329
In Situ Water Treatment
Since the collected water into the plastic tank is just nothing but the liquid form of
vapor, it will not require any sedimentation, coagulation, and chlorination to clean
the water. Only mixing physics (UV application) and filtration will be required to
treat the water to meet the US National Primary Drinking Water Standard code [cc].
It is the simplest way to treat water by using SODIS system (SOlar DISinfection),
where a transparent container is filled with water and exposed to full sunlight for
several hours. As soon as the water temperature reaches 50 °C with a UV radiation
of 320 nm, the inactivation process will be accelerated in order to lead to complete
microbiological disinfection immediately and the treated water shall be used to
meet the total domestic water demand (Fig. 14.2).
Results and Discussion
To mathematically determine the electric static force proliferation around the plastic
tank to confirm the tug down of the water, I have initially solved the dynamic photon
proliferation by integrating HSEF electric field; thus, the local U(1) gauge invariant
allows to add a mass term for the gauge particle under ∅
′
→ e
iα(x)
∅. In detail it can
be explained by a covariant derivative with a special transformation rule for the
scalar field expressed by [11, 12]
∂ →
= ∂ =
[
]
=
+ ∂
′
µ
µ
µ
µ
µ
µ
µ
µ
α
D
i eA
A
A e
A
covariant derivatives
derivati
1
v ves
(14.13)
where the local U(1) gauge invariant HSEF for a complex scalar field is given by
(14.14)
The term
1
4
F F
v
v
∝
∝ is the kinetic term for the gauge field (heating photon) and
V(∅) is the extra term in the HSEF that will be V(∅
∗
∅) = μ
2
(∅
∗
∅) + λ (∅
∗
∅)
2
.
Therefore, the HSEF (ɧ) under perturbations into the quantum field is initiated
with the massive scalar particles ϕ 1 and ϕ 2 along with a mass μ. In this situation
μ
2
< 0 has an infinite number of quantum; each has been satisfied by
φ φ
µ λ
1
2
2
2
2
2
+ = −
=
/
v ; and the ɧ through the covariant derivatives using again the
shifted fields η and ξ defined the quantum field as φ
υ η
ξ
0
1
2
=
+
(
)+
i .
(14.15)
Results and Discussion
In Situ Water Treatment
Since the collected water into the plastic tank is just nothing but the liquid form of
vapor, it will not require any sedimentation, coagulation, and chlorination to clean
the water. Only mixing physics (UV application) and filtration will be required to
treat the water to meet the US National Primary Drinking Water Standard code [cc].
It is the simplest way to treat water by using SODIS system (SOlar DISinfection),
where a transparent container is filled with water and exposed to full sunlight for
several hours. As soon as the water temperature reaches 50 °C with a UV radiation
of 320 nm, the inactivation process will be accelerated in order to lead to complete
microbiological disinfection immediately and the treated water shall be used to
meet the total domestic water demand (Fig. 14.2).
Results and Discussion
To mathematically determine the electric static force proliferation around the plastic
tank to confirm the tug down of the water, I have initially solved the dynamic photon
proliferation by integrating HSEF electric field; thus, the local U(1) gauge invariant
allows to add a mass term for the gauge particle under ∅
′
→ e
iα(x)
∅. In detail it can
be explained by a covariant derivative with a special transformation rule for the
scalar field expressed by [11, 12]
∂ →
= ∂ =
[
]
=
+ ∂
′
µ
µ
µ
µ
µ
µ
µ
µ
α
D
i eA
A
A e
A
covariant derivatives
derivati
1
v ves
(14.13)
where the local U(1) gauge invariant HSEF for a complex scalar field is given by
(14.14)
The term
1
4
F F
v
v
∝
∝ is the kinetic term for the gauge field (heating photon) and
V(∅) is the extra term in the HSEF that will be V(∅
∗
∅) = μ
2
(∅
∗
∅) + λ (∅
∗
∅)
2
.
Therefore, the HSEF (ɧ) under perturbations into the quantum field is initiated
with the massive scalar particles ϕ 1 and ϕ 2 along with a mass μ. In this situation
μ
2
< 0 has an infinite number of quantum; each has been satisfied by
φ φ
µ λ
1
2
2
2
2
2
+ = −
=
/
v ; and the ɧ through the covariant derivatives using again the
shifted fields η and ξ defined the quantum field as φ
υ η
ξ
0
1
2
=
+
(
)+
i .
(14.15)
Results and Discussion