Ohm’s Law Derivation Class 12 Physics: Formula, Vector Form, Applications and Limitations

 

Deduction of Ohm’s Law


We know that the relation between drift speed and electric current is 


        `I = n A e v_d`


        `frac{I}{A} = n  e v_d`


        ` J = n  e v_d`                 


Where J is the current density.


Also,


        `v_d = frac{e tau}{m}E`


Substituting the value of `v_d` in the above equation,


        ` J = n  e   frac{e tau}{m}  E`


        ` J =   frac{n  e^2   tau}{m}  E`


    Here, m and e are constant, while n and `tau` are the characteristics of the conductor. 


    For a homogeneous conductor, frac{n  e^2   tau}{m}  ` is constant. It is called the conductivity `sigma` of the material.


Thus,


        ` J =   sigma  E`


In vector form,


        ` vec J =   sigma  vec E`


    This equation is the microscopic form or vector form of Ohm’s law.


    Consider a conductor having a length of `l` and a cross-sectional area A.


Now we know that 


        ` J =   sigma  E`


Using,


        `J = frac{I}{A}`


and


        `E = frac{V}{l}`


we get,


        ` frac {I}{A} =   sigma  frac{V}{l}`


        ` V = frac{1 }{ sigma}frac {l}{A} I`


Since,


        `rho = frac{1}{sigma}`


therefore,


        ` V = rho  frac {l}{A} I`


        ` V =  frac {rho  l}{A} I`


But,


        `R = frac{rho l}{A}`


Hence,


        ` V =  R I`


    This is Ohm’s law.


Where,


        `rho = frac {1}{sigma}=` Resistivity


        ` sigma =` Conductivity


        `E = frac {V}{l} = `electric field inside the conductor.


Microscopic and Macroscopic Forms of Ohm’s Law


Microscopic form


        `vecJ = sigma vec E`


Macroscopic form


        `V = I R`


Limitations of Ohm’s Law


Non-Linear Devices

        Semiconductors, diodes, and transistors do not strictly follow Ohm’s law. These devices exhibit non-linear behavior and are called non-ohmic devices. The graph between voltage (V) and current (I) is not a straight line.


Heating effect due to High Current


    If a large current flows through a conductor. According to `H = I^2 R t`. Due to heating, the resistance of the conductor increases. Therefore, instead ofobtaining a straight-line graph between V and I, a curved graph is obtained.

Temperature-Dependent Resistance


    Ohm’s law is not applicable at very high temperatures because the resistance of a conductor changes with temperature.


Applications of Ohm’s Law in Electrical Circuits


Series Circuits 


    In a series combination of resistors, the current remains the same through each component, while the voltage is distributed among them.


Parallel Circuits


    In a parallel combination of resistors, the voltage remains the same through each component, while the current is distributed among them.


Mixed Circuits


    In a series-parallel mixed combination of resistors, Ohm’s law is used to find branch currents, total resistance, and voltage drops.


Conditions for Ohm’s Law to be Valid


  • The temperature should remain constant
  • Physical dimensions should not change
  • Applicable only for Ohmic materials
  • Constant Physical State

Other Applications


1.    Electrical fuse ratings.

2.    Power consumption calculations.

3.    Fan speed regulation.

4.    Resistor selection.

5. Determinations of voltage, resistance, and current in circuits.

V-I Graph of Ohmic and Non-Ohmic Conductors


  • Straight line for ohmic conductors

  • Curved graph for non-omic devices


Ohm’s Law Solved Example


    The resistance of an electric coil is 60 Ω, and a current of 3.2 A flows through it. Find the potential difference between two points.


Solution


Using Ohm’s law,


        `V = R I`


        `V = 60 times 3.2`


        `V = 192 V`


Hence, the voltage across the coil is 192 V.