Stronger links between researchers who work on Earth’s and other planets’ atmospheres, and between the experimental, modelling and observational communities, will help to interpret the astronomical da...

The Jet Propulsion Laboratory in Pasadena laid off about 550 employees, or 11% of its total staff, on Tuesday.

A message from JPL Director Dave Gallagher

The Air Quality Research Center is excited to announce the 2024 Atmospheric Chemical Mechanisms Conference at the UC Davis Conference Center in December 2024.

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More than 1,000 chemists, biologists and other scientists could be laid off under a plan to dismantle the Office of Research and Development.

The current administration's 2026 budget request includes a staggering 47% cut to NASA's science programs as part of a 25% cut to NASA overall. This is an extinction-level event for the Earth and spac...

OH+NO is an important termolecular association reaction in the troposphere and stratosphere that influences the atmospheric ozone budget. In this study, rate coefficients for the reaction of OH + NO + M → HONO + M were measured under conditions relevant to the troposphere/lower stratosphere over a temperature range of 228–298 K and pressure range of 50–750 Torr using N2 as a bath gas. Time-resolved kinetics were studied by pulsed laser photolysis-laser-induced fluorescence (PLP-LIF) detecting OH by laser-induced fluorescence. Data for the temperature range 258–298 K were fit to two falloff expressions, with the JPL expressions (k1,0N2 = 7.37 × 10–31(T/300 K)−2.90 cm6 molecule–2 s–1 and k1,∞ = 3.44 × 10–11(T/300 K)−0.1cm3 molecule–1 s–1) and IUPAC expression (k1,0N2 = 6.80 × 10–31(T/300 K)−2.81 cm6 molecule–2 s–1, FC = 0.81, k1,∞ = 1.96 × 10–11(T/300 K)−0.3 cm3 molecule–1 s–1). At temperatures T < 258 K, the measured rate coefficients were significantly higher than the IUPAC and JPL fits. To accommodate the rate coefficient deviation from the two expressions, data across the entire temperature range (228–298 K) was fit with two approaches. First, rate coefficients were fit with an empirical modification by adding a second falloff term to the JPL expression with a second low-pressure rate coefficient of k1,0N2 = 5.20 × 10–35(T/300 K)−30.4 cm6 molecule–2 s–1. Second, k1,0N2, k1,∞, and n were fit globally to the entire temperature data set, but FC was varied for each individual temperature, which increased with decreasing temperature. In the second portion of the study, the influence of H2O on the reaction rate was investigated using a N2–H2O mixture as the bath gas at 50 Torr and 273 and 298 K. The JPL and IUPAC falloff expressions were modified to include H2O as a third-body collisional partner consistent with a nonlinear mixture model. Fits to the data yielded the low pressure termolecular rate coefficients in H2O, k1,0H2O = 3.81 × 10–30(T/300 K)−6.04 and k1,0H2O = 3.31 × 10–30(T/300 K)−5.81 cm6 molecule–2 s–1, respectively. Experimental data were fit using MESMER give energy relaxation parameters of <ΔEdown,295 K, N2> = 170 ± 10 cm–1 and <ΔEdown,295 K,H2O> = 634 ± 20 cm–1, indicating that H2O is a 4× more efficient collisional quencher than N2 alone. The modified JPL expressions with the newly derived low pressure rate coefficients were implemented into a STOCHEM-CRI atmospheric model. Predictions of HONO concentrations with the new rates were up to 15% higher in remote tropical regions.

White House aims to end NOAA’s research office; NASA also targeted