In this article, we will discuss Anderson’s Bridge in electrical measurement. Here, we will cover the circuit diagram, equation, phasor diagram, and advantages and disadvantages of Anderson’s Bridge.

**What is Anderson’s Bridge?**

In electrical measurement, Anderson’s Bridge is a circuit that is used to determine the self-inductance of the circuit. It is a type of AC (alternating current) bridge. Anderson’s Bridge for the measurement of inductance is one of the most common and best bridges for precise measurement of inductance over a wide range. In the case of Anderson’s bridge, the self-inductance is measured in terms of a standard capacitor.

Anderson’s bridge is basically a modified form of Maxwell’s bridge that is used for the measurement of self-inductance of low Q coils(Q<1). The key difference between Anderson’s bridge and Maxwell’s bridge is that Anderson’s bridge uses a fixed capacitor instead of a variable capacitor. Therefore, Anderson’s bridge gives more accurate results as compared to Maxwell’s bridge.

**Circuit Constructions of Anderson’s Bridge **

The circuit diagram of Anderson’s bridge is shown in Figure 1.

It consists of four arms namely *ab, bc, cd, da*. The circuit arrangement of Anderson’s bridge is as follows-

- An unknown inductance is connected between the terminals
*a*and*b*along with a resistance*R*is connected in series with this unknown inductance._{1} - A fixed capacitor
*C*is connected between the terminals c and e. - A variable resistor
*r*is connected between the terminals e and d. - An alternating voltage source is connected between terminals a and c.

**Equation of Anderson’s Bridge**

In the circuit of Anderson’s Bridge, let,

At the balance condition of the bridge, we have,

And,

Now, the voltage across R and capacitor C is equal and no current flows through the galvanometer.

VBC = VCE

Therefore,

Another balance equations of the bridge are,

**The voltage across AB = Voltage across AD + Voltage across DE**

The voltage across VDE + voltage across VEC= Voltage across VDC

Now, on substituting the value of *I _{C}* from equation(1) in equations (2) we get,

Now, on substituting the value of *I _{C}* from equation(1) in equations (3) we get,

On substituting the value of I_{2} from equation(5) in equation (4), we get,

On separating the real and imaginary parts of equation (6), we get,

And,

Hence, using equation (8), we can determine the value of the self-inductance of the coil.

**Phasor Diagram of Anderson’s Bridge **

The current I_{1} is flowing through arm AB i.e., through non-inductive resistance R_{1} and inductor L_{1}. Thus the total drop V_{1} in arm AB is the vector sum of I1 (R1 + r1) (which is in phase with I1) and I1 ωL1 (which is 90 degrees lagging with I_{1}).

The same current will also pass through R_{3} (in arm BC) i.e., I_{1} = I_{3} when the bridge is balanced. Therefore, the voltage drop I3 R3 ( V3) is in phase with current I1. The potential between junctions BC will be equal to the potential between junctions EC because no current flow through the galvanometer under bridge-balanced conditions. Therefore, the voltage drop V_{3} = I_{c}/ωC and the voltage drop I_{c} r in the resistor r will lie along with I_{c}.

Voltage V_{4} will be equal to V_{EC} when the potential across the galvanometer is zero under bridge-balanced conditions. Thus, V4 is the sum of the voltage drop across resistor r, and V_{EC}. Thus, voltage V_{4} is the sum of voltage drop I_{c} r and V_{3}.

The current I_{2} is the sum of the currents I_{c} and I_{4} under bridge balanced conditions. Therefore, the drop V2 ( I2 R2) in the arm AD due to I_{2} lies along with it. Therefore, the

The current I_{2} is the sum of the currents I_{c} and I_{4} under bridge balanced conditions. Therefore, the drop V_{2} ( I_{2} R_{2}) in the arm AD due to I2 lies along with it. Therefore, supply voltage V is the resultant of the phasors V1 and V3 or V2 and V4.

**Advantages of Anderson’s Bridge**

The following are the major advantages of Anderson’s bridge-

- Anderson’s bridge determines the value of self-inductance more accurately.
- Anderson’s bridges require a standard fixed capacitor instead of a variable capacitor.
- In Anderson’s bridge, the bridge balance point can be easily obtained.
- A fixed capacitor is used in place of a variable capacitor in Anderson’s bridge. Hence, the bridge is cheaper than Maxwell’s bridge.
- It is possible to determine the value of unknown capacitance in terms of known inductance.
- The calculation of self-inductance of the coil does not get affected even with the use of an imperfect capacitor. The imperfect capacitor only affects the value of coil resistance.
- We need to subtract the lead wire inductance from the calculated inductance value for more precise measurements. Therefore, we can get the second balance condition by short-circuiting the coil, as a result, the bridge shows the value of leads inductance. The difference in both measurements of self-inductance shows the exact value of the self-inductance of a coil.

**Disadvantages of Anderson’s Bridge**

The following are the disadvantages of Anderson’s bridge-

- Anderson’s bridge involves a more complex process for determining the inductance equation.
- The provision of the capacitor junction in the bridge increases the circuit complexity, which in turn makes the shielding of the bridge difficult.
- The calculation of the bridge balance equation is more complicated than the calculation of Maxwell’s bridge.

**Solved Problem on Anderson’s Bridge**

The above figure shows the connection of an Anderson Bridge for measuring the inductance L_{x }and Resistance R_{x }of the coil. Find L_{x}, if balance is obtain when R_{4} = R_{2} = 2kΩ, R_{3} = 500 Ω, r = 50 Ω and C = 0 .5 μF.

**Solution:**

At balance condition

As per the given values we have,

R_{4} = R_{2} = 2kΩ

R_{3} = 500 Ω

r = 50 Ω

C = 0 .5 μF

From equation 1,