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Lecture handout including QS - Department of Materials Science ...

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BH19 Course B: <strong>Materials</strong> for Devices BH19<br />

How big is a polymer molecule<br />

A polymer chain can be modelled as a series <strong>of</strong> shorter, rigid segments (each <strong>of</strong> length l ) that can<br />

rotate freely where they join.<br />

“Random walk”:<br />

r 1<br />

• If the chain consists <strong>of</strong> n segments, and it<br />

were stretched out straight, its length, L, would<br />

be nl.<br />

• end-to-end vector,<br />

• A useful measure <strong>of</strong> the size <strong>of</strong> the polymer molecule is given by the<br />

<br />

2<br />

root mean square <strong>of</strong> R n<br />

: R n<br />

€ €<br />

r n-1<br />

r 2<br />

r 3 r 4<br />

R n -1<br />

R n<br />

r n<br />

€<br />

also,<br />

<br />

R n<br />

=<br />

<br />

R n−1<br />

=<br />

n<br />

<br />

∑ and<br />

• The average value € <strong>of</strong> the end to end vector,<br />

<br />

R n<br />

, is zero: R n<br />

= 0<br />

€<br />

i=1<br />

r i<br />

<br />

n−1<br />

∑r i<br />

i=1<br />

<br />

R n<br />

= R <br />

n−1<br />

+ r <br />

n<br />

1 2<br />

where γ is the angle between the vector<br />

R 2 n<br />

= ( R n−1<br />

+ r n ) ⋅ <br />

Rn−1 + r n<br />

€ 2<br />

= R n−1<br />

+ € 2R n−1<br />

× l cosγ<br />

( ) = R 2<br />

n−1<br />

( ) + l 2<br />

The average value <strong>of</strong> cosγ must be zero, and therefore,<br />

( ) + r n<br />

+ 2 R n−1<br />

⋅ r n<br />

and the last segment,<br />

<br />

R n<br />

2<br />

2<br />

= R 2<br />

n−1<br />

€ = R 2<br />

n−2<br />

<br />

r n<br />

+ l 2<br />

€<br />

+ l 2 + l 2 etc.<br />

<br />

R n−1<br />

And, by induction:<br />

mean square end-to-end distance,<br />

R n<br />

2<br />

= nl 2<br />

root mean square,<br />

R n<br />

2<br />

1 2<br />

= n 1 2<br />

l<br />

We might assume that each segment <strong>of</strong> the chain, € l, corresponds to a single C-C bond. But such<br />

segments can never be completely freely jointed (bond angles are limited, and adjacent segments can<br />

simply get in the way <strong>of</strong> each other). € Hence real polymer chains are always stiffer than shown by this<br />

model using a single C-C bond as a segment length, and their stiffness is dependent upon the nature<br />

<strong>of</strong> the monomer units involved.<br />

The model can be used more generally if we define l, the segment length, as the length scale below<br />

which the chain is effectively straight and rigid – this is called the Kuhn length. The simple<br />

polyethylene structure has a Kuhn length <strong>of</strong> about 3.5 times the C-C bond length, whilst polystyrene,<br />

which has more bulky side-groups, has a Kuhn length <strong>of</strong> 5 × C-C (it’s stiffer).

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