This experiment demonstrates the use of a voltage divider within a Wheatstone bridge circuit, a common setup for precise measurement of unknown resistances, often used with sensors.
To understand the operation of a Wheatstone bridge circuit and its application in measuring unknown resistances or sensor outputs.
Connect the circuit as shown below, with two voltage dividers forming a Wheatstone bridge. The bridge is balanced when the ratio of resistances on each side is equal.
A Wheatstone bridge circuit consists of two voltage dividers connected in parallel. The output voltage, or bridge voltage (V_out
), is measured between the midpoints of the two dividers. The circuit is balanced when the ratios of resistances on each side of the bridge are equal, resulting in zero voltage across V_out
:
(R1 / R2) = (R3 / R4)
If one resistance changes (for example, a sensor in place of R4
), the bridge becomes unbalanced, and V_out
varies proportionally to the change. This configuration is commonly used for precise measurements in strain gauges, temperature sensors, and more.
R1
, R2
, and R3
. Connect them as shown in the circuit diagram.R4
as the unknown resistor or a variable resistor that you can adjust to simulate a changing sensor value.R1
and R3
and the other side to the bottom of R2
and R4
.V_out
.R4
and observe how V_out
changes in response to resistance changes. Find the point where V_out
is zero, indicating the bridge is balanced.Record the resistance values of R1
, R2
, R3
, and R4
. Note the bridge output voltage V_out
at various resistance settings for R4
. Observe the conditions under which the bridge is balanced (i.e., when V_out
is close to zero).
This experiment demonstrates how a Wheatstone bridge circuit can precisely measure changes in resistance. When one resistor is unknown or varies (e.g., a sensor), the circuit can detect small changes by monitoring V_out
. This setup is widely used for precise sensor applications, such as in load cells or temperature sensing.