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Zhang Z, Yang A, Wang J, Sun Z, Lv J, Zhang G, Zhang X, Li X, Liu Y, Cheng G. OH planar laser-induced fluorescence imaging system using a kilohertz-rate 283 nm UV Ti:sapphire laser. APPLIED OPTICS 2023; 62:1915-1920. [PMID: 37133074 DOI: 10.1364/ao.484749] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/04/2023]
Abstract
A narrow linewidth Ti:sapphire laser is developed and characterized for the generation of an ultraviolet nanosecond laser pulses for the planar laser-induced fluorescence (PLIF) imaging of hydroxyl (OH). With a pump power of 11.4 W at 1 kHz, the Ti:sapphire laser produces 3.5 mJ at 849 nm with pulse duration of 17 ns and achieves a conversion efficiency of 28.2%. Accordingly, its third-harmonic generation outputs 0.56 mJ at 283 nm in BBO with type I phase match. An OH PLIF imaging system has been built; a 1 to 4 kHz fluorescent image of OH of a propane Bunsen burner has been captured based on this laser system.
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Zhang W, Dong X, Sun Z, Zhou B, Wang Z, Richter M. 100 kHz CH 2O imaging realized by lower speed planar laser-induced fluorescence and deep learning. OPTICS EXPRESS 2021; 29:30857-30877. [PMID: 34614804 DOI: 10.1364/oe.433785] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/10/2021] [Accepted: 08/20/2021] [Indexed: 06/13/2023]
Abstract
This paper reports an approach to interpolate planar laser-induced fluorescence (PLIF) images of CH2O between consecutive experimental data by means of computational imaging realized with convolutional neural network (CNN). Such a deep learning based method can achieve higher temporal resolution for 2D visualization of intermediate species in combustion based on high-speed experimental images. The capability of the model was tested for generating 100 kHz PLIF images by interpolating single and multiple PLIF frames into the sequences of experimental images of lower frequencies (50, 33, 25 and 20 kHz). Results show that the prediction indices, including intersection over union (IoU), peak signal to noise ratio (PSNR), structural similarity index (SSIM), and time averaged correlation coefficient at various axial positions could achieve acceptable accuracy. This work sheds light on the utilization of CNN-based models to achieve optical flow computation and image sequence interpolation, also providing an efficient off-line model as an alternative pathway to overcome the experimental challenges of the state-of-the-art ultra-high speed PLIF techniques, e.g., to further increase repetition rate and save data transfer time.
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Lauriola DK, Rahman KA, Stauffer HU, Slipchenko MN, Meyer TR, Roy S. Concentration and pressure scaling of CH 2O electronic-resonance-enhanced coherent anti-Stokes Raman scattering signals. APPLIED OPTICS 2021; 60:1051-1058. [PMID: 33690411 DOI: 10.1364/ao.415496] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/20/2020] [Accepted: 12/30/2020] [Indexed: 06/12/2023]
Abstract
Nanosecond electronic-resonance-enhanced coherent anti-Stokes Raman scattering (ERE-CARS) is evaluated for the measurement of formaldehyde (CH2O) concentrations in reacting and nonreacting conditions. The three-color scheme utilizes a 532 nm pump beam and a scanned Stokes beam near 624 nm for Raman excitation of the C-H symmetric stretch (ν1) vibrational mode; further, a 342 nm resonant probe is tuned to produce the outgoing CARS signal via the 101403 vibronic transition between the ground (X~1A1) and first excited (A~1A2) electronic states. This allows detection of CH2O at concentrations as low as 9×1014molecules/cm3 (55 parts per million) in a calibration cell with CH2O and N2 at 1 bar and 450 K with 3% uncertainty. The measurements show a quadratic dependence of the signal with CH2O number density. Pressure scaling experiments up to 11 bar in the calibration cell show an increase in signal up to 8 bar. We study pressure dependence up to 11 bar and further apply the technique to characterize the CH2O concentration in an atmospheric premixed dimethyl ether/air McKenna burner flame, with a maximum concentration uncertainty of 11%. This approach demonstrates the feasibility for spatially resolved measurements of minor species such as CH2O in reactive environments and shows promise for application in high-pressure combustors.
