US1068341A - Fusible cut-out for controlling electric circuits - Google Patents

Description

V. HOPE.

FUSIBLE OUT-OUT FOR GONTRQLLING ELECTRIC CIRCUITS. APPLICATION FILED JUNB13,1912.

1,068,341 Patented July 22, 1913.

2 SHEETS-SHEET 1.

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l l l l Invenfi I Vefnon fi e va N-L 00W 33 2: 2,;22: g 0%? VJ HOPE.

FUSIBLE CUT-OUT FOR CONTROLLING ELECTRIC CIRCUITS.

APPLICATION FILED JUNE'13,1912.

1,068,341 Patented July 22,1913.

2 SHEETS-SHEET 2.

7+1. M %W8m/W VERNON HOPE, or maivcnns'raa, ENGLAND.

FUSIBIIE CUT-OUT FOR CONTROLLING ELECTRIC C IRCUITS.

Specification or Eetters Patent.

Patented July 22, 1913.

Application medium- 13, 1912. Serial No. 703,552.

To all whom it may concern Beit known that I, VERNON HOPE, a

subject of the King of Great Britain, and

residing in Manchester, England, have invented certa'in new and useful Improvements in Fusible Cut-Outs for Controlling Electric Circuits, of which the following is a specification.

This inventionrelates to fusible cut-outs for electric circuits, which for the sake of brevity will be termed fuses, and has referonce more particularly to fuses made up of two metals, thc one having a high electrical conductivity and a relatively high temperature fusing point and the other a relatively low temperature melting point, so arranged- -that an excess current melts the latter at a comparatively low temperature, whereupon the whole of the-excess current is carried by the former, the cross-sectional area of which is such that it is quickly fused by this current,

The objects of the present invention are to so arrange the two metals as to provide a fuse, in which the fusing current shall be very little in excess of the normal current which can be-continuously carried by the fuse; in which the total cross-sectional area shall be small in relation to the normal current; in which the resistance and therefore the heat developed while carrying thenormal current is small; and in which the fusing shall take place quickly when the current exceeds the -maximum.

'The two metals used are preferably copper and tin,-or a tin-lead-alloy, the former having a high conductivity and a relatively high fusing temperature, and the latter a relatively low melting point, but other pairs of metals having these characteristics may be employed.

-I prefer to arrange the fuse in the form of a cylindrical wire of tin or tin-lead alloy' provided with an inner core of stranded copper wires; the relative cross-sectional areas are determined by the following considerations:Let A be the normal current, and 0 and 25 the portions thereof carried, say by the copper and the tin respectively, so that heat developed will be (P.Rlc, where k is a constant, The radiating surface of the fuse,

is such that under ordinary working atmospheric temperature this quantity of heat is radiated from the fuse and terminals when the temperature of the fuse is safely below the temperature 6 at which the tin melts. Assuming that the fusing current is A, then the heat represented by (A .R]c.

is such that the fuse will not radiate it at ordinary atmospheric temperatures until its temperature is higher than that at which the tin melts, and the cross-sectional area of the copper must be such that when it has, on the melting of the tin, to carry the whole current A the heat developed will be sufficient, in relation to the radiating power of the copper, to raise the temperature of the latter quickly to its fusing point. Thus, while the heat developed by the current 0 in the copper and the current t in the tin, is such as can be effectively dissipated without the temperature of the fuse rising beyond that of the melting point of the tin, the can rent A carried bythe copper alone develops more heat than can be dissipated without raising'the temperature beyond that of the fusing point of the copper. It is desirable therefore to have a comparatively high radiating power while the fuse is intact, and a comparatively low radiating power when the tin has melted, and the arrangement of the compound fuse in the form of a tin or the like wire with copper core com lies with this requirement, giving a large ra iating surface when the current is below the minimumand the tin intact, and a small radiating surface of copper when the excess current melts the tin; the addition of the copper corergives considerable carrying capacity and reduces the resistance; and the stranding of this core gives it the flexibility necessary to prevent the distortion of the outer tin layer due to bending, and so permits of the bi-metallic wire being handled without damage so that it can be vended in rolls or coils in the ordinary way. It is not necessary to strand'the copper core in sizes where a single wire is sufiiciently flexible, and as a single wire is a less effective radiator than equivalent strands, there is an advantage in its use.

The invention is illustrated in-the accomanying drawings in which then, if R be the resistance of the fuse, the- Figure 1 is an elevation, with a part of the sheathing cut away, and Fig.- 1 a transverse sectlon of a fuse wire with a solid copper core and tin or tin-lead alloy sheathing. Figs. 2 and 2 are similar views, showing a fuse wirewith a stranded copper core and a tin or ti iilad sheathing. Figs. 3 and 3" are similar views, showing a fuse with a copper core and a tin or tin-alloy sheathing formed with radiating fins. Figs. f and 4 are similariviews and show a fuse section in whichfl't'here -are several copper cores cmbedd sheathing of tin or tinalloy. Figs. ando are similar views and show a fuse wire'with a tin or tin-alloy core and a copper sheathing. Figs. 6 and 6 are similar views showing a fuse wire with a tin or tin-alloy core and'a sheathing of fine copper wires woven or twisted thereon. Fig. 7 shows the mode in which the fuse wire is applied to ordinary open type fuse terminals. Fig. 8 shows the fuse wire fitted to an inclosed handle type fuse, the latter being shown in section, andFigs. 9 10 and 11 show multiple fuse wires fitted to an inclosed handle type fuse of comparatively large capacity, Fig. 9 being an elevation partly in sect-ion, Fig. 10 being an end elevation, and Fig. 11 an end viewin section. 7 Figs. 1 and 11 show the preferred form; in this case the core C is of copper,'and the sheathing S of a tin lead alloy, suitable for application to the core in the manner now well known and adopted in providing a lead sheathing for insulated cables; that is to say, by forcing the alloy under considerable pressure, when heated and in a semi-plastic condition through a suitable nozzle, through the center of which the copper Wire is drawn, being coated or sheathed with the alloy as it emerges. The proportions of tin and lead may be varied, but sufficient lead must be added to enable the alloy to flow through the nozzle as described.

