yungman
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I am a self studier, there might be things seems obvious to you guys that are not obvious for me. I have a few questions here, I write down the equation first and present the question in the last part. Please bare with me. Thanks.
Eulers equation of 2nd order: L[y]=x^{2} y''+ \alpha xy'+ \beta y = 0 (3)
Let y = x^{r}
=> L[x^{r}]=x^{r}[r(r-1)+\alpha x(x^{r})'+ \beta (x^{r})] = 0
If r is a root of the quadratic equation: F(r)=r(r-1)+\alpha r + \beta = 0
r_{1} , r_{2} =\frac{-(\alpha - 1)^{+}_{-}\sqrt{(\alpha-1)^{2}-4\beta}}{2}
and
F(r)=(r-r_{1})(r-r_{2})
For r_{1} = r_{2}, F(r)=(r-r_{1})^{2}, Both F(r) and F'(r) =0.
We only find y_{1}=x^{r}. We need to find y_{2}.
We differentiating(3) \frac{d}{dr}[L(x^{r}]=\frac{d}{dr}{x^{r}F(r)](4)
\frac{dx^{r}}{dr}=x^{r}ln(x)
L[x^{r}ln(x)]=(r-r_{1})^{2}x^{r}ln(x)+2(r-r_{1})x^{r}(5)
For r=r_{1}, right side of (5) equal to zero.
Therefore y_{2}(x)=x^{r_{1}}ln(x).
My questions are:
1) How is \frac{d}{dr}[L(x^{r}]=\frac{d[x^{r}ln(x)]}{dr} from (4) to (5)?
2) Why For r=r_{1}, right side of (5) equal to zero. And therefore y_{2}(x)=x^{r_{1}}ln(x)?
Eulers equation of 2nd order: L[y]=x^{2} y''+ \alpha xy'+ \beta y = 0 (3)
Let y = x^{r}
=> L[x^{r}]=x^{r}[r(r-1)+\alpha x(x^{r})'+ \beta (x^{r})] = 0
If r is a root of the quadratic equation: F(r)=r(r-1)+\alpha r + \beta = 0
r_{1} , r_{2} =\frac{-(\alpha - 1)^{+}_{-}\sqrt{(\alpha-1)^{2}-4\beta}}{2}
and
F(r)=(r-r_{1})(r-r_{2})
For r_{1} = r_{2}, F(r)=(r-r_{1})^{2}, Both F(r) and F'(r) =0.
We only find y_{1}=x^{r}. We need to find y_{2}.
We differentiating(3) \frac{d}{dr}[L(x^{r}]=\frac{d}{dr}{x^{r}F(r)](4)
\frac{dx^{r}}{dr}=x^{r}ln(x)
L[x^{r}ln(x)]=(r-r_{1})^{2}x^{r}ln(x)+2(r-r_{1})x^{r}(5)
For r=r_{1}, right side of (5) equal to zero.
Therefore y_{2}(x)=x^{r_{1}}ln(x).
My questions are:
1) How is \frac{d}{dr}[L(x^{r}]=\frac{d[x^{r}ln(x)]}{dr} from (4) to (5)?
2) Why For r=r_{1}, right side of (5) equal to zero. And therefore y_{2}(x)=x^{r_{1}}ln(x)?
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