Example sentences of "[pers pn] get for [art] " in BNC.

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1 ‘ The money I get for the scrap is paid into the Finance Department , and when the fund has built up to a worthwhile sum I 'll be calling for suggestions for a local charity to whom we can donate the cash . ’
2 ‘ That 's a bargain when you consider how much protection you get for a building 's contents alone , ’ says Kelly .
3 What sort of a racehorse d' you think you get for a hundred quid ?
4 Weight for weight it does not compare favourably with foods like cereals and nuts in fibre content , although it works out well when you take into account how much fibre you get for a modest number of calories .
5 Yet the final equation of what you can afford to spend on a new car is likely to be influenced by what you get for the old one .
6 Well it 's only fifteen thirty five now so Oh it is two hours you get for the er that 's right , it 's not an hour and a half , it 's two hours you get is n't it ?
7 and they absconded it , and the dog has n't a hope in hell and also the ones you get for the kids , when you sit in them they sit up like little chairs do n't they ?
8 Now , I 'm a pensioner , and I think it 's a scandal what we get for a pension after all the years that you , you fight for you , you put away for your old age , and before you know it you 've nothing !
9 Quantum theory then predicts that when a measurement of some property of one of the particles ( call it A ) is made the results we obtain for certain measurements on particle B depend , not only on the results we get for the measurement on A , but also on what property of A we decide to measure .
10 Since the values for E and G vary , of course , for each solid the values we get for the theoretical strengths will vary too .
11 With the aid of eqn ( 2.4 ) we get for the force upon
12 The usual convention is to choose the reference point at infinity and choose the corresponding potential ( a ) = 0 , so we get for the potential of a point charge
13 Performing the integration in the z direction for any finite length , we get for the electric field strength unc in agreement with eqn ( 2.41 ) .
14 Noting that unc we get for the components of the magnetic field
15 Turning now to the case when the point of observation is in the vicinity of the axis , we get for the vector potential
16 Hence we get for the magnetic flux density
17 Assuming now that all the flux produced by coil 1 will pass through coil 2 as well , we get for the voltage in coil 2
18 Erm what we get for the money , and erm where there are possibilities for us to consider reducing that overhead .
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