(sheng)流(liu)(liu)產生(sheng)(sheng);在離(li)開區,軸向分(fen)量強(qiang)度由中間最大值(zhi)逐(zhu)漸減小,于是形成與原磁(ci)化(hua)(hua)電(dian)流(liu)(liu)方向相(xiang)同的(de)感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu),最終(zhong)鋼管中感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)分(fen)布(bu)如(ru)圖5-2a所示。如(ru)果改變磁(ci)化(hua)(hua)電(dian)流(liu)(liu)方向,根據式(shi)(5-3),同樣可得(de)出鋼管內感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)分(fen)布(bu),如(ru)圖5-2b所示。
從圖5-2中(zhong)可以看出,鋼(gang)管(guan)(guan)中(zhong)感生(sheng)(sheng)(sheng)電(dian)(dian)流(liu)分布方向(xiang)(xiang)由磁(ci)(ci)化(hua)電(dian)(dian)流(liu)方向(xiang)(xiang)和鋼(gang)管(guan)(guan)運動(dong)方向(xiang)(xiang)共同決定。在(zai)(zai)(zai)進入(ru)區,鋼(gang)管(guan)(guan)中(zhong)的感生(sheng)(sheng)(sheng)渦流(liu)J1與(yu)磁(ci)(ci)化(hua)電(dian)(dian)流(liu)方向(xiang)(xiang)相反;在(zai)(zai)(zai)磁(ci)(ci)化(hua)線圈(quan)中(zhong)間位置無感生(sheng)(sheng)(sheng)渦流(liu)產(chan)生(sheng)(sheng)(sheng);在(zai)(zai)(zai)離開區,感生(sheng)(sheng)(sheng)渦流(liu)J2與(yu)磁(ci)(ci)化(hua)電(dian)(dian)流(liu)方向(xiang)(xiang)相同。從而,在(zai)(zai)(zai)感生(sheng)(sheng)(sheng)渦流(liu)產(chan)生(sheng)(sheng)(sheng)的磁(ci)(ci)場作用下,鋼(gang)管(guan)(guan)的磁(ci)(ci)化(hua)狀態(tai)將發生(sheng)(sheng)(sheng)變(bian)化(hua)。

建立如(ru)圖(tu)5-3所示(shi)的仿真模型。鋼(gang)管直徑為(wei)(wei)400mm、壁厚為(wei)(wei)15mm、長(chang)度為(wei)(wei)3000mm,材質為(wei)(wei)25鋼(gang)(電(dian)導率為(wei)(wei))。磁化線(xian)圈內(nei)徑為(wei)(wei)440mm、外徑為(wei)(wei)750mm、厚度為(wei)(wei)160mm,磁化電(dian)流(liu)密度iA/㎡,電(dian)流(liu)方向如(ru)圖(tu)5-3所示(shi)。

對(dui)不(bu)銹鋼管(guan)中的(de)感(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)分(fen)(fen)布(bu)進(jin)行(xing)仿真研究。磁化線圈固定不(bu)動(dong),鋼管(guan)運行(xing)速度設置為1m/s,不(bu)銹鋼管(guan)從左(zuo)端進(jin)人并向右端移動(dong),當鋼管(guan)中心與(yu)磁化線圈中心重合時獲取感(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)分(fen)(fen)布(bu)云圖(tu),如圖(tu)5-4所示。從圖(tu)中可(ke)以看出,進(jin)入區的(de)感(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)方向與(yu)磁化電(dian)流(liu)(liu)方向相(xiang)反,離(li)(li)開區的(de)感(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)方向與(yu)磁化電(dian)流(liu)(liu)方向相(xiang)同(tong),在線圈中部感(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)幾乎為零。進(jin)入區和離(li)(li)開區的(de)渦(wo)流(liu)(liu)分(fen)(fen)布(bu)相(xiang)對(dui)于線圈呈對(dui)稱分(fen)(fen)布(bu),方向相(xiang)反,強(qiang)度基本相(xiang)同(tong),仿真結(jie)果與(yu)圖(tu)5-2所示的(de)渦(wo)流(liu)(liu)分(fen)(fen)布(bu)理論分(fen)(fen)析結(jie)論相(xiang)同(tong),其(qi)中感(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)最大值為1.4×105A/㎡。
