6.3 Electromagnatism Flashcards
(27 cards)
Magnetic Field
A region where a force will act on a magnetic or charged material
What the closeness of field lines represents
The magnetic flux density
Direction of a magnetic field around a wire
Use right hand rule
A circle with a dot vs cross
dot - out of plane
cross - into plane
Solenoid
A long coil of current carrying wire
What causes a magnetic field
Moving charges or permanent magnets
When a force is induced by a magnetic field
When a current is perpendicular to a uniform field
Flemings left hand rule
First finger - field
seCond finger - current
thuMb - motion
Causes of a magnetic field (2)
- Moving charges
- Permanent magnets
Force on a current carrying conductor
F = BILsinθ
Experiment to determine magnetic flux density
Set up a wire between two permanent magnets and place the setup on some digital scales. Set the scales to 0. The circuit should contain a variable resistor and ammeter. Turn on the circuit and a downwards force will be produced causing a reading on the scales, note this down along with the current. Vary the resistance and repeat this. Plot a graph of F(=mg) against I and the gradient will be Bl so divide by l (length of magnets) to obtain the flux density
Force on a charged particle in a magnetic field
F = BQv
Motion of charged particles inside a uniform magnetic field
They will move in a circular path
How to calculate the radius of the circular path of a charged particle in a magnetic field
Equate centripetal force to the force from the magnetic field
How velocity selectors work
There is a magnetic field acting in an opposite direction to an electric field and charged particles are projected perpendicular to the direction of the fields. There is a small gap directly ahead and therefore to make it through the gap the force of the magnetic field must equal the force of the electric field.
EQ = BQv
E = Bv
v = E/B
Therefore only particles with a velocity of E/B will make it through
Magnetic flux
Magnetic flux density * perpendicular area
Magnetic flux linkage
Magnetic flux * number of coils
Faraday’s law
The induced e.m.f. is directly proportional to the rate of change of flux linkage
Gradient of a flux linkage - time graph
negative e.m.f.
Area under a e.m.f. - time graph
negative change in flux linkage
Lenz’s law
Induced e.m.f. will be in a direction to oppose the change that caused it
So whats the big idea with why you can move straight wires in a field and get emf but when you move a coil you dont
Perhaps because its round so the emf would go both ways and cancel itself out who knows
Experiment to investigate link between e.m.f. and flux linkage
Place a search coil between two magnets. The search coil should be connected to a data recorder which will record the induced e.m.f. with a very small time interval. Move the coil out of the field and look at the graph. The area under the e.m.f-time graph should be equal to the magnetic flux linkage. So you can then find B from this (youll need to measure area and number of coils e.t.c.)
Components of an A.C. generator (4)
- Magnets
- Coil
- Slip rings
- Brushes