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Dive into the research topics where Monali Kawade is active.

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Featured researches published by Monali Kawade.


Journal of Physical Chemistry A | 2011

Dynamics of Cl (2Pj) atom formation in the photodissociation of fumaryl chloride (ClCO - CH = CH - COCl) at 235 nm: a resonance enhanced multiphoton ionization (REMPI) time-of-flight (TOF) study.

Monali Kawade; Ankur Saha; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik; P.N. Bajaj

The photodissociation dynamics of fumaryl chloride (ClCO-CH═CH-COCl) has been studied in a supersonic molecular beam around 235 nm using resonance enhanced multiphoton ionization (REMPI) time-of-flight (TOF) technique by detecting the nascent state of the primary chlorine atom. A single laser has been used for excitation of fumaryl chloride and the REMPI detection of chlorine atoms in their spin-orbit states, Cl ((2)P(3/2)) and Cl* ((2)P(1/2)). We have determined the translational energy distribution, the recoil anisotropy parameter, β, and the spin-orbit branching ratio for chlorine atom elimination channels. To obtain these, measured polarization-dependent and state-specific TOF profiles are converted into kinetic energy distributions, using a least-squares fitting method, taking into account the fragment recoil anisotropies, β(i). The TOF profiles for both Cl and Cl* are found to be independent of laser polarization; i.e., β is well characterized by a value of 0.0, within the experimental uncertainties. Two components, namely, the fast and the slow, are observed in the translational energy distribution, P(E(T)), of Cl and Cl* atoms, and assigned to be formed from different potential energy surfaces. The average translational energies for the fast components of the Cl and Cl* channels are 14.9 ± 1.6 and 16.8 ± 1.6 kcal/mol, respectively. Similarly, for the slow components, the average translational energies of the Cl and Cl* channels are 3.4 ± 0.8 and 3.1 ± 0.8 kcal/mol, respectively. The energy partitioning into the translational modes is interpreted with the help of various models, such as impulsive and statistical models. Apart from the chlorine atom elimination channel, molecular hydrogen chloride (HCl) elimination is also observed in the photodissociation process. The HCl product has been detected, using a REMPI scheme in the region of 236-237 nm. The observation of the molecular HCl in the dissociation process highlights the importance of the relaxation process, in which the initially excited parent molecule relaxes to the ground state from where the molecular (HCl) elimination takes place.


Journal of Physical Chemistry A | 2012

Photodissociation Dynamics of Halogenated Thiophenes at 235 nm: A Resonance Enhanced Multiphoton Ionization-Time-of-Flight (REMPI-TOF) Study

Monali Kawade; Ankur Saha; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik; P.N. Bajaj

The photodissociation dynamics of halogen-substituted thiophenes, namely, 2-chlorothiophene and 2-bromo-5-chlorothiophene, has been studied in a supersonic molecular beam around 235 nm, using resonance enhanced multiphoton ionization (REMPI) time-of-flight (TOF) technique, by detecting the nascent state of the primary halogen atoms. A single laser has been used for excitation of halothiophenes, as well as for the REMPI detection of photoproducts, namely, chlorine and bromine atoms, in their spin-orbit states X((2)P(3/2)) and X*((2)P(1/2)). We have determined the translational energy distribution, the recoil anisotropy parameter, β, and the spin-orbit branching ratio, for chlorine and bromine atom elimination channels. State-specific TOF profiles are converted into kinetic energy distributions, using a least-squares fitting method, taking into account the fragment anisotropies, β(ι). The TOF profiles for Cl, Cl*, Br, and Br* are found to be independent of laser polarization; i.e., the β is well characterized by a value of ~0.0, within the experimental uncertainties. For 2-chlorothiophene, we have observed two components for the Cl and only one component for the Cl* atom elimination channel in the translational energy distributions. The average translational energies for the fast and the slow components of the Cl channel are 3.0 ± 1.0 and 1.0 ± 0.5 kcal/mol, respectively. For Cl*, the average translational energy is 3.5 ± 1.0 kcal/mol. For 2-bromo-5-chlorothiophene, we have observed only one component for Cl, Cl*, Br, and Br* in the translational energy distributions. The average translational energies for the Cl and Cl* channels are 3.5 ± 1.0 and 5.0 ± 1.0 kcal/mol, respectively, whereas the average translational energies for the Br and Br* channels are 2.0 ± 1.0 and 3.5 ± 1.0 kcal/mol, respectively. The energy partitioning into the translational modes is interpreted with the help of various models, such as impulsive and statistical models. The ΔH(f)(298) value for 2-chlorothiophene has been estimated theoretically to be 23.5 kcal/mol.


