In this work, a detailed calibration study is performed to establish non-intrusive one-dimensional (1D) rovibrational temperature measurements in unseeded air, based on air resonance enhanced multiphoton ionization thermometry (ART). ART is generated by REMPI (resonance enhanced multi-photon ionization) of molecular oxygen and subsequent avalanche ionization of molecular nitrogen in a single laser pulse. ART signal, the fluorescence from the first negative band of molecular nitrogen, is directly proportional to the 2-photon transition of molecular oxygen C3Π (v = 2) ← X3Σ (v’=0), which is used to determine temperature. Experimentally, hyperfine structures of the O2rotational branches with high temperature sensitivity are selectively excited through a frequency-doubled dye laser. Electron-avalanche ionization of N2results in the fluorescence emissions from the first negative bands of N2+near 390, 425, and 430nm, which are captured as a 1D line by a gated intensified camera. Post processing of the N2+fluorescence yields a 1D thermometry line that is representative of the air temperature. It is demonstrated that the technique provides ART fluorescence of ∼5cm in length in the unseeded air, presenting an attractive thermometry solution for high-speed wind tunnels and other ground test facilities.
This paper presents an extensive parameter study of a non-intrusive and non-seeded laser diagnostic method for measuring one dimensional (1D) rotational temperature of molecular nitrogen (N2) at 165 - 450 K. Compared to previous efforts using molecular oxygen, here resonantly ionized and photoelectron induced fluorescence of molecular nitrogen for thermometry (N2RIPT) was demonstrated. The RIPT signal is generated by directly probing various rotational levels within the rovibrational absorption band of N2, corresponding to the 3-photon transition of N2(
- Award ID(s):
- 2026242
- PAR ID:
- 10470001
- Publisher / Repository:
- Optical Society of America
- Date Published:
- Journal Name:
- Optics Continuum
- Volume:
- 2
- Issue:
- 11
- ISSN:
- 2770-0208
- Format(s):
- Medium: X Size: Article No. 2255
- Size(s):
- Article No. 2255
- Sponsoring Org:
- National Science Foundation
More Like this
-
-
Characterization of the thermal gradients within supersonic and hypersonic flows is essential for understanding transition, turbulence, and aerodynamic heating. Developments in novel, impactful non-intrusive techniques are key for enabling flow characterizations of sufficient detail that provide experimental validation datasets for computational simulations. In this work, Resonantly Ionized Photoemission Thermometry (RIPT) signals are directly imaged using an ICCD camera to realize the techniques 1D measurement capability for the first time. The direct imaging scheme presented for oxygen-based RIPT (O2RIPT) uses the previously established calibration data to direct excite various resonant rotational peaks within the S-branch of the
C 3Π, (v = 2) ←X 3Σ(v ′ = 0) absorption band of O2. The efficient ionization of O2liberates electrons that induce electron avalanche ionization of local N2molecules generating N2+, which primarily deexcites via photoemissions of the first negative band of. When sufficient lasing energy is used, the ionization region and subsequent photoemission signal is achieved along a 1D line thus, if directly imaged can allow for gas temperature assignments along said line; demonstrated here of up to five centimeters in length. The temperature gradients present within the ensuing shock train of a supersonic under expanded free jet serves as a basis of characterization for this new RIPT imaging scheme. The O2RIPT results are extensively compared and validated against well-known and established techniques (i.e., CARS and CFD). The direct imaging capability fully realizes the technique’s fundamental potential and is expected to be the standard of implementation going forward. The direct imaging capability can play instrumental roles in future scientific studies that rely upon acute characterization of thermal gradients within a medium that cannot be easily resolved by a point. Furthermore, the removal of the spectrometer greatly reduces the cost, complexity, and optical alignment associated with prior RIPT measurements. -
