MuffinMan
Juno 15/4/08 :)
Heres section 1 of the syllabus
* discuss the effect on the magnitude of the force on a current-carrying conductor of variations in:
– the strength of the magnetic field in which it is located
– the magnitude of the current in the conductor
– the length of the conductor in the external magnetic field
– the angle between the direction of the external magnetic field and the direction of the length of the conductor
Factors affecting the magnitude of the force depends on the following factors:
- The strength of the external magnetic field. The force is proportional to the magnetic field strength, B.
- The magnitude of the current in the conductor. The force is proportional to the current, I
- The length of the conductor in the field. The force is proportional to the length, l
The angle between the conductor and the external magnetic field.
The force is at maximum when the conductor is at right angles to the field, and is zero when the conductor is parallel to the field.
The magnitude of the force is proportional to the component of the field and the conductor. If θ is the angle between the field and the conductor, then the force is the maximum value multiplied by the sine of θ.
This can be expressed mathematically as:
BIl sin θ
[Ref: p100, Jacaranda HSC Physics, 2nd ed.]
*describe qualitatively and quantitatively the force between long parallel current-carrying conductors:
f a finite distance separates two parallel current-carrying conductors, then each conductor will experience a force due to the interaction of the magnetic fields that exists around each. The magnetic field strength at a distance, d, from a long straight conductor can be found using the formula
B = (kI)/d
Where k = 2.0 x 10-7 N A-2
The magnitude of the force experienced by the length, l, of a conductor due to the external magnetic field provided by another conductor is
F = I2l(kI1 / d)
[Ref: p101-103, Jacaranda HSC Physics, 2nd ed.]
define torque as the turning moment of a force using:
τ= Fd
A torque can be thought of as a turning effect of a force acting on an object. It is easier to rotate an object if the force, F, is applied at greater distance, d, for the pivot axis to its point of application. It is also easier to rotate an object if the force is at right angles to a line joining the pivot axis to the point of application.
The torque, τ, increases when the force, F, is applied at a greater distance, d, from the pivot axis. It is greater when the force is applied at right angles to the line joining the point of application of the force and the pivot axis. The SI unit for torque is the newton metre (N m), and is found using the equation:
τ = Fd sin θ
[Ref: p101-102, Jacaranda HSC Physics, 2nd ed.]
identify that the motor effect is due to the force acting on a current-carrying conductor in a magnetic field
A current carrying conductor produces a magnetic field. When the current-carrying conductor passes through an external magnetic field, the magnetic field of a conductor interacts with the external magnetic field and the conductor experiences a force. This effect was discovered by Michael Faraday (1791-1867) and is known as the motor effect.
The direction of the force on a current-carrying conductor in an external magnetic field can be determined using the right-hand push rule
*describe the forces experienced by a current-carrying loop in a magnetic field and describe the net result of the forces
The forces experienced by a current-carrying loop in a magnetic field depend on the orientation of the loop relative to the magnetic field. You will need to describe both the direction and the relative magnitude of particular forces, in addition to the net result of all forces.
Assume, for simplicity of discussion, that the axis of a rectangular coil is perpendicular to the magnetic field, and that the long sides of the coil are parallel to the axis and equidistant from it.
• Each long side of the coil experiences a force whose magnitude does not change throughout a rotation of the coil, since the sides always remain perpendicular to the field. The force on each long side can be shown, by the right-hand palm rule, to be always in the same direction throughout a rotation of the coil, opposite in direction to the force on the other long side, and always perpendicular to the axis.
• Each end of the coil will experience a force which varies from zero, when the plane of the coil is parallel to the field, to a maximum when the plane of the coil is perpendicular to the field. The forces on the two ends can be shown, by the right-hand palm rule, to be opposite in direction, always parallel to the axis, and alternating in direction through a full rotation of the coil.
• The force on each long side produces a torque about the axis. As the forces are in opposite directions, and their lines of action are on opposite sides of the axis, they produce a torque in the same direction. Thus, their effect is to rotate the coil about its axis. The net torque is at its maximum when the plane of the coil is parallel to the field, as the perpendicular distance, d, to the line of action is maximum, and reduces to zero as the plane of the coil rotates to be perpendicular to the field, as the line of action of each force is then through the axis (d = zero). The direction of the torque alternates through a complete rotation of the coil: its direction is always to rotate the coil to be perpendicular to the field.
• As the forces on the two ends are always opposite in direction, and always parallel to the axis, their net effect is zero.
• For any current-carrying loop in a magnetic field, free to rotate about any axis, the net effect of the forces will be such as to rotate the loop to lie perpendicular to the magnetic field. A current-carrying loop orientated in a plane at right angles to a magnetic field will experience no net force.
*describe the main features of a DC electric motor and the role of each feature
see attatchment
identify that the required magnetic fields in DC motors can be produced either by current carrying coils or permanent magnets
The magnetic field of a DC motor can be provided by permanent magnets, or by electromagnets. The permanent magnets are fixed to the body of the motor. Electromagnets can be created using a soft iron shape that has coils of wire around it. The current that flows through the armature coil can be used in the electromagnetic coils.
