∫∫ln(1 x² y²)dσ
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极坐标∫∫(D)ln(1+x²+y²)dxdy=∫∫(D)rln(1+r²)drdθ=∫[0→2π]dθ∫[0→1]rln(1+r²)dr=2π∫[0→1]rl
{x=rcosθ、y=rsinθe²≤x²+y²≤e⁴→e²≤r²≤e⁴→e≤r≤e²∫∫_[D]ln(x²
再问:极径r积分区域为什么是0
答:设极坐标x=cosθ,y=sinθ,1
用分步积分∫x*ln(x-1)dx=1/2∫xln(x-1)dx^2=1/2x^2ln(x-1)-1/2∫x^2dln(x-1)=1/2x^2ln(x-1)-1/2∫x^2/(x-1)dx=1/2x^
复合函数f(x)=lnxg(x)=ln[ln(x)]r(x)=ln{lnln(x)]}r'(x)=[1/lnln(x)]g'(x)=[1/lnln(x)][1/ln(x)]f'(x)=[1/lnln(
∫(D)∫ln(1+x^2+y^2)dxdyD:x^2+y^2=1与两坐标所围成的位于第一象限内的闭区ρ=1,θ从0,到π/2dS=ρdθdρ∫(D)∫ln(1+x^2+y^2)dxdy=∫[0,1]
表示以e为底的对数函数符号
用分部积分法:∫x*ln(x-1)dx=1/2∫xln(x-1)dx^2=1/2x^2ln(x-1)-1/2∫x^2dln(x-1)=1/2x^2ln(x-1)-1/2∫x^2/(x-1)dx=1/2
解(极坐标法):做变换,设x=rcosθ,y=rsinθ,则dxdy=rdθdr∴原式=∫(0,2π)dθ∫(a,b)rlnrdr=2π∫(a,b)rlnrdr=2π[(r²lnr/2)|(
答:∫(0到π/2)dθ∫(0到1)ln(1+r^2)rdr算不定积分∫rln(1+r^2)dr=∫1/2ln(1+r^2)d(1+r^2)=1/2∫ln(1+r^2)d(1+r^2)∫lnxdx=x
d(ln(x^2+y))=[1/(x^2+y)].(2xdx+dy)再问:那d(2y-t*y^2)怎么算再答:t是常数d(2y-t*y^2)=(2-2ty)dyt是变数d(2y-t*y^2)=2dy-
y'=(1+x/√(1+x^2))/(x+√(1+x^2))=1/√(1+x^2)y''=-x/(1+x^2)^(3/2)
∫(r^2/r^2+1)dr=∫dr-∫1/(r^2+1)dr再问:∫1/(r^2+1)dr怎么求再答:arctanr
y=e^c·x^(-1/3)
当中那个式子有问题,应该等于=-∫(ln(x+1)-lnx)d(ln(x+1)-lnx),有个负号再问:恩我主要想知道最后答案是怎么得出来的再答:有个公式:∫f(x)d[f(x)]=[f(x)]^2/