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Mass Spectrometry By-Saurav K. Rawat (Rawat DA Greatt)
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Mass spectroscopy

Nov 22, 2014

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Rawat DA Greatt

mass spectroscopy, functions, principle and applicatioins
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Page 1: Mass spectroscopy

Mass Spectrometry

By-Saurav K. Rawat(Rawat DA Greatt)

Page 2: Mass spectroscopy

Mass spectrometry

• A mass spectrometer measures molecular masses.

• The mass unit is called dalton, which is 1/12 of the mass of a carbon atom, and is about the mass of one hydrogen atom.

• If there is a mixture of different molecules in a sample, all the masses are measured simultaneously. So you get a spectrum.

Page 3: Mass spectroscopy

Some PicturesMALDI-R Q-Tof Micro

FT-ICR LTQ-Orbitrap

Page 4: Mass spectroscopy

Each peak corresponds to a different type of molecule in your sample

1000 1200 1400 1600 1800 2000 2200 2400 2600 2800 3000m/z0

100

%

2790.22

1324.60

1265.62

1179.41

2789.22

1325.62

2466.18

2465.20

1759.931326.60

1477.62

1327.611460.59

1748.86

1478.611540.63

1974.94

1760.93

1761.92

1975.93

2356.102355.111976.92

2179.87

2467.19

2468.20

2469.172746.23

2791.23

2792.23

2793.23

3104.412794.20

3103.432795.06 3106.42

...…2789.22 3597.02790.22 5018.02791.23 4406.02792.23 2868.02793.23 1234.0……

peak list

Page 5: Mass spectroscopy

Three Components of an MS• A typical mass spectrometer contains

– Ionizer– Mass analyzer– Detector

• Ion source charges the to-be-measured molecules.– Charge can be negative but often positive.– Two common types: MALDI and ESI.– John B. Fenn & Koichi Tanaka 2002 Nobel Prize in Chemistry

for Electrospray and MALDI

• Mass analyzer separates ions according to the mass to charge ratio (m/z) of the ions.– Iontrap, TOF, Quadrupole, FTICR.

• Detector detects the ions.

Page 6: Mass spectroscopy

Matrix Assisted Laser Desorption/Ionization

Formation of singly charged ions

Sample is co-crystallized with matrix (solid)

Koichi Tanaka, Nobel Prize 2002

Ionization (1): MALDI

Other ionization method exists.

Page 7: Mass spectroscopy

Mass Analyzer (1) – TOF

• Time of Flight.

+ -

+

Detector

Time of flight is proportional to sqrt(m/z)

Other mass analyzer exists.

Page 8: Mass spectroscopy

Drift region (D)

MALDI Time-of-flight

Putting Them Together

MALDI TOF

Average time in TOF: 10-7 sec : average speed 1-2 x 105 km/h

Page 9: Mass spectroscopy
Page 10: Mass spectroscopy
Page 11: Mass spectroscopy

MALDI-TOF Linear

Mass range = 800-200,000

Sensitivity and accuracy decrease rapidly with size !

Page 12: Mass spectroscopy

MALDI-TOF Linear vs Reflectron Mode

Reflectron gives much better resolution for mass < 6,000

• Linear = poor resolution due to velocity variation of ions with the same m/z •Reflectron = Contact lens for a near sighted machine!

Page 13: Mass spectroscopy

Protein “identification” with intact mass

• We measure the intact mass of the protein.• Then search in the protein database to find a

protein with the same mass.• Good idea but there are too many proteins

with the same mass.• In the rest of the lecture we study more

sophisticated methods and why protein ID is important.

Page 14: Mass spectroscopy

Complications

isotopes

widened peaks

profile

Page 15: Mass spectroscopy

Centroiding

Page 16: Mass spectroscopy

Another example with lower resolution

Page 17: Mass spectroscopy

Chemical Composition of Living Matter27 of 92 natural elements are essential.  Elements in biomolecules (organic matter): H, C, N, O, P, S These elements represent approximately 92% of

dry weight.

Organic Matter Organized in "building blocks"

amino acids polypeptides ( proteins)

monosaccharides starch, glycogen

nucleic acids DNA, RNA 

Back to Basics…

Page 18: Mass spectroscopy

element nominal exact Percent average

mass mass abundance mass

 C 12 12.00000 98.9%

13 13.00335 1.1% 12.00115

H 1 1.00783 99.98%

2 2.0140 0.02% 1.008665

O 16 15.99491 99.8% 18 17.9992 0.02% 15.994

 N 14 14.00307 99.63%

15 15.00011 0.37% 14.0067

S 32 31.97207 94.93%

33 32.97146 0.76%

34 33.96787 4.29% excercise

  