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Mishra YN, Boggavarapu P, Chorey D, Zigan L, Will S, Deshmukh D, Rayavarapu R. Application of FRAME for Simultaneous LIF and LII Imaging in Sooting Flames Using a Single Camera. SENSORS (BASEL, SWITZERLAND) 2020; 20:s20195534. [PMID: 32992557 PMCID: PMC7582434 DOI: 10.3390/s20195534] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 08/19/2020] [Revised: 09/19/2020] [Accepted: 09/24/2020] [Indexed: 06/11/2023]
Abstract
In this article, the application of the FRAME (Frequency Recognition Algorithm for Multiple Exposures) technique is presented for multi-species measurements in symmetric and asymmetric ethylene/air diffusion flames. Laminar Bunsen-type and swirled diffusion flames are investigated to gain a better understanding of sooting combustion. For this purpose, simultaneous imaging is conducted in terms of Laser-Induced Fluorescence (LIF) of Polycyclic Aromatic Hydrocarbons (PAH) and Laser-Induced Incandescence (LII) of soot particles. Subsequently, the approach is utilized for simultaneous imaging of hydroxyl (OH)-LIF and soot-LII. Here, the modulated LIF- and LII-signals are acquired together as a single sub-image-with a single exposure utilizing the full sensor size of a single camera. By employing the frequency-recognition algorithm on the single image, the LIF- and LII-signals are spectrally isolated-generating two individual LIF- and LII-images. The flame luminosity and out-of-focus light such as reflected surrounding laser light are detected as non-modulated signals in the unprocessed image. These unwanted signals are suppressed using the image post-processing, and, therefore, the image contrast of the two resulting images is improved. It is found that PAHs mainly exist in the inner region near the burner and are surrounded by soot. The majority of the OH is distributed on the outer edges of the flame-representing the reaction zone and soot-oxidation region of the flame.
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Affiliation(s)
- Yogeshwar Nath Mishra
- Institute of Engineering Thermodynamics, Friedrich-Alexander University (FAU), 91058 Erlangen, Germany; (L.Z.); (S.W.)
- Discipline of Mechanical Engineering, Indian Institute of Technology, Indore 453552, India; (D.C.); (D.D.)
- NASA-Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA 91109, USA
| | - Prasad Boggavarapu
- Department of Mechanical Engineering, Indian Institute of Science, Bangalore 560012, India; (P.B.); (R.R.)
| | - Devashish Chorey
- Discipline of Mechanical Engineering, Indian Institute of Technology, Indore 453552, India; (D.C.); (D.D.)
| | - Lars Zigan
- Institute of Engineering Thermodynamics, Friedrich-Alexander University (FAU), 91058 Erlangen, Germany; (L.Z.); (S.W.)
- Erlangen Graduate School in Advanced Optical Technologies, FAU, 91054 Erlangen, Germany
| | - Stefan Will
- Institute of Engineering Thermodynamics, Friedrich-Alexander University (FAU), 91058 Erlangen, Germany; (L.Z.); (S.W.)
- Erlangen Graduate School in Advanced Optical Technologies, FAU, 91054 Erlangen, Germany
| | - Devendra Deshmukh
- Discipline of Mechanical Engineering, Indian Institute of Technology, Indore 453552, India; (D.C.); (D.D.)
| | - Ravikrishna Rayavarapu
- Department of Mechanical Engineering, Indian Institute of Science, Bangalore 560012, India; (P.B.); (R.R.)
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Gao Y, Yang X, Fu C, Yang Y, Li Z, Zhang H, Qi F. 10 kHz simultaneous PIV/PLIF study of the diffusion flame response to periodic acoustic forcing. APPLIED OPTICS 2019; 58:C112-C120. [PMID: 31045081 DOI: 10.1364/ao.58.00c112] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/26/2018] [Accepted: 03/19/2019] [Indexed: 06/09/2023]
Abstract
Response of a laminar diffusion dimethyl-ether flame forced by an acoustic field is provided. A forcing frequency of 100 Hz, which is chosen based on the typical thermo-acoustic instability frequency in a practical combustor, is applied to the flame at a Reynolds number of 250. The development of the forced vortical structures present in this flame has been investigated utilizing a burst mode laser with a repetition rate of 10 kHz. Flame/vortex interaction is visualized by planar laser-induced fluorescence (PLIF) of formaldehyde, which is used to identify the early-stage fuel decomposition in the flame. The flame structure is also correlated with the velocity field, which is obtained utilizing particle imaging velocimetry (PIV). The resulting phase-resolved and time-averaged velocity and vortex images indicate that the amplitude of excitation has pronounced effects on the flame via modifying the local heat release.
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Wang S, Liu X, Wang G, Xu L, Li L, Liu Y, Huang Z, Qi F. High-repetition-rate burst-mode-laser diagnostics of an unconfined lean premixed swirling flame under external acoustic excitation. APPLIED OPTICS 2019; 58:C68-C78. [PMID: 31045033 DOI: 10.1364/ao.58.000c68] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/19/2018] [Accepted: 01/25/2019] [Indexed: 06/09/2023]
Abstract
Lean premixed swirling flames are important in practical combustors, but a commonly encountered problem of practical swirl combustors is thermo-acoustic instability, which may cause internal structure damage to combustors. In this research, a high-repetition-rate burst-mode laser is used for simultaneous particle image velocimetry and planar laser-induced fluorescence measurement in an unconfined acoustically excited swirl burner. The time-resolved flow field and transient flame response to the acoustic perturbation are visualized at 20 kHz, offering insight into the heat release rate oscillation. The premixed mixture flow rate and acoustic modulation are varied to study the effects of Reynolds number, Strouhal number, and acoustic modulation amplitude on the swirling flame. The results suggest that the Strouhal number has a notable effect on the periodic movements of the inner recirculation zone and swirling flame configuration.
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