Journal of Physical Chemistry A | 2014

Photodissociation dynamics of benzoyl chloride at 235 nm: resonance-enhanced multiphoton ionization detection of Cl and HCl.

Ankur Saha; Monali Kawade; Sumana SenGupta; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik

The photodissociation dynamics of benzoyl chloride at 235 nm has been investigated and compared with that of 2-furoyl chloride. Atomic Cl and molecular HCl channels have been detected in benzoyl chloride by employing resonance-enhanced multiphoton ionization technique and time-of-flight mass spectrometry. Both the Cl fragments, Cl((2)PJ=3/2, relative quantum yield 0.70 ± 0.15) and Cl*((2)PJ=1/2), show isotropic angular distribution and bimodal translational energy distributions. The predominant high kinetic energy channel contributes 72% to the C-Cl bond scission and arises from the S1 state having nπ* character of benzoyl chloride. However, the low-energy Cl and HCl channels originate from the ground electronic state. The most plausible mechanism of HCl formation is proposed based on molecular orbital calculations. In contrast to benzoyl chloride, the HCl channel is not observed in 2-furoyl chloride on excitation at 235 nm, and this is attributed to an energy constraint.


Journal of Chemical Physics | 2011

Laser-induced UV photodissociation of 2-bromo-2-nitropropane: Dynamics of OH and Br formation

Ankur Saha; Monali Kawade; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik


Journal of Physical Chemistry A | 2013

Photodissociation dynamics of enolic 1,2-cyclohexanedione at 266, 248, and 193 nm: mechanism and nascent state product distribution of OH.

Monali Kawade; Ankur Saha; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik


Chemical Physics | 2013

Photoexcitation of 2-bromo-2-chloro-1,1,1-trifluoroethane (halothane) to repulsive surface nσ∗(C–Br) at 234 nm: Dynamics of C–Br and C–Cl bond rupture

Ankur Saha; Monali Kawade; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik


Chemical Physics Letters | 2017

Kinetics of gas phase OH radical reaction with thiophene in the 272–353 K temperature range: A laser induced fluorescence study

Monali Kawade; D. Srinivas; Hari P. Upadhyaya


Chemical Physics | 2012

Resonance enhanced multiphoton ionization time-of-flight (REMPI-TOF) study of phosphorous oxychloride (POCl3) dissociation at 235 nm: Dynamics of Cl(2Pj) formation

Ankur Saha; Monali Kawade; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik; P.N. Bajaj


Journal of Physical Chemistry A | 2010

Dynamics of N-OH bond dissociation in cyclopentanone and cyclohexanone oxime at 193 nm: laser-induced fluorescence detection of nascent OH (v'', J'').

Monali Kawade; Ankur Saha; Hari P. Upadhyaya; Awadhesh Kumar; Prakash D. Naik


ChemistrySelect | 2018

Gas Phase OH Radical Reaction with 2-Chloroethyl Vinyl Ether in the 256-333 K Temperature Range: A Combined LP-LIF and Computational Study

Monali Kawade; Doddipatla Srinivas; Hari P. Upadhyaya

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Hari P. Upadhyaya

Bhabha Atomic Research Centre

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Ankur Saha

Bhabha Atomic Research Centre

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Awadhesh Kumar

Bhabha Atomic Research Centre

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Prakash D. Naik

Bhabha Atomic Research Centre

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P.N. Bajaj

Bhabha Atomic Research Centre

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D. Srinivas

Bhabha Atomic Research Centre

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A. Sharma

Bhabha Atomic Research Centre

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Sumana SenGupta

Bhabha Atomic Research Centre

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