A Wheatstone bridge is an electrical circuit used to measure an unknown electrical resistance by balancing two legs of a bridge circuit, one leg of which includes the unknown component. Its operation is similar to the original potentiometer. It was invented by Samuel Hunter Christie in 1833 and improved and popularized by Sir Charles Wheatstone in 1843. One of the Wheatstone bridge's initial uses was for the purpose of soils analysis and comparison.
In the figure, is the unknown resistance to be measured; , and are resistors of known resistance and the resistance of is adjustable. If the ratio of the two resistances in the known leg is equal to the ratio of the two in the unknown leg , then the voltage between the two midpoints (B and D) will be zero and no current (electricity) will flow through the Galvanometer (G) or . No current flow through G , the bridge is said to be "balanced". If the bridge is unbalanced, the direction of the current indicates whether is too high or too low. is varied until there is no current through the galvanometer, which then reads zero.
Detecting zero current with a galvanometer can be done to extremely high accuracy. Therefore, if , and are known to high precision, then can be measured to high precision. Very small changes in disrupt the balance and are readily detected.
At the point of balance, the ratio of
Alternatively, if , , and are known, but is not adjustable, the voltage difference across or current flow through the meter can be used to calculate the value of , using Kirchhoff's circuit laws (also known as Kirchhoff's rules). This setup is frequently used in strain gauge and resistance thermometer measurements, as it is usually faster to read a voltage level off a meter than to adjust a resistance to zero the voltage.
First, Kirchoff's current law is used to find the currents in junctions B and D:
The potential difference between points B and D will be near zero (0 VDC) volts using a digital multimeter.
Then, Kirchhoff's voltage law (KVL) is used for finding the voltage in the loops ABD and BCD:
When the bridge is balanced, then IG = 0, so the second set of equations can be rewritten as:
Then, the equations are divided and rearranged, giving:
From the first rule, I3 = Ix and I1 = I2. The desired value of R4 is now known to be given as:
If all four resistor values and the supply voltage (VS) are known, and the resistance of the galvanometer is high enough that IG is negligible, the voltage across the bridge (VG) can be found by working out the voltage from each potential divider and subtracting one from the other. The balance state equation for this is:
where VG is the voltage of node D relative to node B.
In a balanced state, where all four resistances are known. The Wheatstone bridge can be analysed as two series resistances in a parallel circuit. For example, you have a Wheatstone Bridge balanced state circuit with four known resistance values: R1 = 5Ω, R2 = 10Ω, R3 = 2Ω, and R4 = 8Ω. Voltage source (Vs) equals 12 VDC. Find Vg which is the circuits Vout.
In an unbalanced state, only three resistances are known (R1, R2, along with a variable potentiometer (R3/4 or Rv). This Wheatstone bridge is still two series resistors in a parallel circuit; its unbalanced because we have to calculate the fourth resistance. Calculating the resistance and adjusting the pot (Rv) balances the voltage potential within the circuit to zero across the galvanometer. For example, you have a Wheatstone Bridge unbalanced state circuit with three known resistance values: R1 = 10Ω, R2 = 100Ω, Rv = 25Ω, and Rx = ???Ω. Voltage source (Vs) equals 12 VDC. Find Rx (unknown resistor value) using the circuit ratio method:
Next, we re-arrange the ratio to find VR2.
Here IA and IB cancel each other out and is re-written as.
Now, we rearrange the equation to solve for Rx.
Finally, we plug in the numbers from above.
The Wheatstone bridge illustrates the concept of a difference measurement, which can be extremely accurate. Variations on the Wheatstone bridge can be used to measure capacitance, inductance, electrical impedance and other quantities, such as the amount of combustible gases in a sample, with an explosimeter. The Kelvin bridge was specially adapted from the Wheatstone bridge for measuring very low resistances. In many cases, the significance of measuring the unknown resistance is related to measuring the impact of some physical phenomenon (such as force, temperature, pressure, etc.) which thereby allows the use of Wheatstone bridge in measuring those elements indirectly.
The concept was extended to alternating current measurements by James Clerk Maxwell in 1865 and further improved by Alan Blumlein around 1926.
The practical applications for the Wheatstone Bridge circuit is used for many biomedical applications to include but not limited to:
- MRI/CT - table positioning, accurate movement of the CT scan imaging device and equal patient weight distribution. High accuracy is needed to perform imaging functions while preventing over-travel of the patient placed within the scanning tube.
- Infusion pumps/Syringe pumps - monitors and controls the amount of fluid flow of intravenous medication that was to be received via the tubing.
- Mammography - monitors the amount of physical force that is applied to the patients breast by the machine itself when attempting to take an image.
- Conventional radiography - monitors the amount of x-ray dose received to the AEC cells and the patient.
- Scales, weighing/Patient lifts - with the incorporation of a load cell into the bottom metal plates these scales routinely require re-zeroing which uses the above circuit.
- Remote robotic surgeries - used so physicians are able to precisely measure both depth of force and drill bit rotational force during remote hip surgeries
- Dialysis machines - ensures uniform fluid flow and circulation of proper rate, proportion and frequency according to the parameters set by its accompanying electronic controller device.
- Ventilator gas tester - ensures uniform gas flow (i.e I:E, PEEP, TV, fIO2, SIMV, AC, etc...).
- Pressure Meter - ensures uniform negative and positive pressure flow (i.e. mmHg, cmH20, inH20, PSI, etc...).
- Vital signs simulator
- Strain gauge circuits
- Pressure transducer circuits
- and more
The Wheatstone bridge is the fundamental bridge, but there are other modifications that can be made to measure various kinds of resistances when the fundamental Wheatstone bridge is not suitable. Some of the modifications are:
- Carey Foster bridge, for measuring small resistances
- Kelvin Varley Slide
- Kelvin bridge
- Maxwell bridge
- ↑ "The Genesis of the Wheatstone Bridge" by Stig Ekelof discusses Samuel Hunter Christie and Charles Wheatstone's contributions, and why the bridge carries Wheatstone's name. Published in "Engineering Science and Education Journal", volume 10, no 1, February 2001, pages 37–40.
- ↑ Chevalier, Robert., "Strain Gauge Technology in OEM Medical Devices." Design News. 4/7/2011. http://www.designnews.com/document.asp?doc_id=230407&
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