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• DEPARTEMENT: C/PHARMACY
• YEAR: 3rd SEM: II
• ASSIGNMENT OF PHARMACEUTICAL
ANALYSIS-II
Submitted to Mona
Quadrupole Analyzer
 four parallel metal rods
 an ion source,
 ion optics ,
 the quadrupole filter itself with control voltage supplies,
 an exit aperture,
 an ion detector,
 detection electronics,
 and a high-vacuum system.
 (U+Vcos(wt)) = the potential of two opposite rods
 - (U+Vcos(wt)) =the potential of other rods
 U = a dc voltage and Vcos(wt) =an ac voltage
 ions travel down the flight path which is centered between the
four rods, and because of the applied voltages the trajectory
of ions is affected.
 This filter is selective of ions depending on their certain m/z
and Vac/Vdc ratios:some of them pass and the others are
thrown out.
 Voltages on the rod vary and mass spectrum is obtained
 There are two methods: varying w and holding U and V constant, or
varying U and V (U/V) fixed for a constant w.
Ion Trap Analyzer
 Ions are trapped by applying rf
frequencies on the ring electrode
and endcaps
 Then ions are scanned out of the
trap by m/z as the base mass
voltage is increased over time
 This is accomplished by
maintaining in the trap a
pressure of helium gas which
removes excess energy from the
ions by collision.
 DISADVANTAGES:
-Mass measurement accuracy is relatively poor
◗ ADVANTAGES:
- MS/MS/MS…..
- High sensitivity full scan MS/MS
- Compactness
• The Back Plate and Grid are used to accelerate the ions
• The Ion source is used to ionize the Sample
• The Sample Inlet introduces the sample to the source
• The vacuum is used to maintain a low pressure
• The Drift Region separates the ions according to their
mass
• The Detector outputs current as each ion strikes it
• The Oscilloscope displays the detector output
Time-of-Flight Analyzer
ADVANTAGES:
• Unlimited mass range
• Ideal for Pulsed ionization or spatially confined
• For each ionization complete mass spectrum
• High transmission
• Valid for extremely small sample amounts
• Relatively low cost
• Fast mass scanning
DISADVANTAGES:
 The pulse is not felt by all ions to the same intensity and so a kinetic energy
distribution for each discrete m/z exists. This lowers the resolution by creating a
time-of-flight distribution for each m/z

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g.pptx

  • 1. • DEPARTEMENT: C/PHARMACY • YEAR: 3rd SEM: II • ASSIGNMENT OF PHARMACEUTICAL ANALYSIS-II Submitted to Mona
  • 2. Quadrupole Analyzer  four parallel metal rods  an ion source,  ion optics ,  the quadrupole filter itself with control voltage supplies,  an exit aperture,  an ion detector,  detection electronics,  and a high-vacuum system.  (U+Vcos(wt)) = the potential of two opposite rods  - (U+Vcos(wt)) =the potential of other rods  U = a dc voltage and Vcos(wt) =an ac voltage  ions travel down the flight path which is centered between the four rods, and because of the applied voltages the trajectory of ions is affected.  This filter is selective of ions depending on their certain m/z and Vac/Vdc ratios:some of them pass and the others are thrown out.  Voltages on the rod vary and mass spectrum is obtained  There are two methods: varying w and holding U and V constant, or varying U and V (U/V) fixed for a constant w.
  • 3. Ion Trap Analyzer  Ions are trapped by applying rf frequencies on the ring electrode and endcaps  Then ions are scanned out of the trap by m/z as the base mass voltage is increased over time  This is accomplished by maintaining in the trap a pressure of helium gas which removes excess energy from the ions by collision.  DISADVANTAGES: -Mass measurement accuracy is relatively poor ◗ ADVANTAGES: - MS/MS/MS….. - High sensitivity full scan MS/MS - Compactness
  • 4. • The Back Plate and Grid are used to accelerate the ions • The Ion source is used to ionize the Sample • The Sample Inlet introduces the sample to the source • The vacuum is used to maintain a low pressure • The Drift Region separates the ions according to their mass • The Detector outputs current as each ion strikes it • The Oscilloscope displays the detector output Time-of-Flight Analyzer ADVANTAGES: • Unlimited mass range • Ideal for Pulsed ionization or spatially confined • For each ionization complete mass spectrum • High transmission • Valid for extremely small sample amounts • Relatively low cost • Fast mass scanning DISADVANTAGES:  The pulse is not felt by all ions to the same intensity and so a kinetic energy distribution for each discrete m/z exists. This lowers the resolution by creating a time-of-flight distribution for each m/z