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With our Rails project created, we can install Delayed Job Unlike BackgrounDRb, Delayed Job has no prerequisite gems that need to be installed So installing the plugin is simply a matter of running the following command from within the Rails application folder:

(10.2.97)

P l1 = W [sin 2 () sin2 ()' + 2 sin () sin ()' cos () cos ()' cos( - ') + cos 2 () cos 2 ()' cos 2( - ')] (10.2.98) 2 () sin 2( - ') P12 = W cos (10.2.99) 2 () P = W [cos 0 sin 0 sin ()' sin( - ') cos

P 21

. cos ()' sin( - ') cos( - ')] = W cos 2 ()' sin 2( - ')

1 1

(10.2.100) (10.2.101) (10.2.102) (10.2.103) (10.2.104) (10.2.105)

P 22 =wcos 2( - ') P23 = - W cos 0' sin( - ') cos( - ') P 31 = w [-2 sin () sin ()' cos 0' sin( - ')

- 2 cos () cos 2 ()' cos( - ') sin( - ')]

= 2w cos () sin( - ') cos( - ')

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P33 = w [sin 0 sin 0' cos( - ')

I would like to take this opportunity to point out that the URL we used to install the plugin is actually a fork of the original project Currently this fork is generally considered to be the best version of Delayed Job As you will see in a minute, it has a few enhanced offerings, including a generator to generate the necessary migrations and files we need This may change in the future Should you want to use Tobias s original version of the project, or if he merges in the changes from other forks, you can find the original version at http://githubcom/tobi/delayed_job/tree/master As I mentioned, we need to generate a migration to create the table that Delayed Job will use to store the tasks you ask it to perform To do that we can use the builtin generator to create the migration:

L( p)

- sin 2( - '))]

- ')

(10.2.106) (10.2.107)

=w[sin 0 sin 0' cos( - ')

(10.2.108) (10.2.109)

O( p j ) =

cos 8 = cos 0 cos 0'

+ sin 0 sin 0' cos(

- ')

Simulations of particle positions by packing several thousands of particles randomly in a box was done in 8. In this section, we solve Maxwell's equations for scattering by these realizations of particle positions. The simulations are performed over many samples (realizations) and the scattering results are averaged over these realizations. The results give information about the collective scattering effects of many particles packed together. In this section, we use volume integral equation to simulate the scattering by densely packed spheres. We still restrict our attention to the case of small particles. In Section 4, we shall use multipole expansions to study scattering by spheres. 3.1 Volume Integral Equation

This should generate the following migration:

Consider waves in an inhomogeneous medium with permittivity Ep(r). For the case of N discrete scatterers with permittivity Ep , occupying regions VI, V2 , , VN, we have discontinuous permittivity Ep(r) with

cos t(i, j) + C j (t)

(10.3.1)

_ Ep(r) _ x(r) = - - - 1 = Er(r) - 1

(10.3.2)

where Er (r) is the relative permittivity. The electric field is, from (2.1.37) of 2,

E(r) = Einc(r)

j Ri (t)

dr'g(r, r')x(r')E(r')

(10.3.3)

dr' g(r, r')\7' . (x(r')E(r'))

class CreateDelayedJobs < ActiveRecord::Migration def selfup create_table :delayed_jobs, :force => true do |table| tableinteger :priority, :default => 0 tableinteger :attempts, :default => 0 tabletext :handler tabletext :last_error tabledatetime :run_at tabledatetime :locked_at

Note that the integration space of (10.3.3) is over all space. The first integral is over regions where x(r) is nonzero, that is, where Ep(r) i- E. The second integral is over space where 'V. (X(r)E(r)) is nonzero. For the case of discontinuous permittivity like discrete scatterers, the jump of permittivity across the scatterer boundary can have nonzero divergence at the boundary and give rise to a surface integral. Thus 'V. (x(r)E(r)) in (10.3.3) can be both zero outside and inside the scatterer and yet have a surface integral contribution. We can also use polarization density P(r). Let (10.3.4) Then (10.3.3) becomes

cos t(i, j ) + C j (t)

E(r) = Einc(r)

dr'g(r, r') P(r')

dr'g(r,r')'V'. (p(r'))

(10.3.5)

dr'g(r,r')'V' (p(r'))

O( p)

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