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Topic 9.3 
3.1.1 – The Motor Effect
Magnetic Field Direction 
● The direction of a magnetic field is defined to 
be the direction that a small North monopole 
(assuming one existed) would move if place in 
the field. 
● Magnetic field lines always point away from North 
and towards South and do not cross.
Magnetic Field Strength 
● The strength of a magnetic field is indicated by 
how close together the lines of flux are. 
● For this reason, the strength of the magnetic 
field B is known as the magnetic flux density. 
● B is measured in Teslas (T) 
● 1 Tesla is the strength of the magnetic field when a 
charge of 1C feels a force of 1N when moving with 
a velocity of 1ms-1 perpendicular to the field. 
● B measures the strength of the magnetic field 
as it is observed externally to the system.
Electric Charge and Magnetism 
● A moving charge creates a small magnetic field 
around it. 
● The magnetic field around a wire forms a 
circular field around the axis of motion. 
● The magnetic flux density gives an indication of 
how close together the lines of magnetic force 
are and hence the strength of the magnetic 
field.
Magnetic field around a current 
carrying wire 
● A current is simply a flow of 
charged particles. 
● Therefore, the magnetic field 
around a long straight current 
carrying wire is cylindrical 
around the axis of the wire. 
● The direction of the field is 
given by the right hand 
thumb rule.
Right hand Thumb Rule 
● Grab the wire in your 
right hand 
● Point your thumb in 
the direction of the 
current. 
● Your fingers curl in 
the direction of the 
magnetic field.
Magnetic Fields around Current 
Carrying Wires 
● Current Into Page ● Current Out Of Page
Forces on Wires 
● A current passing through a 
wire will generate a magnetic 
field around it. 
● If this wire is placed inside a 
magnetic field then the two 
magnetic fields will interact. 
● This will cause a force. 
● This is known as the motor 
effect. 
● Consider the diagram below. 
● A current I flows in the wire 
through a region of uniform 
magnetic field into the page (B) 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
I 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + B +
Forces on Wires 
● The current creates a 
circular magnetic field 
around it (Red) 
● According to the right 
hand grip rule, the 
field is out of the page 
above the wire, and 
into the page below it. 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
· · · I · · · · · · · · 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + B +
Forces on Wires 
● The additional +'s below the line 
increase the local field strength in 
this region. 
● The · and + cancel out above the 
wire decreasing the strength of the 
local field. 
● There is therefore a thrust force 
(FT) upwards on the wire as the 
field pushes the wire to try to 
balance out the local changes. 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + B + 
FT 
· · · I · · · · · · · · 
+ + + + + + + + + + +
Forces on Wires 
● Looking at exactly the 
same situation but end on 
to the wire (from the Left 
hand end) gives the 
diagram shown. 
● Note how the fields above 
the wire cancel out and 
below reinforce. 
● This induces a force 
upwards on the wire. 
FORCE 
S + N
The Left Hand Motor Rule. 
● The left hand rule is 
used to determine the 
direction of the motor 
effect force for a 
conventional current. 
● First finger = Field 
● seCond finger = Current 
● Thumb = Thrust
The Right Hand Palm Rule 
● The right hand palm 
rule is also used to 
determine the 
direction of the motor 
effect force for a 
conventional current. 
● Fingers = Field 
● Thumb = Current 
● Palm Slap = Force
Forces on Wires 
● It is interesting to note that 
the force is perpendicular 
to both the current and 
magnetic field. 
● This implies that the 
direction of the Force is 
given by the cross product 
of the current and 
magnetic field vectors. 
● i.e. 
● 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + B + 
FT 
· · · I · · · · · · · · 
+ + + + + + + + + + + 
⃗F ∝⃗I×⃗B
Factors affecting the Force 
● There are 4 factors that effect the magnitude of 
the force on the current carrying wire: 
● The strength of the 
magnetic field 
● The magnitude of the 
current 
● The length of the 
conductor in the field 
● The angle between the 
field and the conductor 
● A stronger field means more 
flux lines means more force. 
