在光滑的直角坐標(biāo)系xOy水平面的第一象限內(nèi)分布有磁感應(yīng)強(qiáng)度的大小為B、方向垂直紙面向內(nèi)的勻強(qiáng)磁場(chǎng)。在xOy平面內(nèi)放置一單匝矩形導(dǎo)線(xiàn)框abcd,線(xiàn)框邊長(zhǎng)ab = L、ad = 2L,電阻為R,質(zhì)量為m。t = 0時(shí),bc邊與Oy軸重合,線(xiàn)框以初速度υ0沿x軸正方向進(jìn)入磁場(chǎng),不計(jì)空氣阻力。
(1)求cd邊剛進(jìn)入磁場(chǎng)時(shí),c、d間的電勢(shì)差U;
(2)試討論求線(xiàn)框最終速度大小及對(duì)應(yīng)的初速度υ0的范圍;
(3)求線(xiàn)框進(jìn)入磁場(chǎng)的過(guò)程中通過(guò)導(dǎo)線(xiàn)橫截面的電荷量q大;
【猜題理由】電磁感應(yīng)問(wèn)題是近年江蘇高考的必考的內(nèi)容,往年高考中沒(méi)有同時(shí)考查瞬時(shí)感應(yīng)電動(dòng)勢(shì)和平均感應(yīng)電動(dòng)勢(shì),2010年高考很可能以討論運(yùn)動(dòng)狀態(tài)、微積分等難度設(shè)置高門(mén)檻作為壓軸題,以法拉第電磁感應(yīng)定律、閉合電路歐姆定律、部分電路歐姆定律、動(dòng)量定理為規(guī)律命題。
【標(biāo)準(zhǔn)解答】⑴線(xiàn)框cd邊剛進(jìn)入磁場(chǎng)時(shí),切割磁感線(xiàn)的速度為υ0,線(xiàn)框中電動(dòng)勢(shì)大小
E = B Lυ0············································································································· ①(1分)
導(dǎo)線(xiàn)中的電流大小
I = ············································································································· ②(1分)
c、d間的電勢(shì)差
U = I · R = BLυ0 ······················································································· ③(1分)
(2)線(xiàn)框進(jìn)入磁場(chǎng)的過(guò)程中速度為υ時(shí),受到的安培力
F = BiL = B L = ········································································· ④(1分)
在t→t + Δt時(shí)間內(nèi),由動(dòng)量定理
– FΔt=mΔυ··································································································· ⑤(1分)
求和得 – ∑υ△t = ∑mΔυ
若x < 2L時(shí),線(xiàn)框速度為零,以后保持靜止?fàn)顟B(tài),則
∑△x = x = mυ0 ········································································· ⑥(1分)
解得 x = ························································································ ⑦(1分)
即線(xiàn)框的初速度υ0滿(mǎn)足 0 < υ0 < 時(shí),線(xiàn)框最終速度為零。 ················· ⑧(1分)
若x ≥ 2L時(shí),線(xiàn)框速度不為零,而速度υ沿x軸正方向做勻速直線(xiàn)運(yùn)動(dòng),則
∑△x = · 2L = mυ0 – mυ································································· ⑨(1分)
得υ = υ0 – ···························································································· ⑩(1分)
即線(xiàn)框的初速度υ0滿(mǎn)足υ0 ≥ 時(shí),線(xiàn)框最終速度大小為υ0 – 。 (11)(1分)
(3)導(dǎo)線(xiàn)框的平均感應(yīng)電動(dòng)勢(shì)為
= ··································································································· (12)(1分)
導(dǎo)線(xiàn)框中的電流為
= ······································································································· (13)(1分)
線(xiàn)框進(jìn)入磁場(chǎng)的過(guò)程中通過(guò)導(dǎo)線(xiàn)橫截面的電荷量
q = △t ····································································································· (14)(1分)
得 q =
當(dāng) 0 < υ0 < 時(shí),△Ф= B · Lx = ,得q = ···················· (15)(1分)
當(dāng)υ0 ≥ 時(shí),△Ф= B · 2L2,得 q = ······································· (16)(1分)
【思維點(diǎn)拔】對(duì)于(1)、(2)兩問(wèn)要搞清瞬時(shí)感應(yīng)電動(dòng)勢(shì)和平均感應(yīng)電動(dòng)勢(shì)的區(qū)別,c、d間的電勢(shì)差U是指作為電源的cd邊的端電壓,求通過(guò)導(dǎo)線(xiàn)橫截面的電荷量時(shí)要用平均感應(yīng)電動(dòng)勢(shì)來(lái)解。本題難點(diǎn)在于要知道線(xiàn)框最終可能停止運(yùn)動(dòng),也可能勻速運(yùn)動(dòng),所以要進(jìn)行討論。進(jìn)入磁場(chǎng)的過(guò)程,受到的安培力是變力,無(wú)法用動(dòng)力學(xué)觀點(diǎn)直接求解,可以用動(dòng)量定理結(jié)合微積分求出位移,然后算出對(duì)應(yīng)的電荷量。
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