Q.5
ICAR AIEEA PG Statistical Sciences 09 July 2023 (Shift 1) Paper (Q.101)
MCQ (Single Correct) +4 −1
If $\theta = t^n e^{-\frac{r^2}{4t}}$, then the value of $n$ that will make $\frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2 \frac{\partial \theta}{\partial r}\right) = \frac{\partial \theta}{\partial t}$ is given by :
यदि $\theta = t^n e^{-\frac{r^2}{4t}}$ है, तो $n$ का वह मान जो समीकरण $\frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2 \frac{\partial \theta}{\partial r}\right) = \frac{\partial \theta}{\partial t}$ को संतुष्ट करेगा, होगा :

Given $\theta = t^n e^{-r^2/(4t)}$. Let $u = -r^2/(4t)$, so $\theta = t^n e^u$.
Calculate spatial derivatives:
$\frac{\partial \theta}{\partial r} = t^n e^u \left(-\frac{2r}{4t}\right) = -\frac{r}{2} t^{n-1} e^u$.
Then $r^2 \frac{\partial \theta}{\partial r} = -\frac{1}{2} t^{n-1} r^3 e^u$.
Differentiating with respect to $r$:
$\frac{\partial}{\partial r}\left(r^2 \frac{\partial \theta}{\partial r}\right) = -\frac{1}{2} t^{n-1} \left[3r^2 e^u + r^3 e^u \left(-\frac{r}{2t}\right)\right] = -\frac{1}{2} t^{n-1} e^u \left[3r^2 - \frac{r^4}{2t}\right]$.
Dividing by $r^2$:
$\text{LHS} = \frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2 \frac{\partial \theta}{\partial r}\right) = e^u \left[-\frac{3}{2} t^{n-1} + \frac{r^2}{4} t^{n-2}\right]$.
Now calculate time derivative:
$\text{RHS} = \frac{\partial \theta}{\partial t} = n t^{n-1} e^u + t^n e^u \left(\frac{r^2}{4t^2}\right) = e^u \left[n t^{n-1} + \frac{r^2}{4} t^{n-2}\right]$.
Equating LHS and RHS:
$-\frac{3}{2} t^{n-1} + \frac{r^2}{4} t^{n-2} = n t^{n-1} + \frac{r^2}{4} t^{n-2}$.
Comparing coefficients of $t^{n-1}$ yields:
$n = -\frac{3}{2}$.

Detailed analysis of options:

  • 0 is incorrect.
  • is incorrect.
  • $-1/2$ corresponds to 1D diffusion, not 3D spherical coordinates.
  • $-3/2$ is the correct value corresponding to 3-dimensional spherical diffusion.

दिया गया है $\theta = t^n e^{-\frac{r^2}{4t}}$।
त्रिज्यीय अवकलज (radial derivatives) ज्ञात करने पर:
$\frac{\partial \theta}{\partial r} = t^n e^{-\frac{r^2}{4t}}\left(-\frac{2r}{4t}\right) = -\frac{r}{2} t^{n-1} e^{-\frac{r^2}{4t}}$.
$r^2 \frac{\partial \theta}{\partial r} = -\frac{1}{2} t^{n-1} r^3 e^{-\frac{r^2}{4t}}$.
$r$ के सापेक्ष पुनः अवकलन करके $r^2$ से भाग देने पर:
$\text{LHS} = \frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2 \frac{\partial \theta}{\partial r}\right) = e^{-\frac{r^2}{4t}}\left[-\frac{3}{2} t^{n-1} + \frac{r^2}{4} t^{n-2}\right]$.
अब समय के सापेक्ष अवकलज (time derivative):
$\text{RHS} = \frac{\partial \theta}{\partial t} = n t^{n-1} e^{-\frac{r^2}{4t}} + t^n e^{-\frac{r^2}{4t}}\left(\frac{r^2}{4t^2}\right) = e^{-\frac{r^2}{4t}}\left[n t^{n-1} + \frac{r^2}{4} t^{n-2}\right]$.
दोनों पक्षों (LHS और RHS) की तुलना करने पर:
$-\frac{3}{2} t^{n-1} = n t^{n-1} \implies n = -\frac{3}{2}$.

विकल्पों का विस्तृत विश्लेषण:

  • 0 गलत है।
  • गलत है।
  • $-1/2$ एक-विमीय विसरण (1D diffusion) के लिए होता है।
  • $-3/2$ सही उत्तर है (त्रिविमीय गोलीय निर्देशांकों हेतु)।
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