In Figs. 2 and 2 the copper core C instead of-being solid, is stranded. As stated,

-in larger sizes of fuses, the stranded core is preferable, as it will bend more readily without distorting the sheathing.

In Figs. 3 and 3 the sheathing S instead of having a plain cylindrical periphery, 1S so drawn as to form a series of longitudinal fins as shown, which increase the radiating surface.

In Figs. 4 and 4= a number of separated copper cores C are inclosed in the one sheathing S so as to form a tape; obviously the separate cores C may be replaced by a ribbon of copper.

In Figs. 5 and 5 the core 0 maybe of tin or tin lead alloy, and the sheathing S of copper may be in the form of a tube having thin walls and being preferably perforated; or the tin lead alloy may be coated electrolytically or otherwise with copper, preferably in a granular state, so applied as to leave interstices for the escape of the core when it melts.

Figs. 6 and 6 show a modification equivalent to the last mentioned arrangement, in which the copper sheathing S consists of fine copper wires loosely woven, braided or twisted on to the core.

I find that the last two modifications, while forming effective fuses, and providing very effective low resistance contact with the terminals, do not give as good results as when the metal of low melting point forms the sheathing, since, when the metal of low melting point melts, it does not get away so freely, nor is the radiating surface of the fuse wire so effectively reduced when the metal of low melting point melts.

Fig. 7 shows the bi-metallic fuse wire F used in the ordinary way between the terminals T and T of an open type fuse.

Fig. 8 shows the bi-metallic fuse wire F applied to an inclosed handle type fuse consisting. of a hollow handle H carrying terminal contacts Ii to which the fuse Wire is attached by screws 70.

Figs. 9, 10 and 11 show an arrangement in which a number of bi-metallic fuse wires are fitted to an inclosed handle type fuse. The ends of the fuse wires F are gripped between the fianges A and B which are metallically connected to the contacts K the latter being mounted on a-fiber handle H which is lined with fire-proof material it. The flanges A and B are drawn together by screws a. L are fuse sockets into which the terminal plates K enter.

Pairs of metals possessing the characteristics described, other than copper and tin lead alloy, may obviouslybe used in the manner described, the high fusing point metal having preferably a comparatively high electrical conductivity, as is the case for example with copper; or in some cases a third metal having characteristics intermediate between the other two may be employed, so that the three metals melt or fuse in succession; and fuse wires of different cross-sectional areas than those shown (which are those I have found to give good results in practice) may be employed.

The low melting point metal 'must constitute a considerable proportion of the total cross-sectional area, and when applied as a sheathing, its walls must have substantial thickness, otherwise the characteristics of the fuse will practically be that of the high fusing point metal only; the precise proportions of the relative cross-sectional areas will to some extent depend upon the electrical conductivities of the respective metals.

When the fuse carries the current at which it is designed to blow, the metal of low melting point of course melts first, and the metal of high fusing point carries the current for a sufficient length of time to allow the metal of low melting point to fall away, so that when the final rupture of the fuse takes place, the low melting point metal is not volatilized by the momentary are formed.

()n securing the bi-metallic Wire in the fuse terminals, the wire should when it has a copper core, be screwed down so as to flatten the sheathing and practically make contact case of a series of handle fuses the presence of the melted tin indicates clearly the fuse which has blown.

The compound fuse wire would usually be manufactured in lengths and of sizes to give standard ratings.

Fuses constructed as described will carry as much as 90 per cent. of the full load current withoutundue heating, and without oxidizing, and, such fuses have a definite time element, and for short periods will carry considerably more than the full load current, say six times the full load current; and are thus particularly useful in controlling small alternating current motors where the starting current is excessive.

When used in inclosed replacement or handle fuses, the carrying capacity is somewhat reduced, but such fuses are much more reliable when used in this way than is the case with single metal fuses.

Having now fully described my inven tion, I declare that what I claim, and desire" to secure by Letters Patent is 1. A fuse consisting of two metals, the one having a relatively high fusing point and the other having a relatively low fusing sheathing for the other one; substantiallyas described.

2. A fuse consisting of a copper and a tin-lead alloy, one of the said two metals forming a sheathing for the other one, substantially as described.

3. A fuse consisting of a core of metal having a high fusing point and of a sheathing therefor of metal having a low melting point; substantially as described.

4. A fuse consisting of a core of copper and off'a sheathing therefor of tin-lead alloy; substantially as described.

5. A fuse consisting of two metals the one being arranged in the form of multi le wires and the other as asheathing there or;.substantially as described.

6. A fuse consisting of multiple Wires of copper and a tin-lead sheathing therefor; substantially as described. l

7. A fuse consisting of two metals having different fusing points the one'metal forming a sheathing for the other, the combined cross-sectional area of which two metals is suflicient to carry the rated current without undue heating, the area of the metal of higher fusing point being too small to carry the rated current; substantially as described.

8 A fuse consisting of a plurality of metals one of which has a higher melting point than the others and one of which forms an outer sheathing; substantially as described. i

In testimony whereof, I affix my signature in presence 0 two witnesses.

, VERNON HOP E1. Witnesses: ALICE S. ALLEN,

J osEPH E. Hms'r.

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