為了研究感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)(liu)(liu)與(yu)不(bu)銹(xiu)鋼(gang)管運(yun)(yun)(yun)行(xing)速(su)(su)度(du)(du)(du)的關系,分別取速(su)(su)度(du)(du)(du)0.1m/s、1m/s、2m/s、5m/s、8m/s、10m/s、20m/s、30m/s、40m/s和50m/s進行(xing)仿真。當(dang)鋼(gang)管中部(bu)與(yu)磁(ci)化線圈重合時提(ti)取渦(wo)流(liu)(liu)(liu)(liu)密(mi)(mi)度(du)(du)(du)最(zui)大值(zhi)(zhi)和最(zui)小(xiao)(xiao)值(zhi)(zhi),繪制成如圖5-5所(suo)示的渦(wo)流(liu)(liu)(liu)(liu)密(mi)(mi)度(du)(du)(du)與(yu)運(yun)(yun)(yun)行(xing)速(su)(su)度(du)(du)(du)關系曲線。從圖中可(ke)以看(kan)出,感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)(liu)(liu)與(yu)不(bu)銹(xiu)鋼(gang)管運(yun)(yun)(yun)行(xing)速(su)(su)度(du)(du)(du)成近(jin)似正比關系。鋼(gang)管低速(su)(su)運(yun)(yun)(yun)動時感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)(liu)(liu)很小(xiao)(xiao),可(ke)忽略不(bu)計;當(dang)運(yun)(yun)(yun)行(xing)速(su)(su)度(du)(du)(du)增(zeng)至50m/s時,渦(wo)流(liu)(liu)(liu)(liu)密(mi)(mi)度(du)(du)(du)為2。此時,感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)(liu)(liu)已(yi)接近(jin)傳導電(dian)流(liu)(liu)(liu)(liu)密(mi)(mi)度(du)(du)(du)。因此,高速(su)(su)運(yun)(yun)(yun)動時,感(gan)(gan)(gan)生(sheng)(sheng)渦(wo)流(liu)(liu)(liu)(liu)對鋼(gang)管漏磁(ci)檢測的影響不(bu)可(ke)忽視。

二、磁化線圈中產生(sheng)的感生(sheng)電流
當不銹鋼管端部(bu)進入(ru)和離開磁(ci)(ci)化線(xian)(xian)圈時(shi)(shi),線(xian)(xian)圈中的(de)磁(ci)(ci)通(tong)量(liang)(liang)發生(sheng)變(bian)化而產(chan)生(sheng)感(gan)(gan)(gan)生(sheng)電(dian)(dian)流(liu)。設磁(ci)(ci)化電(dian)(dian)源提供的(de)電(dian)(dian)壓為(wei)Uo,磁(ci)(ci)化線(xian)(xian)圈電(dian)(dian)阻為(wei)R,則磁(ci)(ci)化電(dian)(dian)源在線(xian)(xian)圈中產(chan)生(sheng)的(de)初始(shi)傳導(dao)(dao)電(dian)(dian)流(liu)為(wei)Io=Uo/RR。磁(ci)(ci)化線(xian)(xian)圈通(tong)過的(de)磁(ci)(ci)通(tong)總量(liang)(liang)為(wei)Φ,當磁(ci)(ci)化線(xian)(xian)圈中磁(ci)(ci)通(tong)總量(liang)(liang)發生(sheng)變(bian)化時(shi)(shi),根據楞次定律,線(xian)(xian)圈中將產(chan)生(sheng)感(gan)(gan)(gan)生(sheng)電(dian)(dian)動勢,對應(ying)的(de)感(gan)(gan)(gan)生(sheng)電(dian)(dian)流(liu)磁(ci)(ci)化線(xian)(xian)圈中通(tong)過的(de)電(dian)(dian)流(liu)I為(wei)初始(shi)傳導(dao)(dao)電(dian)(dian)流(liu)和感(gan)(gan)(gan)生(sheng)電(dian)(dian)流(liu)之和,即(ji)
