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Electric field
the field in which an electric charge attracts or repels
Can be both radial and uniform
Electric charge
certain elementary particles, such as electrons and protons, that cause them to interact with reach other
Coulomb
unit of electric charge
One coulomb is equivalent to the charge transported by 1 ampere of current in a second
Protons charge - 1.6 x 10-19 C
Electrons have an electric charge of -1.6 x 10-19
Static electricity
build up of electric charge on the surface of an object due to the removal or addition of electrons, commonly caused by friction
Electric field
a region where a charged particle will experience a force
All charged objects surrounded by one
Direction of the lines represents the direction of the field, where it shows the direction a positive charge would move in the field
The concentration of field lines represent the strength of the field, the more concentrated the lines, the stronger the field

Coulomb's law / Force between two point charges equation
F= 1/4πε0 x Q1Q2/r2
Magnitude of F is proportional to the product of q1 and q2
Inversely proportional to the square of the distance between them
1/(4πε0) - coulombs constant
ε0 - permittivity of free space - 8.85 x 10-12 C2N-1m-2 or Fm-1

Radial electric field
Pointing in the direction which a positive test charge would go

Uniform electric field
Pointing in the direction which a positive test charge would go
Only in between two charged plates
electric field between two parallel plates,
Charge will experience same force wherever it is placed between the plates
Depends on the voltage between the plates and the distance between them
Typically measured in NC-1, but can also be in Vm-1
NC-1 typically for point charge and Vm-1 for parallel plates

Test charge
A small enough charge that does not impact the shape of a field
Fields around a pair of charges
Field on the side without the other charge behaves as a normal electric field

Electric field strength
The electrostatic force experienced per unit of positive test charge placed at a specific point in an electric field
Electric field strength equations
E = F / Q
All fields
E - Electric field strength
F - Force
Q - Charge
E = 1/(4πε0) x Q/r2
Radial fields only
E - Electric field strength
1/(4πε0) - coulombs constant
ε0 - permittivity of free space - 8.85 x 10-12 Fm-1
Q - Charge
r - distance between charges

Uniform electric field strength equation
E = V/d
E - Electric field strength
V - P.D. / voltage
d - distance
Electric Potential
If a positive test charge is moved from infinity to a position in an electric field, the electric potential energy of the charge will change.
Work is done on the charge
In an electric field the Ep is at infinity when it is around a point charge.
The strength of the field would be zero at infinity.

Work done from Electric potential equation
∆W = Q∆V
W - work done to move a charge
Q - Charge
V - Electric potential
Electric potential equation for a point charge (radial field)
V = Q / (4πεor)
Potential gradient
the rate of change of electric potential per unit change of distance in a certain direction within that field
Also known as the the electric field strength at a point
The gradient in a V-r graph
Potential gradient equation
E = ∆V/∆r
E - Electric field strength
∆V - change in potential
∆r - change in distance
Capacitor
a pair of plates with an insulator between them that store charge
Only works in a dc circuit (as charge needs to build up)
AC will remove and add charge to each plate resulting in an overall neutral charge
The electric field around capacitors is uniform

Capacitance
the amount of charged stored per unit potential difference between the plates
Capacitance equation
Q=CV
Q - Charge, measured in Coulombs
C - Capacitance, measured in Farads
Coulomb per volt = farad
V - Potential difference, measured in Volts
Charged stored factors
Distance between plates - Greater distance, hence less charge stored
Voltage - Greater voltage, hence more charge stored
Capacitance - Greater Capacitance, hence more charge stored
Size of plates - Greater area of plates, hence more charge stored
Work done from capacitance
The area under a Q-V graph
W = ½ QV
W is not proportional to V due to Q changing when V is changed so Q cannot be made constant while V varies with W
W = ½ CV2
W is proportional to V2
W = Q2 / 2C
W is proportional to Q2

Capacitor charging
Increasing the potential difference between the two plates of the capacitor
This stores charge within the capacitor

Capacitor discharging
Decreasing the potential difference between the two plates of the capacitor by using the potential difference to power a component
This decreases/uses charge within the capacitor

Capacitor charging graphs
The gradient of a charge time graph is the current
The area under a current time graph is the charge

Capacitor discharging graphs
The gradient of a charge time graph is the current
The area under a current time graph is the charge

Factors for time take for capacitor discharge
Time constant
Resistance of the resistor in the circuit
capacitance of capacitor
Time constant (𝛕)
the time taken for the charge on the capacitor to discharge to 1/e (~ 37%) of its initial value or the time taken to charge to 63%
1 time constant drops by 37% of its previous / initial value
The charge drops by the same proportion each time
Time constant equation
𝛕 = RC
𝛕 - time constant [s]
R - resistance [Ω]
C - capacitance [F]
Rate of removal of charge
Proportional to the amount of charge remaining
Half life of a discharging capacitor
the time taken for the charge, current or voltage of a discharging capacitor to reach half of its value
Half life of capacitor equation
t1/2 = 0.69𝛕 = 0.69RC