Four terminal approach is used in measuring low resistance because it -
Eliminates the effect of leads and currents
Measuring very low resistance values, typically below 1 ohm, presents a challenge. Standard resistance measurement methods, like the two-terminal method, can introduce significant errors due to the resistance of the connecting leads and the contact resistance between the leads and the component being measured. These resistances, even if small, can be comparable to or even larger than the low resistance value being measured, leading to inaccurate results.
In a two-terminal measurement, the instrument applies a current through the unknown resistance and measures the voltage across it. The same two terminals are used for both current injection and voltage sensing. The total resistance measured by the instrument includes:
So, the measured resistance $R_{measured}$ is approximately $R_{measured} = R_{component} + R_{leads} + R_{contact}$. When measuring high resistances, $R_{component}$ is much larger than $R_{leads}$ and $R_{contact}$, making their effect negligible. However, for low resistances, $R_{leads}$ and $R_{contact}$ can be significant compared to $R_{component}$, leading to a large percentage error in the measurement.
The four-terminal method, also known as the Kelvin method, overcomes the limitations of the two-terminal method by separating the current-carrying leads from the voltage-sensing leads. It uses four terminals connected to the low resistance component:
The high impedance of the voltmeter ensures that very little current flows through the voltage leads. Therefore, the voltage drop measured by the voltmeter is essentially only the voltage drop across the unknown resistance element itself, with minimal voltage drop caused by the resistance of the voltage leads or their contact resistance.
According to Ohm's Law, the resistance ($R$) is calculated as the voltage ($V$) measured by the voltmeter divided by the current ($I$) flowing through the component:
\(R = \frac{V}{I}\)
Because the voltage ($V$) is measured precisely across the resistance element, excluding the voltage drops in the current leads and contacts, this method effectively eliminates the influence of lead and contact resistances on the measurement of the low resistance value.
| Feature | Two-Terminal Method | Four-Terminal Method |
|---|---|---|
| Leads Used | 2 (for both current and voltage) | 4 (2 for current, 2 for voltage) |
| Measured Voltage Drop | Across component + leads + contacts | Primarily across component |
| Effect of Lead/Contact Resistance | Significant error for low resistance | Minimized/Eliminated for voltage measurement |
| Suitability | High & medium resistance | Low resistance |
Therefore, the most accurate reason for using the four-terminal approach in measuring low resistance is that it effectively eliminates the effect of the resistance of the connecting leads and contact resistances from the voltage measurement.
| Concept | Description | Importance |
|---|---|---|
| Low Resistance | Resistance values typically < 1 ohm. | Challenging to measure accurately due to parasitic resistances. |
| Two-Terminal Method | Uses 2 leads for current & voltage. | Lead/contact resistance adds significant error for low R. |
| Four-Terminal (Kelvin) Method | Uses 4 leads: 2 for current, 2 for voltage. | Voltage measurement excludes lead/contact resistance effect. |
| Contact Resistance | Resistance at point of electrical contact. | Significant source of error in 2-terminal low R measurement. |
The four-terminal sensing method is crucial in various applications where accurate low resistance measurements are required:
This method ensures that the measurement reflects the true resistance of the material or component itself, rather than being skewed by external factors like connection quality.
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