JEE Challenger
More from Thermal Properties of Matter

Heat Radiation and Energy Loss from Human Body

Consider a human body with a surface area of approximately 1 m21\text{ m}^2. The typical body temperature exceeds the ambient room temperature T0T_0 by 10 K10\text{ K}. Assume the room temperature is T0=300 KT_0 = 300\text{ K}. Given that for T0=300 KT_0 = 300\text{ K}, σT04=460 W m−2\sigma T_0^4 = 460\text{ W m}^{-2} (where σ\sigma represents the Stefan-Boltzmann constant), select the correct statement(s):

Options

A

The energy emitted by the human body in 1 second is close to 60 Joules60\text{ Joules}.

B

If the surrounding room temperature drops by a tiny amount ΔT0≪T0\Delta T_0 \ll T_0, maintaining constant body temperature requires the person to radiate an extra energy per unit time of ΔW=4σT03ΔT0\Delta W = 4\sigma T_0^3 \Delta T_0.

C

Reducing the exposed area of the body (e.g., by curling up) enables humans to preserve their body temperature while lowering radiative energy loss.

Correct
D

If body temperature increases considerably, the peak of the electromagnetic radiation spectrum emitted by the body shifts to longer wavelengths.

Step-by-Step Solution

To determine the correct option(s), let us analyze each statement individually using the principles of thermal radiation and thermodynamics:

1. Analysis of Option [A]

According to Stefan-Boltzmann Law, the total rate of energy emitted (radiated) by a body of surface area AA at absolute temperature TT is given by: Pemitted=eσAT4P_{\text{emitted}} = e \sigma A T^4

Assuming the emissivity of human skin e≈1e \approx 1, surface area A=1 m2A = 1\text{ m}^2, room temperature T0=300 KT_0 = 300\text{ K}, and body temperature T=T0+ΔT=310 KT = T_0 + \Delta T = 310\text{ K} (where ΔT=10 K\Delta T = 10\text{ K}):

Pemitted=σAT04(1+ΔTT0)4P_{\text{emitted}} = \sigma A T_0^4 \left(1 + \frac{\Delta T}{T_0}\right)^4

Using the binomial approximation (1+x)n≈1+nx(1 + x)^n \approx 1 + nx for x=10300≪1x = \frac{10}{300} \ll 1: Pemitted≈σAT04(1+4ΔTT0)P_{\text{emitted}} \approx \sigma A T_0^4 \left(1 + 4\frac{\Delta T}{T_0}\right) Pemitted≈(460 W m−2)×(1 m2)×(1+4×10300)=460×(1+215)≈521.3 WP_{\text{emitted}} \approx (460\text{ W m}^{-2}) \times (1\text{ m}^2) \times \left(1 + 4 \times \frac{10}{300}\right) = 460 \times \left(1 + \frac{2}{15}\right) \approx 521.3\text{ W}

Thus, the energy radiated by the body in 1 second1\text{ second} is approximately 521.3 Joules521.3\text{ Joules}.

(Note: The value 60 Joules60\text{ Joules} actually corresponds to the net rate of heat loss Pnet=σA(T4−T04)≈4σAT03ΔT≈61.3 WP_{\text{net}} = \sigma A (T^4 - T_0^4) \approx 4 \sigma A T_0^3 \Delta T \approx 61.3\text{ W}, not the total energy radiated).

Therefore, Option [A] is incorrect.


2. Analysis of Option [B]

The power radiated by the human body depends only on its own surface area, emissivity, and absolute body temperature TT: Pemitted=eσAT4P_{\text{emitted}} = e \sigma A T^4

If the surrounding room temperature drops by ΔT0\Delta T_0, but the body temperature TT is kept constant, the rate at which the body emits radiation remains unchanged.

However, the power absorbed from the surroundings (Pabsorbed=eσAT04P_{\text{absorbed}} = e \sigma A T_0^4) decreases, thereby increasing the net rate of heat loss. To maintain a constant body temperature, the human body needs to generate (produce via metabolism) extra energy per unit time, rather than radiate more energy.

Therefore, Option [B] is incorrect.


3. Analysis of Option [C]

The net rate of heat loss by thermal radiation is given by: Pnet=eσA(T4−T04)P_{\text{net}} = e \sigma A (T^4 - T_0^4)

Since PnetP_{\text{net}} is directly proportional to the exposed surface area AA, reducing the effective surface area exposed to the environment (for example, by curling up into a ball) directly reduces PnetP_{\text{net}}. This allows humans to conserve body heat and maintain temperature while minimizing radiative energy loss.

Therefore, Option [C] is correct.


4. Analysis of Option [D]

According to Wien's Displacement Law, the peak wavelength λmax\lambda_{\text{max}} of the emitted radiation spectrum is inversely proportional to the absolute temperature TT: λmaxT=b  ⟹  λmax=bT\lambda_{\text{max}} T = b \implies \lambda_{\text{max}} = \frac{b}{T}

If the body temperature TT increases significantly, λmax\lambda_{\text{max}} decreases, which means the peak of the spectrum shifts to shorter wavelengths (higher frequencies), not longer wavelengths.

Therefore, Option [D] is incorrect.


Conclusion

The correct option is [C].