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Empirical equations for inter-conversion . . .

Abstract
1. Introduction

2. Methods
2.1.1 Land-based TSR and PAR in air
2.1.2 Solar elevation angles
2.1.3 Equations for computing cloudiness
2.1.4 Conversion between TSR and PAR
2.2.1 Air-water interface measurements in distilled water
2.2.2 Air-water interface measurements in Tampa Bay
2.2.3 Effects of waves on PAR transmission through the air-water interface
2.3.1 PAR irradiance and attenuation measurements in water of Tampa Bay
2.3.2 Laboratory measurements of attenuation of water samples
2.3.3 Estimation of the ratio of 4
p to 2p PAR just below the air-water interface
2.3.4 Prediction of PAR in water from land-based PAR
3. Results

3.1 Maximum TSR and PAR from solar elevation angles
3.2 Conversions between types of solar radiation in air
3.3 Transfer of radiation across the air-water interface
3.3.1 Controlled measurements of refraction in distilled water.
3.3.2 In-water extrapolation of 2
p PAR to just below the air-water interface.
3.3.3 Controlled measurements of effects of waves on 2
p PAR transmission through the air-water interface.
3.4 Conversion of 2
p and 4p PAR just below the air-water interface.
3.5 Attenuation coefficients
3.5.1 Choosing attenuation coefficients for water.
3.5.2 Comparison of diffuse and scalar PAR attenuation coefficients measured simultaneously.
3.6 Modeled results using land-based PAR to predict PAR in water.
4. Discussion

Acknowledgements

References

Abstract

Empirical equations were developed for converting between total solar radiation and photosynthetically active radiation (PAR) and between 2p and 4p sensor geometries allowing one type of solar radiation data to be computed from another type. In situ and laboratory tests indicate that 2p PAR in air is a good estimator of 2p PAR in water just below a calm or rough water surface. Just below the water surface, 4p PAR was 1.29 times the 2p PAR. Land-based 2p PAR data (5-minute averages) were multiplied by 1.29 to convert to 4p PAR in water and observed attenuation coefficients were used to predict PAR at 3 depths. The predicted PAR values were compared to 10-second averages of 4p PAR measured in water. Using these concepts and land-based data from Tampa, 2p and 4p PAR just below the water surface of Tampa Bay is estimated at 1.1×1010 and 1.4×1010 micromoles of photons per square meter per year, respectively. Attenuation was measured simultaneously by 3 in situ methods and also by 2 laboratory methods.