Carey Foster bridge
||This article includes a list of references, related reading or external links, but its sources remain unclear because it lacks inline citations. (January 2013)|
In electronics, the Carey Foster bridge is a bridge circuit used to measure low resistances, or to measure small differences between two large resistances. It was invented by Carey Foster as a variant on the Wheatstone bridge. He first described it in his 1872 paper "On a Modified Form of Wheatstone's Bridge, and Methods of Measuring Small Resistances" (Telegraph Engineer's Journal, 1872–1873, 1, 196).
In the diagram to the right, X and Y are resistances to be compared. P and Q are nearly equal resistances, forming the other half of the bridge. The bridge wire EF has a jockey contact D placed along it and is slid until the galvanometer G measures zero. The thick-bordered areas are thick copper busbars of almost zero resistance.
- Place a known resistance in position Y.
- Place the unknown resistance in position X.
- Adjust the contact D along the bridge wire EF so as to null the galvanometer. This position (as a percentage of distance from E to F) is l1.
- Swap X and Y. Adjust D to the new null point. This position is l2.
- If the resistance of the wire per percentage is σ, then the resistance difference is the resistance of the length of bridge wire between l1 and l2:
To measure a low unknown resistance X, replace Y with a copper busbar that can be assumed to be of zero resistance.
In practical use, when the bridge is unbalanced, the galvanometer is shunted with a low resistance to avoid burning it out. It is only used at full sensitivity when the anticipated measurement is close to the null point.
To measure σ
To measure the unit resistance of the bridge wire EF, put a known resistance (e.g., a standard 1 ohm resistance) that is less than that of the wire as X, and a copper busbar of assumed zero resistance as Y.
Two resistances to be compared, X and Y, are connected in series with the bridge wire. Thus, considered as a Wheatstone bridge, the two resistances are X plus a length of bridge wire, and Y plus the remaining bridge wire. The two remaining arms are the nearly equal resistances P and Q, connected in the inner gaps of the bridge.
Let l1 be the null point D on the bridge wire EF in percent. α is the unknown left-side extra resistance EX and β is the unknown right-side extra resistance FY, and σ is the resistance per percent length of the bridge wire:
and add 1 to each side:
- (equation 1)
Now swap X and Y. l2 is the new null point reading in percent:
and add 1 to each side:
- (equation 2)
Equations 1 and 2 have the same left-hand side and the same numerator on the right-hand side, meaning the denominator on the right-hand side must also be equal:
Thus: the difference between X and Y is the resistance of the bridge wire between l1 and l2.
The bridge is most sensitive when P, Q, X and Y are all of comparable magnitude.
- Carey Foster Bridge (PDF) (St.Stephen's College, Delhi University)
- A. H. Fison (1919). "Obituary notices: .... George Carey Foster, 1835–1919; .....". J. Chem. Soc., Trans. 115: 412–427. doi:10.1039/CT9191500408.