Mass (Weights) of Atoms and Molecules

Page 19: Mass spectroscopy

 Ethyl acetate C4H8O2

4 C12 4 x 12.0000 48.0000 8 H1 8 x 1.0078 8.064 2 O16 2 x 15.99949 31.9898

Nominal Mass: 48 + 8 + 32 = 88

Monoisotopic Mass: 88.0555

Average Mass: 48.04446 + 8.06932 + 31.988 = 88.10178  

Mass or Molecular Weight of molecules

Page 20: Mass spectroscopy

Amino Acids• There are 20 amino acids. All have the

same basic structure but with different side chains:

• Examples: side chain group

H

Glycine, or Gly, or G

Arginine, or Arg, or R

Page 21: Mass spectroscopy

All the 20 Structures

* Picture copied from Dr. R.J. Huskey’s website: http://www.people.virginia.edu/~rjh9u/aminacid.html

Page 22: Mass spectroscopy

Peptides and Proteins

H

Glycine, or Gly, or G

Arginine, or Arg, or R

GR

peptide bonds

N-terminal C-terminal

Page 23: Mass spectroscopy

Exact Mass of Amino Acid Residues in Proteins

Gly G 57.02150Ala A 71.03720Gln Q 128.05860Lys K 128.09500Glu E 129.04270

Note: Leu (L) = Ile (I) = 113.08410

Mass of Amino Acids Residues

Page 24: Mass spectroscopy

Amino Acid Table

AA Codes Mono.

IONSOURCE.COM

AA Codes Mono.Gly G 57.021464 Asp D 115.02694Ala A 71.037114 Gln Q 128.05858Ser S 87.032029 Lys K 128.09496Pro P 97.052764 Glu E 129.04259Val V 99.068414 Met M 131.04048Thr T 101.04768 His H 137.05891Cys C 103.00919 Phe F 147.06841Leu L 113.08406 Arg R 156.10111Ile I 113.08406 CMC 161.01467

Asn N 114.04293 Tyr Y 163.06333

- - - Trp W 186.07931

  

Page 25: Mass spectroscopy

Cysteine

Proteins are often treated so that cysteine becomes carboxyamidomethyl cysteine (CamC) or Carboxymethyl (CmC) in order to break the disulphide bonds.CamC = 160.03

Page 26: Mass spectroscopy

tripeptide (MW 71.04+87.03+147.07+18.01)=323.15More precisely: monoisotopic mass 323.1481 average mass 323.3490

Ala-Ser-Phe (ASF)

Mass of Peptides and Proteins

Page 27: Mass spectroscopy

In a mass spectrum

323.15 324.15 325.15

Deconvolution adds all the isotopic peaks to the monoisotopic peak. So, the later process does not need to worry about the isotopes.Monoisotope peak

isotope peaks

Page 28: Mass spectroscopy

Check the difference

Page 29: Mass spectroscopy

ESI and Multiply Charged Ions

Page 30: Mass spectroscopy

Electrospray

Page 31: Mass spectroscopy

Electrospray Ionization: Formation of Charged Droplets

Formation of multiply charged ions

Ionization (2) – ESI

Page 32: Mass spectroscopy

Multiply Charged Ions• The same molecules may be charged

differently, and therefore form a few peaks in the spectrum.

323.15

324.15

325.15

162.08

162.58

163.08

m/z(M+2)/2(M+3)/3

For protein/peptide with positive charges, the charge is obtained from adding protons (which has mass approx. 1 dalton. As a result, a molecule with mass M will have peaks at (M+Z)/Z

(M+1)/1

Page 33: Mass spectroscopy

How to determine charge states?

• Isotope ions when resolution is enough.• Check different charge states when resolution

is not enough.

Page 34: Mass spectroscopy

Exercise

395.73

396.22

397.24

Page 35: Mass spectroscopy

Exercise

Page 36: Mass spectroscopy

Exercise

(A) “Multi-charge envelope” (B) After “Charge-deconvolution algorithm”

1541.9

1413.21304.7

1211.9

Page 37: Mass spectroscopy

Baseline

Page 38: Mass spectroscopy

Baseline correction

Page 39: Mass spectroscopy

Convex Hull Method

convex

not convex

Page 40: Mass spectroscopy

Convex Hull

• A convex hull is such that all the data points are above the lines and their extensions.

Page 41: Mass spectroscopy

How to calculate convex hull?

• Stack S contains all the data points that form the convex hull so far.• Data point D[i] = (D[i].x, D[i].y).

Algorithm:

1. S.push( D[0] ); s.push(D[1])2. for i from 2 to n2.1 while D[i], S.top(), S.secondtop() are concave2.1.1 S.pop();2.2 S.push(D[i]);3. return S

S.top()

S.secondtop() D[i]

Page 42: Mass spectroscopy

Analyze the convex hull algorithm

• Correctness– The algorithm finishes.– The output is a convex hull.– The proof will be included in an assignment.

• Time complexity– O(n) time.– Proof: each point is checked only once, and added

to (and therefore removed from) the stack at most once.

Page 43: Mass spectroscopy

Summarize of spectrum preprocessing

• Baseline correction• Centroiding• Charge recognition and deconvolution• Noise removal

Page 44: Mass spectroscopy

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