Verification of Compensation Theorem            

Theory

In a linear time invariant network when the resistance `(R)` of an uncoupled branch, carrying current (I), is changed by ΔRL , the currents in all the branches would change and can be obtained by assuming that an ideal voltage source of Vc has been connected such that Vc=IΔRL in series with R+ΔRL when all other sources in the network are replaced by their internal resistances.


Explanation :  

Let us assume a load `R_L` connected to a dc source network whose thevenin's equivalent gives Vo as the Thevenin's voltage and RTh as Thevenin resistance.



[ Fig. 1. Thevenin Equivalent Circuit ]



[ Fig.2 (a) . Explanation of Compensation theorem ]


[ Fig.2 (b) . Explanation of Compensation theorem ]

Let the load resistance Rl be changed to R+ΔRL.Since the rest of the circuit remains unchanged,the Thevenin equivalent network remains the same.This Change of current being termed as ΔI , we find


$$\Delta I = I' - I$$

     $$= \frac{V_o}{(R_{Th} + R_L + \Delta R_L)} - \frac{V_o}{(R_{Th} + R_L)}$$


     $$= \frac{V_o (-\Delta R_L)}{(R_{Th} + R_L)(R_{Th} + R_L + \Delta R_L)}$$


     $$= -\frac{V_c}{R_{Th} + R_L + \Delta R_L} .......(3)$$


$$V_c = I \Delta R_L$$

This voltage Vc is termed as compensating voltage.