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Schedule 08/31/17 (Lecture #1) Schedule 08/31/17 (Lecture #1)

Schedule 08/31/17 (Lecture #1) - PowerPoint Presentation

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Uploaded On 2018-10-28

Schedule 08/31/17 (Lecture #1) - PPT Presentation

090517 Lecture 2 090717 Lecture 3 091217 400 1830 h Lecture 45 091417 Lecture 6 radiation 092117 Lecture 7 radiation lab amp New EC tower 092617 400 1830 h Lecture 89 ID: 699897

radiation lecture surface amp lecture radiation amp surface radiometer angle long wave lab sensor net view object short flat

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Slide1

Schedule

08/31/17 (Lecture #1)09/05/17 (Lecture #2)09/07/17 (Lecture #3)09/12/17 (4:00 – 18:30 h) (Lecture #4-5)09/14/17 (Lecture #6): radiation09/21/17 (Lecture #7): radiation lab & New EC tower09/26/17 (4:00 – 18:30 h) (Lecture #8-9)09/28/17 (Lecture #10)10/03/17 (12:00 – 8:00 h) (Lab #1)10/10/17 (12:00 – 8:00 h) (Lab #2)10/20/17 (8:00 -17:00 h) (Lab #3)10/24/17 (Q&A #1) 10/26/17 (Lecture #11)11/07/17 (Q&A #2)11/14/17 (Q&A #3)11/21/17 (Q&A #4)12/07/17 (Lecture #12): Term paper due on Dec. 14, 2017

12 lectures3 long labs (8 hours each)2 homework1 group project4 Q&A (Geography Room 206)Dr. Dave Reed on CRBasics with CR5000 dataloggerSlide2

Spectral distribution of blackbody radiationm = 2897 • T-1Slide3

Beer-Lambert’s LawI = I0 e-k * b

Attenuation of radiation in a homogeneous mediumApplies for wavebands narrow enough where k remains constant. Hemispherical photos and applications: A “standard” method to characterize light environments beneath forest canopiesDemo of the solar.c model by Chen 1990.Slide4

Diel change of short-wave radiation in and under forest canopies (Chen et al. 1999)Slide5

Greenhouse EffectSlide6

Long waveSlide7

http://www.epa.gov/climatechange/emissions/usinventoryreport.htmlSlide8
Slide9

RadiometersPyranometer: Global shortwave radiationPyrheliometer: direct beam of solar radiationPyrgeometer: measurement of longwave radiationNet radiometer: difference between incoming and outgoing radiationDiffuse radiation: pyranometer

and shadow bandsHemispherical photos: Slide10

The geometrical arrangement of a radiometer above a flat, horizontal surface. Refer to the text for definitions of the geometrical elements.Slide11

View factorsRadiation from one object gets intercepted by anotherView factor = average flux density over the entire surface of the object divided by flux density on a flat absorbing surface facing the source. For beam radiation this is numerically equal to the ratio of projected area (in the direction of the source of the radiation) to total surface areaThe sum of view factors of an object to its surrounding environment is 1For canopy, Fr = Fg

= 0; Fa = Fd = (1+cosg)/2; Fe = 1For leaf, Fp = 0.5 cosq; Fa = Fd = Fr = Fg = 0.5; Fe = 1 q = f{zenith angle; azimuth angle; aspect angle; inclination angle}Slide12

View factorsSlide13

The CNR1 net radiometer is manufactured by Kipp& Zonen for applications requiring research-gradeperformance. The radiometer measures the energybalance between incoming short-wave and long-waveinfrared radiation versus surface-reflected short-waveand outgoing long-wave infrared radiation. The CNR1 consists of a pyranometer and pyrgeometerpair that faces upward and a complementary pair thatfaces downward.Slide14

The Q7.1 is an high-output thermopile sensor that generates a millivolt signal proportional to the net radiation level. The sensor is mounted in a glass-reinforced plastic frame with a built-in level. A ball joint is supplied on the stem to facilitate leveling. The sensor surface and surrounding surfaces are painted flat black to reduce reflections within the instrument and to achieve uniform performance over reflective and non-reflective surfaces.Slide15
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Slide17
Slide18

Programming with radiometersLI190SB: PARQ7.1: net radiometerCNR 4: 4-way radiometerTasks and Assignment fir the EC tower on Baker HallOverall Design: BJLogistics: GabrielaProgramming: Cheyenne

Testing & Mounting: Chase