Transmission quadrupole mass spectrometer: Difference between revisions
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A [[mass spectrometer]] that consists of four parallel rods whose centers form the corners of a square and whose opposing poles are connected. The voltage applied to the rods is a superposition of a static potential and a sinusoidal radio frequency potential. The motion of an ion in the x and y dimensions is described by the [[Matthieu equation]] whose solutions show that ions in a particular [[m/z]] range can be transmitted along the z axis. | A [[mass spectrometer]] that consists of four parallel rods whose centers form the corners of a square and whose opposing poles are connected. The voltage applied to the rods is a superposition of a static potential and a sinusoidal radio frequency potential. The motion of an ion in the x and y dimensions is described by the [[Matthieu equation]] whose solutions show that ions in a particular [[m/z]] range can be transmitted along the z axis. | ||
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== Related Terms == | |||
[[Paul Ion Trap]] | |||
[[Category:M/z Separation]] | [[Category:M/z Separation]] | ||
Revision as of 23:15, 30 November 2005
| DRAFT DEFINITION |
| Transmission quadrupole mass spectrometer |
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A mass spectrometer that consists of four parallel rods whose centers form the corners of a square and whose opposing poles are connected. The voltage applied to the rods is a superposition of a static potential and a sinusoidal radio frequency potential. The motion of an ion in the x and y dimensions is described by the Matthieu equation whose solutions show that ions in a particular m/z range can be transmitted along the z axis. |
| Considered between 2004 and 2006 but not included in the 2006 PAC submission |
| This is an unofficial draft definition presented for information and comment. |
