Skip to main content

Potential due to dipole

 Electrostatic potential due to positive charge is q/4πεₒr and physically it requires work to bring another charge at position r to overcome the force of attraction. If unsupported the charge thus brought will be repelled and accelerated away. Similarly, for a negative charge, the potential is given by  (-q)/4πεₒr and it means that we need to prevent a positive test charge from bumping into the negative charge. If unsupported, the negative charges will be attracted and accelerated towards the negative charge. 

A dipole has positive and negative charges of the same magnitude separated by a certain distance which is of the order of angstrom. At the center of the dipole, there is zero potential. The potential of a dipole is zero if the point happens to be equidistant from the positive and the negative charges. So, for a point on the perpendicular bisector, the potential is always equal to zero. However, it will be influenced by either of the charges if the point is closer to them. We generally try to find the potential due to dipole at a general point that is far away from both the positive and negative charges as well as from the center of the dipole. 

For finding the dipole at any point P,  we mark the positions of the positive and negative charge, the position vector of the point from the center of the dipole, and the angle between the position vector and dipole moment. Thereafter, we add the potentials due to the positive and negative charges and use Cosine law and Binomial expansion to get the final expression of Vdiple =P.r/4πεₒr2. 

The electric field bears a very good relationship with potential. Mathematically, the electric field is negative of the potential gradient. By using calculus, we can show that E = -dv/dr. Similarly, by using equipotential points and surfaces, we can show that the electric field always goes in the direction of decreasing potential. 

Finally, we winded up the class by creating a system of charges. We discussed that to create a system of charges in a space we need to do work if there is more than one charge. 








Comments

Popular posts from this blog

Grade 11 - Engineering Graphics Syllabus

 

Isometric Scale

 An isometric scale is used for isometric projection. Most of the drawings on a plain sheet of paper are 2-dimensional. We can use three axes at 120o with each other to indicate three dimensions of an object. This generally helps in creating 3-dimensional drawings on a 2D plane.  CBSE Class 12 has isometric scale construction as an essential construction skill.  The steps of construction are as follows; (1) Draw a horizontal line.  (2) Draw an inclined line at 45o with east which is the default 0o.  (3) Using your roller, divide the given true length on the inclined line. If you have to draw an isometric scale of 70 mm, then draw the line of up to 80.  (4) Keep the first 1 cm for dividing into 10 equal parts of  1 mm. Thereafter, divide the length into the required number of equal parts.  (5) Draw another line at 30; with default east.  (6) Draw a vertical line at 30.  (5) Take the height of the line as 4 mm and complete the scale. ...

Grade 12 Chapter 2 : Electrostatic Potential and Capacitance

 Chapter 2: Electrostatic Potential and Capacitance.  Starting from the concept of electrical work, we establish the concept of electrostatic potential energy. This energy per unit charge is defined as the electric potential. We obtain an expression for the potential of a source charge by bringing a unit test charge from infinity to a location in the space. Similarly, using the geometry, we can find the potential due to the dipole.  Moreover, we can relate the electric field and the potential also. Usually, the electric field is taken as the negative of the potential gradient.  To create a system of charges, we have to spend some energy and this will be stored as the potential energy of the system. The same logic can be extended for rotating a dipole in an external field. Here also, by doing work against the net torque of the uniform external field, we can store the energy in the dipole.  A very interesting point of discussion in Chapter 2 is related to the elec...