To understand how we can control the strength and orientation of electric fields using the bond axis, it is important first to understand what it means in the context of electrical engineering. An electric field is simply a field produced by an electric source, which in this case is the electric charge of an object.

One approach to controlling the strength of an electric field on the Bond axis is the application of a mechanical force or magnetic field. The simplest form of a mechanical force is the static or rotational force. In this case, the only variable is the amount of rotation the force produces, and it is this type of force which give us our rotational control. There is however another type of mechanical force, which is the dynamic force, which can be used for the same purposes.

Another type of force that can be applied to manipulate the strength of the electric field is the electrostatic force. The effect of this force is basically the same as that of the static force described above, except that the forces are not constant across the length of the electric field. The electrostatic force is normally measured in an electrostatic field. The last example above is of course for one single set of orthogonal p orbitals, while the second example shows the effect of the destructive or constructive interference of the opposing p orbitals together.

The concept of using the bond axis to control the strength of electric fields is quite simple in principle. It requires, however, a set of electric source, such as a magnet, that produces a force perpendicular to the a axis, and which creates an electric field. The force is then used to deflect an electric field from the p axis away from the a axis, so that it moves along the a axis. However, there are a few considerations to make in order to get the best results.

First of all, the force must be produced parallel to the a axis, or else the force will deflect the charge away from the a axis and back to the p axis where it will again produce an electric field perpendicular to the a axis. This problem is particularly important with the static force, since the static force only produces a single force, not multiple forces of which each one deflects the charge back and forth. in a very predictable manner.

Secondly, it is important to note that in general, the force used in controlling the strength of the electric field must be in the same direction as the magnetic field, or else the electric field would deflect the charge back into the magnetic field, thus producing an alternating current. {in which the charge would be trapped. {in order to be moved back to its initial position. The problem with the static force also exists with the constructive interference, where the force deflects the electric field away from the a axis and therefore the charge cannot be moved back to the p axis, but instead stays where it is.

Finally, it is important to note that the destructive interference occurs because the charges have an alternative route. As soon as the magnetic field has been produced, a magnetic field appears, which is known as the negative field. This is due to the attraction of opposite charge particles, which cancel the effect of the positive charge by the electric field, and a repulsive force exists between the positive and negative charge particles.

As soon as the negative charge particle moves towards the p axis, the magnetic force cancels the positive charge. This repulsive force causes the magnetic field to move towards the p axis, and the electric field moves into the magnetic field, creating the opposite magnetic field, and therefore cancels the repulsive force. thus canceling the force.