Uploaded by Ankush Singh

Passive Radiative Daytime Cooling

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Passive Radiative
Daytime Cooling
BY –
ANKUSH KUMAR SINGH
Introduction

Passive radiative cooling can be considered as a renewable energy
source, which can pump heat to cold space and make the devices
more efficient than ejecting heat at earth atmospheric
temperature. Passive radiative cooling is a method of cooling
objects with radiation energy exchange with cold outer space,
which is at 3K. To exchange radiative heat with cold outer space,
radiative cooler is required to emit radiation in atmospheric window
8–13 μm and reflect elsewhere, i.e., solar radiation and atmospheric
radiation.
Energy Exchange

The ideal radiative cooler decoupled from the atmosphere can achieve
equilibrium temperature of outer space, i.e., 3K, but the actual theoretically
limit by considering atmospheric radiation and suppressing parasitic heat
gain attain an average 37 ᵒC below ambient in. The more actual scenarios
have humidity and cloud in the environment and need consideration.
Solar reflectance and LWIR emittance

In the solar spectrum (0.3–2.5 μm), the absorptance should be 0 (100%
reflectance) to avoid solar heating.

In the atmospheric LWIR transmission window (8–13 μm), the emittance should be
1 to effectively radiate heat to outer space through this partially transparent
atmospherewindow.

In other mid-infrared wavelengths (2.5–8 μmand > 13 μm), the emittance should be
0 to avoid the overheating of the atmospheric irradiation at a higher temperature
than that of the PDRC coating.
Reflectance

A mismatch between the refractive index causes scattering of light
in material and backscatters for the slab thickness.

Any change in refractive index leads to some reflection and this
concept can be utilized for maximum reflection of varying refractive
index alternatively in dielectric stack multiple layers.

Other than layered media, randomly distributed particles scatter the
light and lead to diffuse reflection or backscattering.
Non-Radiative heat transfer
Fabrication of PDRC materials
Thermal mid-infrared emittance

To achieve better PDRC performance in sub-ambient conditions,
diverse materials have been proposed to improve the mid-infrared
emittance where λ =8–13 μm.

Inorganic dielectric materials can achieve spectrally selective
infrared emittance because of the wide absorption band of metalO bonds.37,48 In addition, Al2O3, TiO2, and SiO2 are stable and
chemically inert materials, and inorganic coatings inherently exhibit
superior mechanical robustness and retainability, thereby
guaranteeing a long lifespan in exterior environments.

Inorganic PDRC has lack of flexibility,water-repellence, and antiabrasion.
Effect of environmental parameters

The high humidity or cloud cover blocks the atmospheric window in
8–13 μm range due to the presence of water vapor, which
absorbs/emits in the specified atmospheric window, leads to
radiative cooler nearly ineffective.

Convective effects - The effect of wind over a radiative cooler can
be suppressed by a wind-shield and depends directly on change in
wind velocity for daytime and nighttime radiative cooling.
Applications

Space Cooling

Water Cooling

Harvesting Water from atmosphere

Electricity Generation
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