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a) mono-substitutions: bp trends
ALKANES ALKYL HALIDES
#C R-H R-F R-Cl R-Br R-I1 -162 -78 -24 + 3 +42 2 - 89 -32 +12 +38 +72 3 - 42 -3 +47 +71 +103 6 +69 +92 +134 +155 +180
trends verbalized:higher Carbon count and bigger halogens (X) mean higher bp in RX.
Physical Trends in Alkyl Halides (BP): a modest proposal (see also-text pp 289-90) …an example of physical organic chemistry
Dipole slightly decreasing---------
b) multiple halogen substitutions : bp trendsX CH3X CH2X2 CHX3 CX4
F -78 -51 -82 -128Cl -24 +40 +61 +77Br +3.5 +97 +149 +189I +42.5 +182 +218 +218
CH3CH2 X CH3CHX2 CH3CX3 CX3CX3
F -32 -25 -47 -78 Cl +12.3 +57 74 146 Br +38.5 +109 +153 318
trends verbalized: in the main, more halogens correlates with higher bp, but something else unconnected to dipole overrides
dipole effect and it’s not just a mass effect-see “anomalies”
Dipole increases high dipole 0 dipole
high dipole 0 dipole
RX CH3 F CH3 Cl CH3Br CH3 IMolecular mass (g/mol) 34 50 95 142
dipole moment(debyes) 1.86 1.89 1.82 1.62
boiling point (o C) -78 -24 +3 +42
c) “anomalies”
trends verbalized Neither permanent dipoles nor molecular mass are the whole story in allowing prediction of bp 1) why are equivalent masses of alkanes vs alkyl halides so different??? 2) how come a low dipole alkane beats a high dipole alkyl halide in bp ?…Speculation is that something connected to electronic cloud’s `puffiness’ (“P”) is involved
bp of ~equivalent R-H mass -32 +5 69 170
#C in alkane 2 3 6 10
dipole moment (debyes) 0 0.08 0.08 0.07
P=the ease of distortion of the electron cloud of a molecular entity by an electric field (such as that due to the proximity of a charged reagent). P is experimentally measured as the ratio of induced dipole moment (induced ) to the field E which induces it:
P = induced /E
Electronic puffiness =Polarizability, P, defined:
Test (-) charge (`E’)
Extreme polarizability(larger atoms)
Slight polarizability(smaller atoms)
Original, undeformed electron cloud border
Polarizability pictured:Position of original, undeformed cloud
Test distance
Polarizability quantified (sort of…)
Quantifying the intuitionP ~ 1
relevant electron density
The Doc’s little `intuition’less electrons per unit volume=> easier to push e- around=higher P
=>P inverse to electron density
relevant electron density ~ # valence e- in molecule molecular volume
P ~ 1 ~ 1 relevant electron density # valence e-
r3
~ # valence e- in molecule r3
=r3
# valence e-
CH3 F CH3 Cl CH3Br CH3 IMolecular mass (g/mol) 34 50 95 142
dipole moment(debyes) 1.86 1.89 1.82 1.62
boiling point (o C) -78 -24 +3 +42
# valence e- 14 14 14 14r(C-X) (10-10 m) 1.35 1.77 1.94 2.14
Testing the model
P ~ r3
#valence e-
P~ r3/#valence e- = 0.18 0.40 0.53 0.70
y = 229.72x - 118.2
R2 = 0.999
-100
-80
-60
-40
-20
0
20
40
60
0 0.2 0.4 0.6 0.8
P ~ 1/valence electron density
ob
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rve
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oili
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pt,
C
F
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Br
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Plot of observed CH3X boiling point versus rough polarizability measure: P ~ 1/valence electron density
Test of the model: do you get linear relationship ?
Least square r2 ~ 1
Linear correlation of a model with physical observations makes for a….
Happy Physical Organic Chemistry Cat