^Power transferred theorem
Power transferred theorem
The power transferred by a cell to the load is maximum when R = r & given by


Also then 
Power transferred theorem
The power transferred by a cell to the load is maximum when R = r & given by


Also then 
Series combination of resistors
The current across each circuit element is same, but potential difference is different & proportional to resistance of that part.
i.e. I = I1 = I2 = I3 & V1 = IR1, V2 = IR2, V3 = IR3 & R series = R1 + R2 + R3
Electric resistance
Depends upon the nature of material, shape & size, physical state like temperature, pressure, type & extent of impurity etc. of conductor. However r depends upon all above factors except on shape & size.

Series dielectrics in a capacitor
If three dielectric slabs of thickness t1, t2 & t3, dielectric constants K1, K2 & K3 are placed between the plates of a parallel plate capacitor as shown, then the combination behaves as different dielectrics dividing the spacing are considered as capacitors connected in series.

Capacitance of this is given by



Energy (potential) stored in a capacitor
A charged capacitor of any shape or size stores energy (potential) in the form of electrostatic electric field, it is given by

Energy per unit volume is called energy density, it is Electric energy density,

^What is a ratio?
If a physical quantity can be completely described just by knowing its only numerical value, no unit & direction is required, then it is called ratio.
e.g. Strain, Poisson’s ratio, refractive index, relative density, relative permittivity, relative permeability, fine structure constant etc.
Facts
Relative velocity have same dimensions as that of velocity where as relative density is dimensionless.
Parallel plates with different charges
If the two parallel metal plates X & Y having charge q1 & q2 are placed close to each other. Let the medium between the plates is air or vacuum. then in order to make net electric field in each plate zero, charges redistribute such that inner faces have equal & opposite charges & extreme faces have equal & of same sign as shown below

Elec. field on the left side (L) of plates, right side of plate (R) & between the plates due to the charge on face a, b, c & d is

Field due to sheets
Using Gauss law we can prove that electric field sheets of charge density σ
1.
near a infinite sheet or thick sheet
2.
near a finite sheet or thin sheet
^Rules for writing units
In calculations the prefix is attached with the numerator and not with the denominator.