* discuss the effect on the magnitude of the force on a current-carrying conductor of variations in:
– the strength of the magnetic field in which it is located
– the magnitude of the current in the conductor
– the length of the conductor in the external magnetic field
– the angle between the direction of the external magnetic field and the direction of the length of the conductor
Factors affecting the magnitude of the force depends on the following factors:
- The strength of the external magnetic field. The force is proportional to the magnetic field strength, B.
- The magnitude of the current in the conductor. The force is proportional to the current, I
- The length of the conductor in the field. The force is proportional to the length, l
The angle between the conductor and the external magnetic field.
The force is at maximum when the conductor is at right angles to the field, and is zero when the conductor is parallel to the field.
The magnitude of the force is proportional to the component of the field and the conductor. If θ is the angle between the field and the conductor, then the force is the maximum value multiplied by the sine of θ.
This can be expressed mathematically as:
BIl sin θ
[Ref: p100, Jacaranda HSC Physics, 2nd ed.]
*describe qualitatively and quantitatively the force between long parallel current-carrying conductors:
f a finite distance separates two parallel current-carrying conductors, then each conductor will experience a force due to the interaction of the magnetic fields that exists around each. The magnetic field strength at a distance, d, from a long straight conductor can be found using the formula
B = (kI)/d
Where k = 2.0 x 10-7 N A-2
The magnitude of the force experienced by the length, l, of a conductor due to the external magnetic field provided by another conductor is
F = I2l(kI1 / d)
[Ref: p101-103, Jacaranda HSC Physics, 2nd ed.]
define torque as the turning moment of a force using:
τ= Fd
A torque can be thought of as a turning effect of a force acting on an object. It is easier to rotate an object if the force, F, is applied at greater distance, d, for the pivot axis to its point of application. It is also easier to rotate an object if the force is at right angles to a line joining the pivot axis to the point of application.
The torque, τ, increases when the force, F, is applied at a greater distance, d, from the pivot axis. It is greater when the force is applied at right angles to the line joining the point of application of the force and the pivot axis. The SI unit for torque is the newton metre (N m), and is found using the equation:
τ = Fd sin θ
[Ref: p101-102, Jacaranda HSC Physics, 2nd ed.]
identify that the motor effect is due to the force acting on a current-carrying conductor in a magnetic field
A current carrying conductor produces a magnetic field. When the current-carrying conductor passes through an external magnetic field, the magnetic field of a conductor interacts with the external magnetic field and the conductor experiences a force. This effect was discovered by Michael Faraday (1791-1867) and is known as the motor effect.
The direction of the force on a current-carrying conductor in an external magnetic field can be determined using the right-hand push rule
*describe the forces experienced by a current-carrying loop in a magnetic field and describe the net result of the forces
The forces experienced by a current-carrying loop in a magnetic field depend on the orientation of the loop relative to the magnetic field. You will need to describe both the direction and the relative magnitude of particular forces, in addition to the net result of all forces.
Assume, for simplicity of discussion, that the axis of a rectangular coil is perpendicular to the magnetic field, and that the long sides of the coil are parallel to the axis and equidistant from it.
• Each long side of the coil experiences a force whose magnitude does not change throughout a rotation of the coil, since the sides always remain perpendicular to the field. The force on each long side can be shown, by the right-hand palm rule, to be always in the same direction throughout a rotation of the coil, opposite in direction to the force on the other long side, and always perpendicular to the axis.
• Each end of the coil will experience a force which varies from zero, when the plane of the coil is parallel to the field, to a maximum when the plane of the coil is perpendicular to the field. The forces on the two ends can be shown, by the right-hand palm rule, to be opposite in direction, always parallel to the axis, and alternating in direction through a full rotation of the coil.
• The force on each long side produces a torque about the axis. As the forces are in opposite directions, and their lines of action are on opposite sides of the axis, they produce a torque in the same direction. Thus, their effect is to rotate the coil about its axis. The net torque is at its maximum when the plane of the coil is parallel to the field, as the perpendicular distance, d, to the line of action is maximum, and reduces to zero as the plane of the coil rotates to be perpendicular to the field, as the line of action of each force is then through the axis (d = zero). The direction of the torque alternates through a complete rotation of the coil: its direction is always to rotate the coil to be perpendicular to the field.
• As the forces on the two ends are always opposite in direction, and always parallel to the axis, their net effect is zero.
• For any current-carrying loop in a magnetic field, free to rotate about any axis, the net effect of the forces will be such as to rotate the loop to lie perpendicular to the magnetic field. A current-carrying loop orientated in a plane at right angles to a magnetic field will experience no net force.
*describe the main features of a DC electric motor and the role of each feature
see attatchment
identify that the required magnetic fields in DC motors can be produced either by current carrying coils or permanent magnets
The magnetic field of a DC motor can be provided by permanent magnets, or by electromagnets. The permanent magnets are fixed to the body of the motor. Electromagnets can be created using a soft iron shape that has coils of wire around it. The current that flows through the armature coil can be used in the electromagnetic coils.