Accession No

6865


Brief Description

dip circle, made and used in the Cavendish Laboratory, late 19th Century


Origin


Maker


Class

magnetism; earth sciences


Earliest Date

1874


Latest Date

1894


Inscription Date


Material

metal (brass, iron); wood


Dimensions

diameter of ring 173mm; diameter of base 130mm; overall height 205mm


Special Collection


Provenance

It is recorded in the Cavendish Laboratory's 1894 alphabetical catalogue of apparatus on p.49, as part of a set.


Inscription

E 12 E
E [on plinth]


Description Notes

dip circle, 19th C

Brass dip circle with iron needle mounted on a circular wooden base. Ring divided 0 - 90˚ - 0 - [90˚] - 0, numbered by 10˚, graduated to 1˚. Needle is pivoted between two brass columns.

Possibly a classroom demonstration instrument.

Complete


References


Events

Description
A dip circle is used the measure the angle between the horizon and the earth’s magnetic field (the dip angle). They were used in surveying, mining and prospecting as well as for the demonstration and study of magnetism.

Georg Hartmann first discovered dip angle in 1544, when he noticed the needle on a compass dipped towards the north hemisphere. Rather than explore this phenomenon, Hartmann sought ways to eliminate it. However, Robert Norman investigated dip angle further and in 1581 described in print a device to measure this phenomena.

Early dip circles were not accurate and gave poor results. Over the next 300 years many improvements were made, including reducing the friction between the needle and its pivot and encasing the circle in glass. Initially, dip circles could only be used on land, but in 1834 Robert Were Fox designed the first that could be used on board a moving ship. This advance proved to be of major assistance to polar navigation, in particular in the discovery of the exact position of the South magnetic pole. Another important improvement to the instrument was developed in the 1830s by the Dublin Physicist Humphrey Lloyd, who devised a way of attaching a magnetic needle at right-angles to the dip needle in order to measure the intensity of force (by seeing the extent to which the right-angle needle deflected the dip-needle).

The design of dip circles approached its peak at the beginning of the Twentieth century and by World War I the most advanced dip circles were being made. However, with the development of electronic systems dip circles became obsolete.
07/02/2008
Created by: Boris Jardine (with amendments by A. McConnell) on 07/02/2008


FM:40623

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