Membrane inlets Mass spectrometry selleck products operates under high vacuum conditions. The vacuum is essential to prevent inter molecular collision of

analyte ions with atmospheric gas molecules which would otherwise defocus ion trajectories. An important technical issue of mass spectrometry is how the sample (solid/liquid/gaseous) is introduced into the high vacuum space. An elegant solution to detect processes online in liquid or gaseous samples is to separate the liquid or gaseous phase from the high vacuum space by a gas permeable membrane. This technique named membrane-inlet mass spectrometry (MIMS) was developed by Georg Hoch and OICR-9429 cost Bessel Kok in 1963 (Hoch and Kok 1963) and is schematically shown Selleckchem Target Selective Inhibitor Library in Fig. 1. General design features of MIMS cuvettes exemplifying the basic considerations of liquid versus gas phase sampling are displayed in Fig. 2. Fig. 1 Pictorial representation of a MIMS set-up demonstrating the gas sampling interface onto a magnetic sector mass spectrometer (i.e., Thermo Finnigan Delta or Isoprime IRMS series). Gases from photosynthesis traverse a membrane into high vacuum and are ionized by electron impact. The ions that are produced are then drawn into a flight tube and are dispersed by a magnetic field into a 7-cup

Faraday detector array for detection Fig. 2 Membrane-inlet sampling is achieved via different cuvette designs that have a semi-permeable membrane at the high vacuum interface. To avoid boundary layers in liquid phase measurements a magnetic stirrer is placed directly on the membrane. Above the membrane small volume liquid or gas phase cavities are provided so that economical isotopic enrichments can be performed. For photosynthetic studies of leaves (a) sealed cuvettes with volumes ~1 ml are used with a window for illumination, Fossariinae whereas

solutions measurements (b) can employ sample chambers with considerably smaller volumes. The cuvette design incorporates injection ports and thermal regulation via water cooling The key component of MIMS is a membrane that is typically 10–100 μm thick and can be a few cm2 in size. To prevent collapse it requires support from a porous supporting material that does not impose a significant diffusion barrier. Porous plastic sheeting or thin metal supports with fine holes can provide this function. To prevent water vapor entering the mass spectrometer, particularly as result of a membrane puncture, a cryogenic trap is installed between membrane and ion source. In addition to trapping water vapor the trap can be used to differentially remove other organics or gasses by choosing the trap temperature. The trap may be filled for example with dry ice/ethanol (~200 K) or liquid nitrogen (77 K). Membrane properties As mentioned above, in MIMS a semi-permeable membrane functions as analyte inlet system into the high vacuum of the mass spectrometer.