Unit D2: Electricity and magnetism
The gold leaf electroscope
The gold leaf electroscope
Where do the charges come from?
Conservation of:
What is happening?
Attaching a copper earthing wire to plane before refueling
Dangers
Dangers
Why are these surgeons wearing copper bands on their wrists?
There are 6 main points to make here.
Dangers
Why are these surgeons wearing copper bands?
There are 6 main points to make here.
Dangers
Dangers
Electric field
An area or region where a charge feels a force is called an electric field.
The electric field strength at any point in space is defined as the force per unit charge (on a small positive test charge) at that point.
E = F/q (in N C-1)
Electric field patterns
A field is a region of space where small positive test mass/charge feels a force
An electrical field is a region of space in which a small positive test charge experiences a force
Electric field patterns
The arrows show the direction of force that would be felt by a positive charge in the field
Electric field patterns
An electrical field is a region of space in which a small positive test charge experiences a force
Note: The direction of a field line in the electric field is the direction of the force on a small positive test charge.
(or from positive to negative if that is easier)
Shuttling Ball Experiment
Force
Coulomb found that the force between two point charges is proportional to the product of the two charges
and inversely proportional to the square of the
distance (r) between the charges
Example
k = 8.99 × 109 N m2 C-2
Elementary Charge = 1.60 × 10-19 C
How many electrons?
k = 8.99 × 109 N m2 C-2
Elementary Charge = 1.60 × 10-19 C
Coulomb’s law
The constant k is sometimes written as
where εo is called the permittivity of free space.
Permittivity
Permittivity changes relative to the substance
Relative Permittivity
IB might ask you about this: the higher the relative permittivity, the harder it is for electrostatic forces to travel over a distance…
Some examples of relative permittivities:
Permittivity
Sample question including ε0
A point charge of 4.5 × 10−8 C is situated in air 3.2 cm from another charge of –1.3 × 10−7 C.
a Determine the electrical force between them.
b If they were separated by polythene, calculate the approximate force between the charges.
Sample question including ε0
A point charge of 4.5 × 10−8 C is situated in air 3.2 cm from another charge of –1.3 × 10−7 C.
a Determine the electrical force between them.
b If they were separated by polythene, calculate the approximate force between the charges.
Answer
a F = –5.1 × 10–2 N
The negative sign represents an attractive force.
b Polythene has a relative permittivity of about 2, so the force would be divided by 2 (approximately), F ≈ −3 × 10−2 N.
Summary so far:
What is the force between two charges of 3.2 μC and 5.6 μC separated by a distance of 34 cm?
Using the relationships
What is the force between two charges of 3.2 μC and 5.6 μC separated by a distance of 34 cm?
Using the relationships
What is the force between two charges of 3.2 μC and 5.6 μC separated by a distance of 34 cm?
F = 1.4 N
Using the relationships
What is the force experienced by a charge of +6.3 μC placed at a point where the electric field strength is 410 NC-1?
Using the relationships
What is the force experienced by a charge of +6.3 μC placed at a point where the electric field strength is 410 NC-1?
Using the relationships
What happens if A is negative?
Try drawing this.
Combining charges and fields
Combining charges and fields
Electric field
Electric field is a vector, and any calculations regarding fields (especially involving adding the fields from more than one charge) must use vector addition.
Field here due to both charges?
q1
q2
Electric field
Electric field is a vector, and any calculations regarding fields (especially involving adding the fields from more than one charge) must use vector addition.
Field here due to both charges?
Field due to q1
q1
q2
Electric field
Electric field is a vector, and any calculations regarding fields (especially involving adding the fields from more than one charge) must use vector addition.
q1
q2
Resultant field
Field due to q1
Field due to q2
Combining charges and fields
Combining charges and fields
Charge is a scalar quantity, with the unit of C (Coulomb)
Coulomb’s Law cf Newton’s Gravitational law
Electric field strength cf gravitational field strength
Can you write electric field strength in terms of k, q and r?
Charge, a recap
Parallel
At right angles to the plates
Pointing from positive to negative (direction a positive test charge would travel)
Parallel plates and an electric field
If you move a test charge between the plates then work must be done:
W = Fd = Eq x d
Can you recall the definition of Potential Difference?
Energy in a uniform field
If you move a test charge between the plates then work must be done:
W = Fd = Eqd
Can you recall the definition of Potential Difference?
Work done per unit charge to move across a PD of V
Energy in a uniform field
Substitution and rearranging gives the field strength at any point between two plates, that are separated by a distance d
W = Fd = Eqd and V = W/q
Energy in a uniform field
The electric field strength E is the force per unit charge on a test charge placed at that point in the field (NC-1)
The formula for calculating the field strength between two parallel plates of separation d is:
Summary
Gravitational potential energy
Gravitational potential energy at a point is defined as the work done to move a mass from infinity to that point.
Ep is always negative
Electrical potential energy
Electrical potential energy at a point is defined as the work done to move a positive charge from infinity to that point.
Electrical Potential
The Electrical potential at a point is the work done per unit charge on a small positive test charge moving from infinity to that point. It is given by
Note the difference between electrical potential energy (J) and Electrical potential (J.C-1)
(a) what would happen to it?
(b) how much KE would it gain when it reached A?
Questions
This also defines an extremely important unit: the electronvolt
1eV = the energy one electron gains moving through a potential difference of 1V
W (J) = W (eV) x 1.6 x 10-19
Electron volts (as an aside)
Field and equipotentials
Equipotentials are always perpendicular to field lines. Diagrams of equipotential lines give us information about the gravitational field in much the same way as contour maps give us information about geographical heights.
Equipotential surfaces/lines
Field strength = gradient on a potential vs distance graph
Summary so far: