Construction of De Sauty Bridge
Let the variable resistors be R3 and R4 respectively. The standard capacitance is C2 and the unknown capacitance is C1. R3, R4, C1, and C2 are placed on four sides of a quadrilateral ABCD. We can place C1 on side AB, R1 on side BC, R4 on side CD and C2 on side AD of the quadrilateral. The galvanometer should be placed along the diagonal BD of the quadrilateral and the AC supply should also be placed along the other diagonal AC. The balanced condition can be obtained by varying the values of R3 and R4. The balance condition is independent of frequency. If either or both of the capacitors are imperfect or not free from dielectric losses, then the balance condition can be never obtained.
De Sauty Bridge
De Sauty Bridge is an AC bridge used to find the unknown capacitance in a circuit. French engineer Paul de Sauty invented it. De Sauty Bridge compares the unknown capacitance with another standard or known capacitor. It can also be used to compare the capacitors used in a circuit. De Sauty Bridge has a high degree of accuracy in measuring unknown capacitance over a wide range of capacitances. It works on the principle of null deflection. It is the simplest way to compare two pure(non-inductive) capacitors. The circuit design of the De Sauty Bridge is very simple and straightforward and the calculations are also simple. However, it can only measure capacitors that are free from dielectric loss. To overcome this disadvantage Grover modified the De Sauty Bridge by adding extra resistors.
Table of Content
- Defintion
- Working Principle
- Components
- Construction
- Formula
- Phasor Diagram
- Modified De Sauty Bridge
- Advantages and Disadvantages
- Application