The Chemistry Maths Book, Second Edition

(Grace) #1

24 Chapter 1Numbers, variables, and units


EXAMPLES 1.18Molecular properties: mass, length and moment of inertia


(i)mass. Atomic and molecular masses are often given as relative masses:A


r

for an


atom andM


r

for a molecule, on a scale on whichA


r

(


12

C) 1 = 112. On this scale,A


r

(


1

H) 1 =


1.0078andA


r

(


16

O) 1 = 1 15.9948. The corresponding relative molar mass of water is


M


r

(


1

H


2

16

O) 1 = 121 × 1 A


r

(


1

H) 1 + 1 A


r

(


16

O) 1 = 1 18.0105,


the molar mass is


M(


1

H


2

16

O) 1 = 1 18.0105 g mol


− 1

1 = 1 0.01801 kg mol


− 1

,


and the mass of the individual molecule is


m(


1

H


2

16

O) 1 = 1 M


r

(


1

H


2

16

O) 1 × 1 u 1 = 1 2.9907 1 × 110


− 26

kg


(ii)length. The bond length of the oxygen molecule is R


e

1 = 1 1.2075 1 × 110


− 10

m, and


molecular dimensions are usually quoted in appropriate units such as the picometre


pm 1 = 110


− 12

m or the nanometre nm 1 = 110


− 9

min spectroscopy, and the Ångström


Å 1 = 110


− 10

mor the Bohr radiusa


0

1 = 1 0.529177 1 × 110


− 10

m 1 = 1 0.529177 Åin theoretical


chemistry. Thus, for O


2

,R


e

1 = 1 1.2075 Å 1 = 1 120.75 pm.


(iii)reduced mass and moment of inertia. The moment of inertia of a system of two


masses,m


A

andm


B

, separated by distanceRisI 1 = 1 μR


2

, where μis the reduced


mass, given by


Relative atomic masses can be used to calculate the reduced mass of a diatomic


molecule. Thus for CO,A


r

(


12

C) 1 = 112 andA


r

(


16

O) 1 = 1 15.9948, and these are the atomic


masses in units of the unified atomic mass unit u. Then


=6.8562 1 × 1 1.66054 1 × 110


− 27

kg 1 = 1 1.1385 1 × 110


− 26

kg


The bond length of CO is 112.81 1 pm 1 = 1 1.1281 1 × 110


− 10

1 m, so that the moment of


inertia of the molecule is


I 1 = 1 μR


2

1 = 1 (1.1385 1 × 110


− 26

kg) 1 × 1 (1.1281 1 × 110


− 10

m)


2

= 1 1.4489 1 × 110


− 46

kg m


2

The reduced mass and moment of inertia are of importance in discussions of


vibrational and rotational properties of molecules.


0 Exercises 104, 105


μ(


.


.


12 16

12 15 9948


27 9948


CO)


u


u


2

=


×


















=6 8562. u


11 1


μ


=+ μ=


mm +


mm


mm


AB

AB

AB

,

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