极坐标系中直线ρsinθ=-2怎样化为普通直角坐标方程 在极坐标系中,直线l的极坐标方程为ρsin(θ+π8)=2,...

\u5c06\u66f2\u7ebf\u6781\u5750\u6807\u65b9\u7a0b\u03c1=-2sin\u03b8\u5316\u4e3a\u76f4\u89d2\u5750\u6807\u65b9\u7a0b

\u03c1=-2sin\u03b8
\u03c1²=-2\u03c1sin\u03b8
\u03c1²=x²+y²\uff0c\u03c1sin\u03b8=y\u4ee3\u5165\uff0c\u5f97x²+y²=-2y
x²+y²+2y=0
x²+y²+2y+1=1
x²+(y+1)²=1
\u6240\u6c42\u76f4\u89d2\u5750\u6807\u65b9\u7a0b\u4e3ax²+(y+1)²=1\uff0c\u662f\u4ee5(0\uff0c-1)\u4e3a\u5706\u5fc3\uff0c1\u4e3a\u534a\u5f84\u7684\u5706\u3002

\u2235cos\u03c08=1+cos\u03c042=2+22 sin\u03c08=1?cos\u03c042=2?22\uff0c\u518d\u6839\u636ex=\u03c1cos\u03b8\uff0cy=\u03c1sin\u03b8\uff0c\u628a\u76f4\u7ebfl\u7684\u6781\u5750\u6807\u65b9\u7a0b\u4e3a\u03c1sin\uff08\u03b8+\u03c08\uff09=2\u5316\u4e3a\u76f4\u89d2\u5750\u6807\u65b9\u7a0b\u4e3a<div style="width:6px;background: url('http://hiph

有公式y=ρsinθ
极坐标系中直线ρsinθ=-2
就是普通直角坐标方程y=-2

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