● A larger current means more 
flux lines means more force. 
● A longer conductor means 
more flux lines means more 
force. 
● The angle controls the magnitude of the 
component of the length in the field. A 
bigger angle means a smaller component 
means less force.
Forces on Wires 
● For a wire of length L in 
a uniform magnetic field 
this becomes: 
● Where θ is the angle 
between the current and 
the normal to the plane 
of magnetic field. 
Note: In the diagram below, the 
wire has been turned out of the 
page and not turned in the plane 
of the page. 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + + + 
+ + + + + + + + + B + 
· · 
T 
· · F· · · + + 
· · + + · · I + + + + + + + ⃗F=L⃗I×⃗B 
⃗F=LIBsinθ 
θ
Forces on Charged Particles 
● A current is simply a flow of charge carriers in a wire. 
● Each has a charge of q and an average speed of v covering a distance of L 
in 1 second. 
● The current due to a simple charge is therefore given by: 
⃗I= 
q⃗v L 
● The force on a moving charge therefore is given by: 
⃗F=q⃗v 
×⃗B 
⃗F=qvBsinθ 
● Here θ is the angle between the B field line and the velocity of the charge.
Parallel Wires 
● It follows that if two 
parallel conducting 
wires are carrying 
currents next to each 
other that: 
● They will both induce 
magnetic fields 
● They will both interact 
● They will both feel an 
equal force. 
+ 
FORCE 
+
Parallel Wires 
● If the two wires are 
carrying currents in 
the same direction 
(parallel) then: 
● The fields between 
them cancel out 
● The fields outside 
therefore push them 
together equally. 
● Parallel current attract 
+ 
FORCE 
+ 
FORCE
Parallel Wires 
● If the two wires are 
carrying currents in the 
opposite direction 
(anti-parallel) then: 
● The fields between 
them cancel reinforce 
● The fields inside 
therefore push them 
outwards equally. 
● Anti-Parallel currents 
Repel 
+ 
FORCE 
. 
FORCE
Parallel wires 
● The magnitude of the force per unit length on 
parallel conducting wires is given by: 
F 
l =k 
I1 I 2 
d 
● A positive answer indicates attraction, a 
negative answer indicates repulsion.

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3.1.1 the motor effect

  • 1. Topic 9.3 3.1.1 – The Motor Effect
  • 2. Magnetic Field Direction ● The direction of a magnetic field is defined to be the direction that a small North monopole (assuming one existed) would move if place in the field. ● Magnetic field lines always point away from North and towards South and do not cross.
  • 3. Magnetic Field Strength ● The strength of a magnetic field is indicated by how close together the lines of flux are. ● For this reason, the strength of the magnetic field B is known as the magnetic flux density. ● B is measured in Teslas (T) ● 1 Tesla is the strength of the magnetic field when a charge of 1C feels a force of 1N when moving with a velocity of 1ms-1 perpendicular to the field. ● B measures the strength of the magnetic field as it is observed externally to the system.
  • 4. Electric Charge and Magnetism ● A moving charge creates a small magnetic field around it. ● The magnetic field around a wire forms a circular field around the axis of motion. ● The magnetic flux density gives an indication of how close together the lines of magnetic force are and hence the strength of the magnetic field.
  • 5. Magnetic field around a current carrying wire ● A current is simply a flow of charged particles. ● Therefore, the magnetic field around a long straight current carrying wire is cylindrical around the axis of the wire. ● The direction of the field is given by the right hand thumb rule.
  • 6. Right hand Thumb Rule ● Grab the wire in your right hand ● Point your thumb in the direction of the current. ● Your fingers curl in the direction of the magnetic field.
