[Detonation temperature measurement of epoxypropane using instantaneous spectrum method]
Ying Li1, Ping Li, Hai-Bo Xiao
1Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China.
Guang Pu Xue Yu Guang Pu Fen Xi = Guang Pu
|June 10, 2008
Summary
Researchers measured the detonation temperature of epoxypropane at 2,416 K. This provides crucial experimental data for understanding the deflagration to detonation transition (DDT) process in fuels.
Area of Science:
- Chemical Engineering
- Combustion Science
- Spectroscopy
Context:
- Investigating the deflagration to detonation transition (DDT) in epoxypropane.
- Addressing challenges in synchronizing measurement systems and preventing false triggers during high-speed events.
Purpose:
- To acquire the instantaneous emission spectrum of epoxypropane during the DDT phase.
- To determine the detonation temperature of epoxypropane through spectral analysis.
Summary:
- An advanced spectroscopic system, including an intensified charge-coupled-device detector and a digital delay generator, was employed to capture the emission spectrum of epoxypropane.
- The system successfully synchronized measurements and avoided false triggers, enabling the acquisition of spectra at 2 microseconds exposure and 0.2 nm resolution.
- Pressure transducers monitored the DDT process, and spectral data, after intensity correction, were fitted to Planck's blackbody formula to derive a detonation temperature of 2,416 K.
Impact:
- Provides the first experimental detonation temperature for epoxypropane.
- Offers critical data for validating computational models of combustion and detonation phenomena.
- Contributes to a deeper understanding of the microscopic mechanisms governing the DDT process in energetic materials.
Related Concept Videos
Flame Photometry: Overview
Flame photometry, also known as flame emission spectrometry, is a technique used for the qualitative and quantitative analysis of elements present in a sample using a flame as the source of excitation energy. The concept of flame photometry was realized in the early 1860s by Kirchhoff and Bunsen, who discovered that specific elements emit characteristic radiation when excited in flames. The first instrument developed for this purpose was used to measure sodium (Na) in plant ash using a Bunsen...
Flame Photometry: Lab
In a flame photometer, when a solution like potassium chloride is aspirated into the flame, the solvent evaporates, leaving behind dehydrated salt. This salt dissociates into free gaseous atoms in their ground state. Some of these atoms absorb energy from the flame, leading to their excitation. The excited atoms return to the ground state, emitting photons at characteristic wavelengths. Because only electronic transitions are involved, the resulting emission lines are very narrow. The intensity...
Atomic Emission Spectroscopy: Instrumentation
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
Atomic Emission Spectroscopy: Lab
AES is a powerful analytical technique, especially effective when used with plasma sources, producing abundant spectra in characteristic emission lines. The Inductively Coupled Plasma (ICP), in particular, yields superior quantitative analytical data due to its high stability, low noise, low background, and minimal interferences under optimal experimental conditions. However, newer air-operated microwave sources are emerging as promising alternatives that could be more cost-effective than...
Atomic Spectroscopy: Effects of Temperature
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature from...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature from...
Atomic Emission Spectroscopy: Overview
Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...