Abstract Potential energy surface (PES) analyses at the SMD[MP2/6–311++G(d,p)] level and higher‐level energies up to MP4(fc,SDTQ) are reported for the fluorinated tertiary carbamate
N ‐ethyl‐N ‐(2,2,2‐trifluoroethyl) methyl carbamate (VII ) and its parent systemN ,N ‐dimethyl methyl carbamate (VI ). Emphasis is placed on the analysis of the rotational barrier about the CN carbamate bond and its interplay with the hybridization of theN ‐lone pair (NLP). All rotational transition state (TS) structures were found by computation of 1D relaxed rotational profiles but only 2D PES scans revealed the rotation‐inversion paths in a compelling fashion. We found four unique chiral minima ofVII , one pair each ofE‐ andZ ‐rotamers, and we determined theeight unique rotational TS structures associated with every possibleE /Z ‐isomerization path. It is a significant finding that all TS structures featureN ‐pyramidalization whereas the minima essentially contain sp2‐hybridized nitrogen. We will show that the TS stabilities are affected by the synergetic interplay between NLP/CO2repulsion minimization, NLP→σ*(CO) negative hyperconjugation, and two modes of intramolecular through‐space electrostatic stabilization. We demonstrate how Boltzmann statistics must be applied to determine the predicted experimental rotational barrier based on the energetics of all eight rotamerization pathways. The computed barrier forVII is in complete agreement with the experimentally measured barrier of the very similar fluorinated carbamateN ‐Boc‐N ‐(2,2,2‐trifluoroethyl)‐4‐aminobutan‐1‐olII . NMR properties ofVII were calculated with a variety of density functional/basis set combinations and Boltzmann averaging over theE‐ andZ ‐rotamers at our best theoretical level results in good agreement with experimental chemical shifts δ(13C) andJ (13C,19F) coupling constants ofII (within 6 %). -
Abstract We have observed electron impact fluorescence from CO2to excite the Cameron bands (CBs), CO (
a 3Π →X 1Σ+; 180–280 nm), the first-negative group (1NG) bands, CO+(B 2Σ+→X 2Σ+; 180–320 nm), the fourth-positive group (4PG) bands, CO (A 1Π →X 1Σ+; 111–280 nm), and the UV doublet, CO2+( 288.3 and 289.6 nm) in the ultraviolet (UV). This wavelength range matches the spectral region of past and present spacecraft equipped to observe UV dayglow and aurora emissions from the thermospheres (100–300 km) of Mars and Venus. Our large vacuum system apparatus is able to measure the emission cross sections of the strongest optically forbidden UV transitions found in planetary spectra. Based on our cross-sectional measurements, previous CB emission cross-sectional errors exceed a factor of 3. The UV doublet lifetime is perturbed through spin–orbit coupling. Forward modeling codes of the Mars dayglow have not been accurate in the mid-UV due to systematic errors in these two emission cross sections. We furnish absolute emission cross sections for several band systems over electron energies 20–100 eV for CO2. We present a CB lifetime, which together with emission cross sections, furnish a set of fundamental physical constants for electron transport codes such as AURIC (Atmospheric Ultraviolet Radiance Integrated Code). AURIC and Trans-Mars are used in the analysis of UV spectra from the Martian dayglow and aurora. -
Abstract Cycling LiCoO2to above 4.5 V for higher capacity is enticing; however, hybrid O anion‐ and Co cation‐redox (HACR) at high voltages facilitates intrinsic O
α −(α < 2) migration, causing oxygen loss, phase collapse, and electrolyte decomposition that severely degrade the battery cyclability. Hereby, commercial LiCoO2particles are operando treated with selenium, a well‐known anti‐aging element to capture oxygen‐radicals in the human body, showing an “anti‐aging” effect in high‐voltage battery cycling and successfully stopping the escape of oxygen from LiCoO2even when the cathode is cycled to 4.62 V. Ab initio calculation and soft X‐ray absorption spectroscopy analysis suggest that during deep charging, the precoated Se will initially substitute some mobile Oα −at the charged LiCoO2surface, transplanting the pumped charges from Oα −and reducing it back to O2−to stabilize the oxygen lattice in prolonged cycling. As a result, the material retains 80% and 77% of its capacity after 450 and 550 cycles under 100 mA g−1in 4.57 V pouch full‐cells matched with a graphite anode and an ultralean electrolyte (2 g Ah−1).