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HIGH VOLTAGE- L2-electrostatics

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HIGH VOLTAGE TECHNIQUES
REVΔ°EW: Electrostatics & Magnetostatics
Assistant Professor Suna BOLAT KRÖGER
Eastern Mediterranean University
Department of Electric & Electronic Engineering
Zap
You walk across the rug, reach for the doorknob and..........ZAP!!!
In the winter, when you change your pullover you hear and/or
see sparks...
you come inside from the cold, pull off your hat and......BOING!!!
Static hair - that static electricity makes your hair stand straight
out from your head.
What is going on there?
Static electricity...
...is the imbalance of positive and negative charges.
• As you walk across a carpet, electrons move from the rug to you.
Now you have extra electrons and a negative static charge. Touch a
door knob and ZAP! The door knob is a conductor. The electrons
jump from you to the knob, and you feel the static shock.
• We usually only notice static electricity in the winter when the air is
very dry. During the summer, the air is more humid. The water in
the air helps electrons move off you more quickly, so you can not
build up as big a static charge.
Static
Question: Static? What does that mean?
Answer: constant with time
Question: How constant is it? Does it really not move at all?
Answer: there is movement of charges.
In fact, when you get zapped, charges are actually moving
between your fingers and the doorknob. However, the
movement is only brief compared to the current in a closed
circuit.
Static regime
In the static regime, electromagnetic quantities do not
vary as a function of time.
We have two main cases:
• ELECTROSTATICS
• MAGNETOSTATICS
Definitions and units
Symbol
𝛁.
𝛁×
𝝏
𝝏𝒕
E
B
D
H
ε0
μ0
Meaning (first term is the most common)
SI Unit of measure
Differential operators
the divergence operator
per meter (factor contributed by applying
either operator)
the curl operator
per second (factor contributed by applying the
partial derivative with respect to time
operator)
Fields
ο‚·
electric field, also called
volt per meter or, equivalently, [V/m]
ο‚·
the electric field intensity
newton per coulomb [N/C]
ο‚·
magnetic field, also called: the magnetic
tesla, or equivalently, [T]
induction
ο‚·
weber per square meter, [Wb/m2]
ο‚·
the magnetic field density
ο‚·
volt-second per square meter [V s/m2]
ο‚·
the magnetic flux density
ο‚·
electric displacement field, also called:
ο‚·
coulombs per square meter or [C/m2]
ο‚·
the electric induction
equivalently,
ο‚·
the electric flux density
ο‚·
newton per volt-meter [N/V m]
ο‚·
magnetizing field, also called: auxiliary
magnetic field
ampere per meter [A/m]
ο‚·
magnetic field intensity
ο‚·
magnetic field
permittivity of free space, also called the
farads per meter [F/m]
dielectric constant, a universal constant
permeability of free space, also called the
henries per meter, [H/m] or newtons per
magnetic constant, a universal constant
ampere squared [N/A2]
Electric field
Electric field is said to exist in a region of space if a charge
experiences a force when placed anywhere in that region.
If a unit positive charge is placed
at some point in the field, the
force experienced by it is said to
be the electric stress at that point.
Electrostatics
The electric charges do not change position in time.
Therefore, ρ, E and D are constant and there is no
magnetic field H, since there is no current density J.
Magnetostatics
The charge crossing a given cross-section (current) does
not vary in time.
Therefore, J, H and B are constant.
Although charges are moving, the steady current
maintains a constant charge density ρ in space and the
electric field E is static.
