Magnetic field due to a current in a solenoid , Force on a current-carrying conductor in a magnetic field, Fleming’s left hand rule, electromagnet
Magnetic field due
to a current in a solenoid
Solenoid:--
Solenoid is a coil of
many circular turns of insulated copper wire which are wrapped closely in the
shape of a cylinder is called a solenoid.
Magnetic field
lines of the magnetic field near current carrying solenoid.
A solenoid having
current is used to magnetise the rod inside it
The magnetic field
around the current carrying solenoid is similar to the magnetic field around
the bar magnet.
One end of the solenoid
behaves as (or act as) magnetic north pole
Other end of the
solenoid behaves as (or act as) the
magnetic south pole.
In the solenoid , The magnetic field lines are In the form of the parallel straight
lines. This shows that magnetic field is
same at every points insides the solenoid. That is , the magnetic field is
uniform inside the solenoid.
A electromagnet consists of a core of soft iron wrapped with a coil
of insulated copper wire
When s current is
flowing through a solenoid , a strong magnetic field is produced inside a
solenoid which can be used to magnetise a piece
of magnetic material (like soft iron ) when placed inside the coil . the
magnet so formed is called as electromagnet.
Force on a
current-carrying conductor in a magnetic field
An electric current is
flowing through a conductor produces a magnetic field. The produced magnetic
field exerts a force on a magnet placed near to the conductor.
A rod AB having
current exerts a force which is perpendicular to its length and magnetic field.
To demonstrate the
force due to a magnetic field acting on the current carrying conductor ,
assume a small aluminium rod is
connected with two connecting wires and its suspended freely horizontally from
a stand.
Now take a strong horse
shoe magnet. And place the strong horse shoe magnet in such a manner that the
rod is kept between the two poles with the magnetic field directed upwards.
For this, the north
pole of the magnet is put vertically below the aluminium rod . And south pole
of the magnet is put vertically above the aluminium rod.
Now to make the circuit
connections, connect the aluminium rod In series with a battery , a key and a
rheostat.
Now , the electric
current is passed through the aluminium rod from end B to end A.
After that we observed
that the rod gets displaced. The rod is now displaced towards the left.
Now , if we reverse the
direction of the current flowing through rod and we get the direction of the
rod move toward the right direction.
By doing this , we
observes the displacement of the rod
explain that the current carrying
aluminium rod is placed in a magnetic field , a force is being exerted.
It also suggests that
when the direction of the current
passing through the conductor is
reversed , then the direction of the
force is also reversed.
Now, if we change the
direction of the magnetic field to vertically downwards by interchanging both
two poles of the magnet. Then we observed that the direction of the force acting
on the current carrying rod gets reversed.
This show that
direction of the force on the conductor is depends on the direction of the
current and direction of the magnetic field.
Also , we observed that
the when the magnitude of the force is more , when the direction of the current
is at right angles to the direction of the magnetic fields.
Fleming’s left
hand rule:--
Consider that the
direction of the current and that of the magnetic field is perpendicular to
each other and found the force is also perpendicular to both of them.
These three directions
can be explained by the simple rule. that rule is called as fleming’s left hand
rule.
According to the
fleming’s left hand rule, stretch the thumb , forefinger and middle finger of
your left hand in a such a manner that they are mutually perpendicular to each
other. If the first finger is pointing in the direction of the magnetic field and second finger is pointing in the direction of the
current , then the thumb will points in the direction of the
motion or the force acting on the conductor.
This rule is used to
find the direction of the force on the conductor.
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