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    Given that the Earth is in radiative equilibrium and the equivalent black body temperature of the Earth without having any atmosphere is T1​. If the S
    Question

    Given that the Earth is in radiative equilibrium and the equivalent black body temperature of the Earth without having any atmosphere is T1​. If the Sun’s emission changes abruptly such that the solar constant increases to four times its previous value, the new equivalent black body temperature of the Earth will be:

    A.

    2T1

    B.

    4T1

    C.

    4 2/3 T1

    D.

    T1

    Correct option is D

    Introduction:

    • For a planet to maintain a stable temperature, it must be in Radiative Equilibrium, meaning the energy it absorbs from the Sun must equal the energy it radiates back into space.
    • Earth absorbs solar radiation (shortwave) over its cross-sectional area (πR2\pi R^2​ and emits terrestrial radiation (longwave) over its entire surface area (4πR24\pi R^2​).
    • According to the Stefan-Boltzmann Law, the energy flux ($E$) emitted by a black body is directly proportional to the fourth power of its absolute temperature (T):
    • E=σT4E = \sigma T^4​​
    • where σ\sigma​ is the Stefan-Boltzmann constant (5.67×108 W/m2K45.67 \times 10^{-8} \text{ W/m}^2\text{K}^4​). By equating the incoming and outgoing energy, we establish the relationship between the Solar Constant (S) and the Earth's equilibrium temperature (T):
    • S(1A)πR2=σT4(4πR2)S(1 - A) \pi R^2 = \sigma T^4 (4\pi R^2)​​
    • S(1A)4=σT4\frac{S(1-A)}{4} = \sigma T^4​​
    • This implies that TS1/4T \propto S^{1/4}​​

    Information Booster:

    • The "equivalent black body temperature" T1T_1​ is derived from the initial solar constant (S1S_1​). We can determine the new temperature (T2T_2​) when the solar constant increases to four times its original value (S2=4S1S_2 = 4S_1).​
    • Step-by-step Derivation:
    1. Initial State:

      T1=(S1(1A)4σ)1/4T_1 = \left( \frac{S_1(1-A)}{4\sigma} \right)^{1/4}​​
    2. New State S2=4S1S_2 = 4S_1​​

      T2=(4S1(1A)4σ)1/4T_2 = \left( \frac{4S_1(1-A)}{4\sigma} \right)^{1/4}​​
    3. Ratio Calculation:

      T2T1=(4S1)1/4(S1)1/4=41/4\frac{T_2}{T_1} = \frac{(4S_1)^{1/4}}{(S_1)^{1/4}} = 4^{1/4}​​
    4. Simplifying the Power:

      Since 4=22,wecanwrite41/4as(22)1/4=22/4=21/24 = 2^2, we can write 4^{1/4} as (2^2)^{1/4} = 2^{2/4} = 2^{1/2}​​

      T2=21/2T1=2T1T_2 = 2^{1/2} T_1 = \sqrt{2} T_1​​
      The new temperature is 2T1\sqrt{2} T_1​ (approximately 1.41 T1T_1).


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