in the diagram of fig1 and 2 , the time in seconds is plotted on the abscissa and the temperature in degrees celsius on the ordinate . in fig1 the burnt gas temperature according to line 1 is constantly 400 ° c . at a likewise constant speed of the burnt gas of 1 m / sec . the triggering temperature provided for is a constant 68 ° c . according to line 2 and the sprinkler starting or initial temperature is 0 ° c . as can be seen in the broken curves 3 and 4 for the values c = 0 or c = 1 , these intersect the straight line 2 for the triggering temperature at only a small interval in time , namely at t = 18 sec ( c = 0 ; curve 3 ) and t = 20 sec ( c = 1 ; curve 4 ). it can be seen from this that the c - value only exerts a small and secondary influence on the achieving of the triggering temperature of 68 ° c . and the rti value is the decisive parameter for the triggering behaviour according to the high supply of energy as a result of the high temperature difference between the burnt gas and the triggering element . for the sake of simplicity , it is assumed here that the pipe and water temperature remains constant at 0 ° c . this also applies correspondingly with respect to the diagram of fig2 in which the line 1 indicates a constant burnt gas temperature of 200 ° c . at a burnt gas speed of 4 m / sec . the triggering temperature provided for according to line 2 is again 68 ° c . and the sprinkler starting temperature is 0 ° c . here too , the broken curves 3 for c = 0 and 4 for c = 1 intersect the straight line 2 for the triggering temperature at only a small interval in time from each other , namely at t = 20 sec ( c = 0 ; curve 3 ) and t = 23 sec ( c = 1 ; curve 4 ). here too , the influence of the parameter c for the heat transfer by heat conduction from the triggering element to the piping or sprinkler body is thus of only secondary importance and the triggering behaviour is thus decisively determined by the rti value . in the diagram in fig3 in which , as was again assumed in fig4 b and 9 , the pipe and water temperature remains constant at 0 ° c ., the burnt gas temperature is again 200 ° c ., as in fig2 but the speed of the burnt gas is only 1 m / sec as in fig1 . here too , 68 ° c . was predetermined as the triggering temperature , and the sprinkler starting temperature is 0 ° c . from the broken curves 3 for c = 0 or 4 for c = 1 respectively , it can be seen that they intersect the triggering temperature straight line 2 at t = 41 sec and t = 56 sec respectively , i . e . at a considerable time lag in relation to each other . it follows from this that due to the supply of energy which is considerably lower than in the examples of fig1 and 2 , the c - value here plays a very considerable part with respect to the triggering behaviour . this is made even more considerably clear by the diagram in fig4 wherein according to line 1 the burnt gas temperature is 130 ° c . and the speed of the burnt gas is again set at 1 m / sec . the triggering temperature and the sprinkler starting temperature are unchanged at 68 ° c . and 0 ° c . respectively . the curve 3 for c = 0 intersects the triggering temperature curve 2 at t = 73 sec , whereas the curve 4 for c = 1 does not intersect the straight line 2 , but rather only approaches it . however , this means nothing more than that at a c - value of 1 there is no response of the sprinkler at all here as a result of not achieving the triggering temperature . therefore the c - value here takes on a quite decisive importance . in the bar chart of fig5 a and fig5 c on the left in fig5 a the rti - values for a series of known and conventionally used soldered and glass bulb sprinklers are plotted for oncoming flow through the burnt gas along and perpendicular to the sprinkler stirrup and on the right in fig5 c the corresponding c - values for most of these sprinklers are plotted in the same manner . as can be seen from this chart , among the soldered sprinklers sprinkler no . 13 and with reservations sprinkler no . 14 have relatively favourable values both for the rti and for the c - values , whereas all the other soldered sprinklers either have an unfavourable rti or c - value or predominantly even both . the relationships are considerably less favourable in the case of glass bulb sprinklers , of which only sprinkler no . 23 has a favourable rti value , but an unfavourable c - value , in particular in the case of oncoming flow through the burnt gases lengthwise to the sprinkler stirrup . in the case of all the other sprinklers , equally the rti values and also the c - values are relatively high , particularly in the case of an oncoming flow lengthwise to the stirrup , which indicates long triggering times or triggering delays . in the diagram in fig5 b , which also clearly shows the considerable influence of the c - value on the triggering delay and the minimum temperature required for triggering at a speed of the burnt gas of 1 m / sec , an initial burnt gas temperature of 70 ° c . at a regular temperature increase of 2 ° c ./ min ( broken line 1a ) was assumed . the triggering temperature ( line 2 ) is again fixed at a constant 68 ° c ., the sprinkler starting temperature here is fixed at 20 ° c . ( line 2b ) and the speed of the burnt gas is again 1 m / sec . as can be seen by the broken curves 3 and 4 for the values c = 0 and c = 1 respectively , these intersect the triggering temperature straight line 2 at approximately t = 170 sec or t = 1 . 