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Introduction to Nanotechnology

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10.2. CATALYSIS 267<br />

where the length parameters a, d, and L are expressed in nanometers, and the density<br />

p has the units g/cm3. In Eq. (10.6~) the area of the side of the disk is neglected, and<br />

in Eq. (1 0.6d) the areas of two ends of the wire are disregarded. Similar expressions<br />

can be written for dis<strong>to</strong>rtions of the cube [Eq. (10.6b)l in<strong>to</strong> the quantum-well and<br />

quantum-wire configurations of Fig. 9.1.<br />

The densities of types 111-V and 11-VI semiconduc<strong>to</strong>rs, from Table B.5, are in the<br />

range from 2.42 <strong>to</strong> 8.25 g/cm3, with GaAs having the typical value p = 5.32 g/cm3.<br />

Using this density we calculated the specific surface areas of the nanostructures<br />

represented by Eqs. (10.6a), (10.6c), and (10.6d), for various values of the size<br />

parameters d and L, and the results are presented in Table 10.1. The specific surface<br />

areas for the smallest structures listed in the table correspond <strong>to</strong> quantum dots<br />

(column 2, sphere), quantum wires (column 3, cylinder), and quantum wells<br />

(column 4, disk), as discussed in Chapter 9. Their specific surface areas are<br />

within the range typical of commercial catalysts.<br />

The data tabulated in Table IO. 1 represent minimum specific surface areas in the<br />

sense that for a particular mass, or for a particular volume, a spherical shape has the<br />

lowest possible area, and for a particular linear mass density, or mass per unit length,<br />

a wire of circular cross section has the minimum possible area. It is of interest <strong>to</strong><br />

examine how the specific surface area depends on the shape. Consider a cube of side<br />

a with the same volume as a sphere of radius r<br />

4nr3<br />

- =a<br />

3<br />

(10.7)<br />

so a = (4~/3)''~r. With the aid of Eqs. (10.6a) and (10.6b) we obtain for this case<br />

Stub = 1.24SS,,, so a cube has 24% more specific surface than a sphere with the<br />

same volume.<br />

To obtain a more general expression for the shape dependence of the<br />

area:volume ratio, we consider a cylinder of diameter D and length L with the<br />

Table 10.1. Specific surface areas of GaAs spheres, long<br />

cylinders (wires) and thin disks as a function of their sizea<br />

Surface Area (m2/g)<br />

Size (nm) Sphere Wire Disk<br />

4<br />

6<br />

10<br />

20<br />

30<br />

40<br />

60<br />

100<br />

200<br />

28 1<br />

187<br />

112<br />

57<br />

38<br />

29<br />

19<br />

11<br />

6<br />

187<br />

125<br />

76<br />

38<br />

26<br />

19<br />

13<br />

8<br />

4<br />

94<br />

62<br />

37<br />

19<br />

13<br />

10<br />

6<br />

4<br />

2

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