Work has the dimensional formula [M^1 L^2 T^-2].

Conventional current is defined as the flow of positive charge, which is from positive to negative.

The electric field due to a negative charge points towards the charge.

The electric field due to a positive charge points away from the charge.

The electric field lines point away from a positive charge.

According to Lenz's law, the induced current will flow in a direction that opposes the change, which is counterclockwise if the magnet is moved towards the coil.

According to Lenz's law, the induced current will flow in a direction that opposes the change in magnetic flux. If the magnetic field is increasing, the induced current will flow counterclockwise.

According to Lenz's law, the induced current will flow in a direction that opposes the change, so it will be counterclockwise if the magnetic field decreases.

The direction of the magnetic field around a current-carrying conductor is given by the right-hand rule, which indicates a counterclockwise direction when viewed from the positive current side.

According to the right-hand rule, if you point your thumb in the direction of the current, your fingers curl in the direction of the magnetic field lines, which is counterclockwise.

The direction of the magnetic field around a current-carrying wire is determined by the right-hand rule, which gives a clockwise or counterclockwise direction based on the current's direction.

Using the right-hand rule, if you point your thumb in the direction of the current, your fingers curl in the direction of the magnetic field, which is counterclockwise.

The direction of the magnetic field around a straight conductor carrying current is counterclockwise when viewed from the positive end of the conductor.

The direction of the magnetic field around a straight current-carrying conductor can be determined using the right-hand rule, which indicates that the field lines form concentric circles around the conductor in a counterclockwise direction when viewed from the positive end.

Using the right-hand rule, if the current flows in a counterclockwise direction when viewed from above, the magnetic field direction is out of the plane.

Using the right-hand rule, the magnetic field at the center of the loop is out of the plane.

The direction of the magnetic field inside a bar magnet is from the north pole to the south pole.

Using the right-hand rule, if the current flows in a counterclockwise direction, the magnetic field inside the loop points out of the plane.

The magnetic field inside a current-carrying solenoid is directed from the north pole to the south pole of the solenoid.

According to the right-hand rule, the magnetic field lines around a straight conductor carrying current are circular and lie in planes perpendicular to the conductor.

The magnetic field produced by a current-carrying loop at its center is perpendicular to the plane of the loop, following the right-hand rule.

Using the right-hand rule, the thumb points in the direction of current, and the fingers curl in the direction of the magnetic field.

According to the right-hand rule, if you point your thumb in the direction of the current, your fingers curl in the direction of the magnetic field.

The direction of the magnetic field produced by a current-carrying wire is perpendicular to both the wire and the direction of the current.

Using the right-hand rule, the magnetic field direction is counterclockwise around the wire.

The direction of the magnetic field produced by a current-carrying wire depends on the direction of the current, as determined by the right-hand rule.

For the equation y^2 = 4px, p = 5. The directrix is given by x = -p, which is x = -5.

The standard form of a parabola is (y - k)^2 = 4p(x - h). Here, p = 2, so the directrix is x = -2.

For the parabola y^2 = 4px, here 4p = 8, so p = 2. The directrix is x = -p = -2.

The discriminant is b² - 4ac = (-12)² - 4*3*12 = 144 - 144 = 0.