  • 7. Magnetic Fields around Current Carrying Wires ● Current Into Page ● Current Out Of Page
  • 8. Forces on Wires ● A current passing through a wire will generate a magnetic field around it. ● If this wire is placed inside a magnetic field then the two magnetic fields will interact. ● This will cause a force. ● This is known as the motor effect. ● Consider the diagram below. ● A current I flows in the wire through a region of uniform magnetic field into the page (B) + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + I + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + B +
  • 9. Forces on Wires ● The current creates a circular magnetic field around it (Red) ● According to the right hand grip rule, the field is out of the page above the wire, and into the page below it. + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + · · · I · · · · · · · · + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + B +
  • 10. Forces on Wires ● The additional +'s below the line increase the local field strength in this region. ● The · and + cancel out above the wire decreasing the strength of the local field. ● There is therefore a thrust force (FT) upwards on the wire as the field pushes the wire to try to balance out the local changes. + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + B + FT · · · I · · · · · · · · + + + + + + + + + + +
  • 11. Forces on Wires ● Looking at exactly the same situation but end on to the wire (from the Left hand end) gives the diagram shown. ● Note how the fields above the wire cancel out and below reinforce. ● This induces a force upwards on the wire. FORCE S + N
  • 12. The Left Hand Motor Rule. ● The left hand rule is used to determine the direction of the motor effect force for a conventional current. ● First finger = Field ● seCond finger = Current ● Thumb = Thrust
  • 13. The Right Hand Palm Rule ● The right hand palm rule is also used to determine the direction of the motor effect force for a conventional current. ● Fingers = Field ● Thumb = Current ● Palm Slap = Force
  • 14. Forces on Wires ● It is interesting to note that the force is perpendicular to both the current and magnetic field. ● This implies that the direction of the Force is given by the cross product of the current and magnetic field vectors. ● i.e. ● + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + B + FT · · · I · · · · · · · · + + + + + + + + + + + ⃗F ∝⃗I×⃗B
  • 15. Factors affecting the Force ● There are 4 factors that effect the magnitude of the force on the current carrying wire: ● The strength of the magnetic field ● The magnitude of the current ● The length of the conductor in the field ● The angle between the field and the conductor ● A stronger field means more flux lines means more force. ● A larger current means more flux lines means more force. ● A longer conductor means more flux lines means more force. ● The angle controls the magnitude of the component of the length in the field. A bigger angle means a smaller component means less force.
  • 16. Forces on Wires ● For a wire of length L in a uniform magnetic field this becomes: ● Where θ is the angle between the current and the normal to the plane of magnetic field. Note: In the diagram below, the wire has been turned out of the page and not turned in the plane of the page. + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + B + · · T · · F· · · + + · · + + · · I + + + + + + + ⃗F=L⃗I×⃗B ⃗F=LIBsinθ θ
  • 17. Forces on Charged Particles ● A current is simply a flow of charge carriers in a wire. ● Each has a charge of q and an average speed of v covering a distance of L in 1 second. ● The current due to a simple charge is therefore given by: ⃗I= q⃗v L ● The force on a moving charge therefore is given by: ⃗F=q⃗v ×⃗B ⃗F=qvBsinθ ● Here θ is the angle between the B field line and the velocity of the charge.
  • 18. Parallel Wires ● It follows that if two parallel conducting wires are carrying currents next to each other that: ● They will both induce magnetic fields ● They will both interact ● They will both feel an equal force. + FORCE +
  • 19. Parallel Wires ● If the two wires are carrying currents in the same direction (parallel) then: ● The fields between them cancel out ● The fields outside therefore push them together equally. ● Parallel current attract + FORCE + FORCE
  • 20. Parallel Wires ● If the two wires are carrying currents in the opposite direction (anti-parallel) then: ● The fields between them cancel reinforce ● The fields inside therefore push them outwards equally. ● Anti-Parallel currents Repel + FORCE . FORCE
  • 21. Parallel wires ● The magnitude of the force per unit length on parallel conducting wires is given by: F l =k I1 I 2 d ● A positive answer indicates attraction, a negative answer indicates repulsion.