WHEATSTONE BRIDGE

WHEATSTONE BRIDGE

I - Goal :

The goal of this manipulation is to determine the value of an unknown resistance using the Wheatstone bridge and the wire bridge.

II - Theoretical reminders :

    II-1- Wheatstone Bridge :

The Wheatstone bridge consists of an electrical circuit comprising three known resistances and a fourth to be determined, powered by a direct current generator E.

Consider then the circuit below, where R1 and R2 are resistors of known ratio, RV is a known adjustable resistance (rheostat) and RX is the unknown resistance. All of these resistances thus form the so-called Wheatstone bridge. The two points C and D are connected to a galvanometer G.


To determine the value of the unknown resistance RX, it is necessary to adjust the variable resistance RV in the bridge until we manage to cancel the intensity of the current in the branch CD of the bridge.

Therefore, by acting on the resistors R1, R2 and RV it is possible to cancel the current in the galvanometer.

In this case, we can write :   

   

      This makes it possible to apply Ohm's law to the terminals of R1 and R2  :

  

from where :          

          

On the other hand :     


Thus :      

           

At the Equilibrium of the bridge, we obtain the relation :

Note that it is useless to know the resistances R1 et R2 ; only their report intervenes 

This report is called beachhead report.

      II-2- Wire bridge :

The wire bridge is another variant of the Wheatstone bridge. We know that for a homogeneous conducting wire, the resistance is proportional to the length. We can replace R2 and RV by a wire AB (of length L, section S and resistivity ρ) along which a cursor D moves.


In equilibrium, we can write, taking into account the relationship (1)


Where:

RAD  is the resistance of the wire of length  L1=AD :


RDB  is the resistance of the wire of length  L2=DB :


By replacing these two values in equation (2), we obtain :




Modifié le: mardi 18 mars 2025, 16:22