Answers to Problem Set 2
200-reflection:
Similarly, for 100-reflection:
From the table and using proportion, we find for 200-reflection:
From the equation
F(S) =
nS
fn e2p i (hx +
ky + lz)
we have for 200-reflection:
and for 100-reflection:
Obviously, 100-reflection is an example of destructive interference ("extinction").
Finally, the intensity for the first reflection will be:
Answer:
d200
=
5.638 Å / (22+02+02)1/2
=
5.638 Å / 2
=>
sin q /
l
=
1/(2d)
=
(5.638 Å)-1
=
0.177 Å-1.
d100
=
5.638 Å / (12+02+02)1/2
=
5.638 Å
=>
sin q /
l
=
(2 · 5.638 Å)-1
=
0.0887 Å-1.
fNa+
=
8.39 + (9.035 - 8.39) · 0.027 / 0.05
=
8.74
fCl-
=
12.20 + (14.12 - 12.20) · 0.027 / 0.05
=
13.24.
Comment: The idea is right but in fact you weighted
the values the wrong way round so that they were closer to the 0.15 rather than
the 0.20 columns; the resulting values are therefore slightly wrong, but this
is only a small error.
4 Marks
F200(S)
=
fNa+
{
1 + 1 +
e
2p i ( 2 · 1/2 )
+
e
2p i ( 2 · 1/2 )
} +
fCl-
{
e
2p i ( 2 · 1/2 )
+ 1 + 1 +
e
2p i ( 2 · 1/2 )
}
=
2 · ( fNa+ + fCl- )
( 1 + e
2p i )
=
2 · ( fNa+ + fCl- )
( 1 + cos 2p + i sin 2p )
=
87.90,
F100(S)
=
fNa+
{
1 + 1 +
e
2p i ( 1 · 1/2 )
+
e
2p i ( 1 · 1/2 )
} +
fCl-
{
e
2p i ( 1 · 1/2 )
+ 1 + 1 +
e
2p i ( 1 · 1/2 )
}
=
2 · ( fNa+ + fCl- )
( 1 + e
p i )
=
2 · ( fNa+ + fCl- )
( 1 + cos p + i sin p )
=
0.
Comment: This is the right idea. You might
also point out that the 100-reflection is one of many examples of
destructive interference brought about by crystal symmetry.
5 Marks
Comment: This is right. The small difference
from my value is due only to my using slightly different f values for
Na and Cl.
5 Marks
There are five more planes that have the same
d as
200-reflection: -200, 020, 0-20, 002, 00-2. Therefore, the multiplicity for 200-reflection
is: 6.
Comment: This is correct.
3 Marks
| d200 | = | 5.638 Å / (22+02+02)1/2 | |
| = | 5.638 Å / 2 | ||
| => | sin q | = | l /(2d200) |
| = | 1.54 Å / 5.638 Å | ||
| = | 0.27315 |
We deal with case (3) (unpolarised X-rays), and formula P = (1 + cos2 2q )/2. The Polarisation allowance factor for this case will be:
| P | = | 0.5 · [ 1 + ( cos2 q - sin2 q )2 ] | |
| = | 0.5 · [ 1 + (1 - 2 sin2 q )2 ] | ||
| = | 0.5 · [ 1 + (1 - 2 · 0.273152 ) 2 ] | ||
| = | 0.86. |
Comment: This is right. I like the neat
way of calculating the answer without having to use the actual value
of the angle.
4 Marks
| L | = | (sin2q cos q)-1 | |
| = | [sin2q ( 1 - sin2q )1/2 ]-1 | ||
| = | [ 0.273152 · ( 1 - 0.273152 )1/2 ]-1 | ||
| = | 13.93. |
[The value for sin q calculated in the previous answer was used here.]
Comment: This is right. Again a neat
avoidance of finding the angle.
3 Marks
| I111/ I200 | = | ( j111 P111 L111 F1112 ) / ( j200 P200 L200 F2002 ) | |
| = | ( 8 · 0.89 ·18.39 · 398 ) / ( 6 · 0.86 ·13.93 · 7726 ) | ||
| = | 0.0938. |
Comment: This is correct.
3 Marks
Two possible examples might be:
It is hoped that, with the combination of your imagination and all the course material you have received so far, you should have no difficulty devising some 5-10 plausible factors; perhaps you might even come up with more than 10.
Generally, here belong all the factors that favorize some reflections.
Comment: You have many good answers though
very slightly more explanation might have been given for example to
explain why one reflection is affected more than another (see my
model answer comments). I have given 1 mark for each reason totalling...
7 Marks
Overall Comment: This is an excellent and
well-thought out set of answers.