$A$ black body radiates maximum energy at wavelength $\lambda$ at temperature $T_1$ and its emissive power is $E$. When the temperature of the body is changed to $T_2$, it radiates maximum energy at wavelength $\frac{2\lambda}{3}$, then the emissive power will become

  • A
    $\frac{99}{16}E$
  • B
    $\frac{81}{16}E$
  • C
    $\frac{63}{16}E$
  • D
    $\frac{45}{16}E$

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