Electric Field & Magnetic Field
Voltage is associated with electric field
Current is associated with magnetic field
Maxwell’s equations
Basic equations:
πœ•π΅
πœ•π‘‘
π‘Ÿπ‘œπ‘‘ 𝐻 = 𝛻 × π» = 𝐽
𝑑𝑖𝑣 𝐷 = 𝜌
𝑑𝑖𝑣 𝐡 = 0
Auxiliary equations (constructive equations):
π‘Ÿπ‘œπ‘‘ 𝐸 = 𝛻 × πΈ =
𝐽 =𝜎𝐸+πœŒπ‘‰+
𝐷 = πœ€πΈ
ο₯: Dielectric constant = ο₯0 ο₯r
ο₯r : relative dielectric constant (no unit), relative
permittivity
ο₯0 = 8.854. 10-12 F/m dielectric constant for space,
permittivity
πœ•π·
πœ•π‘‘
µ: permeability
µr: relative permeability
µ0 = 4 π. 10-7 H/m magnetic constant, relative
permeability of space
The electrostatic equations
The equations of electrostatics are obtained Maxwell’s
equations,
By assuming ∂/∂t , J, H and B are all zero:
The electrostatics equations:
Poisson equation
𝑑𝑖𝑣 𝐷 = 𝛻. 𝐷 = 𝜌
𝑑𝑖𝑣 𝐷 = 𝛻. πœ€πΈ = 𝛻 πœ€ −𝛻𝐸
= −πœ€π›» 2 V = 𝜌
grad V
𝛻2V
=
𝜌
−
πœ€
𝝆
βˆ†π• = −
Poisson equation
𝜺
The electrostatics equations:
Laplace’s equation
If there is no free charges at the medium 𝜌 = 0.
βˆ†π• = 𝟎
Laplace’s equation
Operators:
Laplacian
𝝏𝟐 𝑽 𝝏𝟐 𝑽 𝝏𝟐 𝑽
βˆ†π‘½ = 𝟐 + 𝟐 + 𝟐
𝝏𝒙
ππ’š
𝝏𝒛
Operators:
Gradient
𝝏𝑽
𝝏𝑽
𝝏𝑽
𝛁𝑽 =
π’Šπ’™ +
π’Šπ’š +
π’Šπ’›
𝝏𝒙
ππ’š
𝝏𝒛
Laplace’s equation in Cartesian coordinates:
𝝏 𝟐 𝑽 𝝏𝟐 𝑽 𝝏𝟐 𝑽
βˆ†π‘½ = 𝟐 + 𝟐 + 𝟐 = 𝟎
𝝏𝒙
ππ’š
𝝏𝒛
𝝏𝑽
𝝏𝑽
𝝏𝑽
𝛁𝑽 =
π’Šπ’™ +
π’Šπ’š +
π’Šπ’›
𝝏𝒙
ππ’š
𝝏𝒛
Laplace’s equation in Polar coordinates:
𝝏𝟐 𝑽 𝟐 𝝏𝑽 𝟏 𝝏𝟐 𝑽
𝟏
𝝏𝟐 𝑽 π’„π’π’•π’‚π’πœ½ 𝝏𝟐 𝑽
βˆ†π‘½ = 𝟐 +
+ 𝟐 𝟐+ 𝟐
+
=𝟎
𝟐
𝟐
𝟐
𝟐
𝝏𝒓
𝒓 𝝏𝒓 𝒓 𝝏𝜽
𝒓 π’”π’Šπ’ 𝜽 𝝏𝜢
𝒓
𝝏𝜽
𝝏𝑽
𝟏 𝝏𝑽
𝟏 𝝏𝑽
𝛁𝑽 =
π’Šπ’“ +
π’ŠπœΆ +
π’Šπœ½
𝝏𝒓
𝒓. π’”π’Šπ’πœ½ 𝝏𝜢
𝒓 𝝏𝜽
Laplace’s equation in Cylindrical coordinates:
𝝏𝟐 𝑽 𝟏 𝝏𝑽 𝟏 𝝏𝟐 𝑽 𝝏𝟐 𝑽
βˆ†π‘½ = 𝟐 +
+ 𝟐 𝟐+ 𝟐 =𝟎
𝝏𝒓
𝒓 𝝏𝒓 𝒓 𝝏𝜽
𝝏𝒛
𝝏𝑽
𝟏 𝝏𝑽
𝝏𝑽
𝛁𝑽 =
π’Šπ’“ +
π’Šπœ½ +
π’Šπ’›
𝝏𝒓
𝒓 𝝏𝜽
𝝏𝒛
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