當線(xian)圈中(zhong)沒有鋼管時(shi),磁(ci)(ci)化(hua)(hua)線(xian)圈磁(ci)(ci)通(tong)總量(liang)(liang)為線(xian)圈自(zi)身產生(sheng)的靜態磁(ci)(ci)通(tong)量(liang)(liang),其與磁(ci)(ci)化(hua)(hua)電(dian)流(liu)強度成正比,當磁(ci)(ci)化(hua)(hua)電(dian)流(liu)不(bu)變時(shi),線(xian)圈磁(ci)(ci)通(tong)總量(liang)(liang)也不(bu)發(fa)生(sheng)變化(hua)(hua)。此時(shi)線(xian)圈中(zhong)通(tong)過的電(dian)流(liu)為磁(ci)(ci)化(hua)(hua)電(dian)源(yuan)產生(sheng)的初始磁(ci)(ci)化(hua)(hua)傳(chuan)導(dao)電(dian)流(liu)
當(dang)管頭(tou)進入磁(ci)化線(xian)圈(quan)(quan)時,具有高磁(ci)導率的鋼管磁(ci)介質(zhi)進入磁(ci)化線(xian)圈(quan)(quan)內部,使得線(xian)圈(quan)(quan)內部的磁(ci)通總量(liang)增大。根據式(5-4),磁(ci)化線(xian)圈(quan)(quan)中(zhong)會產生與初始磁(ci)化傳導電(dian)(dian)流(liu)方向相(xiang)反(fan)的感生電(dian)(dian)流(liu),此時線(xian)圈(quan)(quan)中(zhong)通過(guo)的電(dian)(dian)流(liu)為,如圖5-6a所示(shi)。
當(dang)管體通過磁化線(xian)圈(quan)(quan)(quan)時,線(xian)圈(quan)(quan)(quan)內(nei)部(bu)磁介質總量(liang)及分(fen)布特性(xing)基本(ben)不變(bian),從而線(xian)圈(quan)(quan)(quan)內(nei)部(bu)的磁通總量(liang)也保(bao)持恒定(ding)。根據(ju)式(5-4),磁化線(xian)圈(quan)(quan)(quan)基本(ben)無(wu)感生(sheng)電(dian)(dian)流產生(sheng),此(ci)時,磁化線(xian)圈(quan)(quan)(quan)中(zhong)通過的電(dian)(dian)流與(yu)無(wu)鋼(gang)管時相同,為(wei)磁化電(dian)(dian)源產生(sheng)的初始磁化傳(chuan)導電(dian)(dian)流1=,如圖5-6b所示。
當管(guan)尾離開磁(ci)(ci)(ci)化(hua)(hua)線圈(quan)時,由(you)于線圈(quan)內(nei)部的高磁(ci)(ci)(ci)導(dao)率磁(ci)(ci)(ci)介質(zhi)不(bu)斷減少,導(dao)致磁(ci)(ci)(ci)化(hua)(hua)線圈(quan)的磁(ci)(ci)(ci)通(tong)總量也不(bu)斷減少。根(gen)據(ju)式(5-4),磁(ci)(ci)(ci)化(hua)(hua)線圈(quan)中(zhong)會產生與初始磁(ci)(ci)(ci)化(hua)(hua)傳導(dao)電流(liu)方向相同的感(gan)生電流(liu),此(ci)時線圈(quan)中(zhong)通(tong)過的電流(liu)為,如圖5-6c所示。

不銹鋼管(guan)內的(de)(de)磁場(chang)包括:磁化線(xian)(xian)圈(quan)通(tong)過(guo)電流(liu)(liu)(liu)(liu)I產生(sheng)(sheng)的(de)(de)磁場(chang)和鋼管(guan)中(zhong)(zhong)感生(sheng)(sheng)渦(wo)(wo)流(liu)(liu)(liu)(liu)J形成的(de)(de)磁場(chang)。磁化線(xian)(xian)圈(quan)的(de)(de)磁通(tong)總量(liang)(liang)包含了由感生(sheng)(sheng)渦(wo)(wo)流(liu)(liu)(liu)(liu)J產生(sheng)(sheng)的(de)(de)部分磁通(tong)量(liang)(liang),因此(ci)鋼管(guan)中(zhong)(zhong)的(de)(de)渦(wo)(wo)流(liu)(liu)(liu)(liu)效應會對磁化線(xian)(xian)圈(quan)中(zhong)(zhong)的(de)(de)感生(sheng)(sheng)電流(liu)(liu)(liu)(liu)產生(sheng)(sheng)一定(ding)影(ying)響(xiang)。
