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1.设函数x^2+y^2≠0时,f(x,y)=xy/x^2+y^2;当x^2+y^2=0时,f(x,y)=0.问f(x,y)在(0,0)处是否连续?计算计算f’x(0,0)和f’y(0,0)2.将函数f(x)=sin(x/2)展开成x的幂级数.3.将1/(5-x)展开成为x-2的幂级数.并指出收敛

题目详情
1.设函数x^2+y^2≠0时,f(x,y)=xy/x^2+y^2 ;当x^2+y^2=0时,f(x,y)=0.
问f(x,y)在(0,0)处是否连续?计算计算f’x (0,0)和f’y (0,0)
2.将函数f(x)=sin(x/2)展开成x的幂级数.
3.将1/(5-x)展开成为x-2的幂级数.并指出收敛域.
4.求函数f(x,y)=e^(x-y)(x^2-2y^2)的极值.
5.z=xarctan(y/x),求a^2z/axay ,a^z/ax^2,a^2z/ay^2.
6.求方程xy+lny-lnx=0所确定的隐函数y=f(x)的导数dy/dx.
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答案和解析
1.设函数x²+y²≠0时,f(x,y)=xy/(x²+y²) ;当x²+y²=0时,f(x,y)=0;问f(x,y)在(0,0)处是否连续?计算计算f’x (0,0)和f’y (0,0);
当x²+y²=0时,必有x=0且y=0,此时f(x,y)=f(0,0)=0,即函数z=f(x,y)在原点有定义0;
当动点P沿x轴趋近原点时,x➔0limf(x,0)=0;当动点P沿y轴趋近原点时,y➔0limf(0,y)=0;
可见动点无论沿x轴还是沿y轴趋近原点该函数都有极限0,且此极限=f(0,0)=0;但若动点不沿坐标
轴,而沿任意方向趋近原点,情况就不一样了!
令y=kx,k∈R;则【x➔0,y=kx➔0】limf(x,y)=【x➔0,y=kx➔0】limf(x,kx)
=【x➔0,y=kx➔0】limkx²/(x²+k²x²)=k/(1+k²),可见极限值与k有关;由此即可判断该函数f(x,y)在原点没有极限,极在原点不连续.f’x (0,0)=0,f’y (0,0)=0.
【在一元函数里,有导数必连续;但在多元函数里,所有偏导数都存在,但不一定连续,此即
为一例】
2.将函数f(x)=sin(x/2)展开成x的幂级数.
f(0)=0;f'(x)=(1/2)cos(x/2)=(1/2)sin(π/2+x);f''(x)=-(1/2²)sin(x/2)=(1/2²)sin(π+x/2);
f'''(x)=-(1/2³)cos(x/2)=(1/2³)sin(3π/2+x/2);f''''(x)=(1/2⁴)sin(x/2)=(1/2⁴)sin(2π+x/2);
.;f⁽ⁿ⁾(x)=(1/2ⁿ)sin(nπ/2+x/2).
f'(0)=1/2;f''(0)=0;f'''(0)=-1/2³;f''''(0)=0;.;f⁽ⁿ⁾(0)=(1/2ⁿ)sin(nπ/2);
故sin(x/2)=(1/2)x-[1/(2³▪3!)]x³+[1/(2⁵▪5!)]x⁵-[1/(2⁷▪7!)]x⁷+.
3.将1/(5-x)展开成为x-2的幂级数.并指出收敛域.【自己作吧!】
4.求函数f(x,y)=e^(x-y)(x²-2y²)的极值.
令∂f/∂x=e^(x-y)(x²-2y²)+2xe^(x-y)=[e^(x-y)](x²+2x-2y²)=0,得x²+2x-2y²=0.(1)
再令∂f/∂y=-e^(x-y)(x²-2y²)-4ye^(x-y)=-[e^(x-y)](x²+4y-2y²)=0,得x²+4y-2y²=0.(2)
(2)-(1)得4y-2x=0,故得x=2y,代入(1)式得4y²+4y-2y²=2y²+4y=2y(y+2)=0,故得y₁=0,y₂=-2;
相应地,x₁=0,x₂=-4;即有驻点P₁(0,0);P₂(-4,-2);
∂²f/∂x²=e^(x-y)(x²+2x-2y²)+e^(x-y)(2x+2)=e^(x-y)(x²+4x-2y²+2)
∂²f/∂x∂y=-e^(x-y)(x²+2x-2y²)-4ye^(x-y)=-e^(x-y)(x²+2x+4y-2y²)
∂²f/∂y²=e^(x-y)(x²+4y-2y²)-e^(x-y)(4-4y)=e^(x-y)(x²+8y-2y²-4)
对P₁(0,0):A=∂²f/∂x²=2;B=∂²f/∂x∂y=0;C=∂²f/∂y²=-4;B²-AC=0+16>0,
故P₁不是极值点;
对P₂(-4,-2):A=(1/e²)(16-16-8+2)=-6/e²;B=-(1/e²)(16-8-8-8)=-8/e²;
C=(1/e²)(16-16-8-4)=-12/e²
B²-AC=(64-72)/e⁴=-8/e⁴