采用如(ru)(ru)圖(tu)5-3所示(shi)模(mo)型,進(jin)一步(bu)研究磁化(hua)(hua)(hua)線(xian)圈(quan)中產生(sheng)的(de)感(gan)生(sheng)電(dian)(dian)流(liu)變化(hua)(hua)(hua)規律。其中,線(xian)圈(quan)匝(za)數為(wei)600匝(za),磁化(hua)(hua)(hua)電(dian)(dian)流(liu)為(wei)5A。當鋼管(guan)(guan)(guan)(guan)(guan)管(guan)(guan)(guan)(guan)(guan)頭(tou)、管(guan)(guan)(guan)(guan)(guan)體和(he)管(guan)(guan)(guan)(guan)(guan)尾(wei)分(fen)(fen)別與磁化(hua)(hua)(hua)線(xian)圈(quan)耦合時提(ti)取磁化(hua)(hua)(hua)線(xian)圈(quan)內(nei)部產生(sheng)的(de)感(gan)生(sheng)電(dian)(dian)流(liu),如(ru)(ru)圖(tu)5-7所示(shi)。仿(fang)真(zhen)分(fen)(fen)兩種:一是考(kao)慮(lv)鋼管(guan)(guan)(guan)(guan)(guan)渦(wo)(wo)流(liu)效應時分(fen)(fen)析(xi)線(xian)圈(quan)感(gan)生(sheng)電(dian)(dian)流(liu)與運動速(su)度(du)的(de)關系(xi),二(er)是忽略(lve)鋼管(guan)(guan)(guan)(guan)(guan)渦(wo)(wo)流(liu)效應而單獨分(fen)(fen)析(xi)線(xian)圈(quan)感(gan)生(sheng)電(dian)(dian)流(liu)與鋼管(guan)(guan)(guan)(guan)(guan)運動速(su)度(du)關系(xi)。分(fen)(fen)別取速(su)度(du)0.1m/s、1m/s、2m/s、5m/s、8m/s、10m/s、20m/s、30m/s、40m/和(he)50m/s進(jin)行(xing)仿(fang)真(zhen),獲得(de)如(ru)(ru)圖(tu)5-8所示(shi)的(de)磁化(hua)(hua)(hua)線(xian)圈(quan)感(gan)生(sheng)電(dian)(dian)流(liu)與運動速(su)度(du)關系(xi)曲線(xian)。其中I1csI2cs和(he)I3cs分(fen)(fen)別為(wei)考(kao)慮(lv)鋼管(guan)(guan)(guan)(guan)(guan)渦(wo)(wo)流(liu)效應時在管(guan)(guan)(guan)(guan)(guan)頭(tou)、管(guan)(guan)(guan)(guan)(guan)體和(he)管(guan)(guan)(guan)(guan)(guan)尾(wei)處線(xian)圈(quan)中產生(sheng)的(de)感(gan)生(sheng)電(dian)(dian)流(liu),11cI2c和(he)I3c分(fen)(fen)別為(wei)忽略(lve)不銹鋼管(guan)(guan)(guan)(guan)(guan)渦(wo)(wo)流(liu)效應時磁化(hua)(hua)(hua)線(xian)圈(quan)中產生(sheng)的(de)感(gan)生(sheng)電(dian)(dian)流(liu)。

圖5-8所(suo)示(shi)的(de)(de)仿真結(jie)果與圖5-6所(suo)示(shi)的(de)(de)理論(lun)分析結(jie)論(lun)相同:當管頭(tou)進入(ru)磁(ci)(ci)化線(xian)(xian)圈(quan)(quan)(quan)時(shi)(shi)(shi),線(xian)(xian)圈(quan)(quan)(quan)中(zhong)產(chan)(chan)生(sheng)(sheng)(sheng)(sheng)的(de)(de)感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)幅值為負(fu),即與磁(ci)(ci)化電(dian)流(liu)(liu)(liu)方(fang)向相反;當管體(ti)通(tong)過磁(ci)(ci)化線(xian)(xian)圈(quan)(quan)(quan)時(shi)(shi)(shi),線(xian)(xian)圈(quan)(quan)(quan)中(zhong)基(ji)本(ben)無(wu)感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)產(chan)(chan)生(sheng)(sheng)(sheng)(sheng);隨著管尾(wei)離(li)開磁(ci)(ci)化線(xian)(xian)圈(quan)(quan)(quan),此時(shi)(shi)(shi)線(xian)(xian)圈(quan)(quan)(quan)中(zhong)產(chan)(chan)生(sheng)(sheng)(sheng)(sheng)與磁(ci)(ci)化電(dian)流(liu)(liu)(liu)方(fang)向相同的(de)(de)感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)。根據楞次(ci)定(ding)律(lv),線(xian)(xian)圈(quan)(quan)(quan)中(zhong)產(chan)(chan)生(sheng)(sheng)(sheng)(sheng)的(de)(de)感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)會阻礙線(xian)(xian)圈(quan)(quan)(quan)磁(ci)(ci)通(tong)量的(de)(de)變化:當管頭(tou)進入(ru)磁(ci)(ci)化線(xian)(xian)圈(quan)(quan)(quan)時(shi)(shi)(shi),線(xian)(xian)圈(quan)(quan)(quan)中(zhong)會產(chan)(chan)生(sheng)(sheng)(sheng)(sheng)反向感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)來阻礙磁(ci)(ci)通(tong)量的(de)(de)增大;當管體(ti)與磁(ci)(ci)化線(xian)(xian)圈(quan)(quan)(quan)耦合時(shi)(shi)(shi),由于(yu)線(xian)(xian)圈(quan)(quan)(quan)磁(ci)(ci)通(tong)量基(ji)本(ben)不(bu)變而無(wu)感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)產(chan)(chan)生(sheng)(sheng)(sheng)(sheng);當管尾(wei)離(li)開磁(ci)(ci)化線(xian)(xian)圈(quan)(quan)(quan)時(shi)(shi)(shi),線(xian)(xian)圈(quan)(quan)(quan)中(zhong)會產(chan)(chan)生(sheng)(sheng)(sheng)(sheng)同向感(gan)(gan)(gan)生(sheng)(sheng)(sheng)(sheng)電(dian)流(liu)(liu)(liu)來阻礙磁(ci)(ci)通(tong)量的(de)(de)減小。
另(ling)外,從圖5-8中(zhong)可以看出,在(zai)運行速(su)(su)度(du)較(jiao)低時,磁(ci)(ci)(ci)化線(xian)圈中(zhong)感(gan)生(sheng)電流(liu)隨著速(su)(su)度(du)的增加(jia)而快(kuai)速(su)(su)上升;當速(su)(su)度(du)達到一定幅值時,磁(ci)(ci)(ci)化線(xian)圈中(zhong)的感(gan)生(sheng)電流(liu)基本(ben)保(bao)持不變。因為感(gan)生(sheng)電流(liu)只(zhi)能減緩磁(ci)(ci)(ci)化線(xian)圈磁(ci)(ci)(ci)通量(liang)的變化速(su)(su)度(du),而不能改變磁(ci)(ci)(ci)通量(liang)的變化趨勢(shi)。
從圖5-8中(zhong)還可以(yi)看出,鋼管(guan)中(zhong)的(de)渦流會削弱磁化(hua)線圈中(zhong)產生(sheng)的(de)感生(sheng)電流,根據楞次(ci)定律,鋼(gang)(gang)(gang)(gang)管(guan)中(zhong)的(de)渦(wo)流(liu)(liu)同樣會阻礙鋼(gang)(gang)(gang)(gang)管(guan)中(zhong)磁(ci)(ci)通量的(de)變(bian)(bian)化。當不銹鋼(gang)(gang)(gang)(gang)管(guan)進(jin)入和離(li)開磁(ci)(ci)化線(xian)圈(quan)時,鋼(gang)(gang)(gang)(gang)管(guan)中(zhong)的(de)磁(ci)(ci)通量變(bian)(bian)化規律同樣先增(zeng)大后(hou)減小。由于磁(ci)(ci)化線(xian)圈(quan)磁(ci)(ci)通總量包(bao)含(han)了不銹鋼(gang)(gang)(gang)(gang)管(guan)磁(ci)(ci)通量,所以(yi),感生(sheng)(sheng)渦(wo)流(liu)(liu)在阻礙鋼(gang)(gang)(gang)(gang)管(guan)磁(ci)(ci)通量變(bian)(bian)化的(de)同時也阻礙了線(xian)圈(quan)磁(ci)(ci)通量的(de)變(bian)(bian)化速率,最(zui)終削弱了線(xian)圈(quan)感生(sheng)(sheng)電流(liu)(liu)的(de)強(qiang)度。