375 sec . it can be seen by the curves 5a to 5e which have been drawn in for the additional c - values 0 . 2 , 0 . 5 , 1 . 5 , 2 . 0 and 2 . 5 that the relationship between the minimum burnt gas temperature required for triggering and the nominal triggering temperature increases considerably . this relationship is additionally influenced by differing pipe temperatures and / or speeds of the burnt gas . in the sprinkler in fig6 which is partially drawn in section , the collar 6 is provided with the threaded journal 7 , the water through - hole 8 and with the stirrup 9 , which holds the spray disc 10 in the conventional manner . the glass bulb 11 having axis 24 is supported on the collar 6 at its ends by the heat - insulating component 12 with the annular collar - shaped plates 12a and by the disc springs 13 sitting on valve seal 22 and also in the stirrup 9 by the heat - insulating component 14 with annular plates 14a . the heat - insulating components 12 and 14 are here designed as hollow cylinders , at least the hollow cylinder on the piping side being expediently closed facing the piping or water side in order to prevent direct contact between the water in the piping and the glass bulb 11 , which would result in an unwanted flow of heat away from the glass bulb to the piping or water . the dissipation of heat can also be additionally reduced , for instance , in that the sealing member 23 which is conventionally used between the disc spring 13 and the sprinkler body is full - surfaced . of course , a seal could also be provided in another way . both the components 12 and 14 and the plates 12a and 14a formed thereon are constructed with thin cross - sections so that they have a relatively low mass , but a large surface area in comparison . the disc springs 13 and the heat - insulating component 12 on the piping side are naturally arranged and constructed so that -- if necessary with the aid of additional components or elements which are not shown -- secure blocking off of the water is guaranteed until the point of triggering of the sprinkler . the plates , collars or the like 12a and / or 14a may be made from the same high - strength corrosion - resistant material as the cylinders or cylinder sleeves 12 and 14 , for instance from v 2 a steel cr 18 ni 8 or also from another , particularly good heat - conductive , material such as copper , silver , nickel , aluminium or the like . in this case , the plates cause rapid heating - up of the components 12 and / or 14 , which causes a thermal barrier to be built up between the glass bulb 11 and the collar 6 or the stirrup 9 which prevents heat being able to be conducted away from the glass bulb 11 to the collar or stirrup , or , with an appropriate layout and configuration , in particular if the plates adjacent to the glass bulb are in direct contact therewith , even heat is conducted to the glass bulb 11 from the components 12 and / or 14 and thus the triggering thereof is accelerated . as well as the aforementioned v 2 a steel , for instance also chromium / nickel steel , steel with 36 % ni , monel metal , which is a nickel - copper alloy containing approximately 65 % nickel , 30 % copper , and 5 % other materials , especially manganese and iron , ceramic and glass may also be considered for use as a material for the heat - insulating components 12 and 14 due to their properties , in particular with respect to corrosion - resistance , high strength , low heat conductivity and also great heat absorption capacities but low heat storage capacities . however , more conductive materials may also be used if these can be compensated for , for instance , as a result of higher strength by lower material cross - sections . compensation may also take place through longer insulating sections . in the embodiment in fig7 in which the same parts are again marked by the same references , the sealing plate 15 is arranged between the disc spring 13 and the sprinkler collar 6 . the disc spring 13 here takes over the function of the heat - insulating component 12 and is therefore made from a material which has the properties required for this purpose . on the side of the stirrup , the heat - insulating component 14 is constructed here as a hollow cylinder which receives the sealed end of the glass bulb 11 and is made of a suitable material . between the glass bulb 11 and the components 13 ( 12 ) and 14 , the collars or the like 16 which are made of copper or another highly heat - conductive material are arranged resting directly on the glass bulb , which collars or the like surround the end of the disc spring 13 ( 12 ) or of the hollow cylinder 14 which is adjacent to the glass bulb with flanging on the inside and are gripped between the components 13 ( 12 ) and 14 . the thin collars 16 which serve as thermal collectors have a large surface area in comparison with their mass , which causes them to take up a large quantity of heat , and thus are heated up rapidly to a considerable extent by the burnt gases which occur in the case of a fire . since only relatively little heat can be conducted away via the components 13 ( 12 ) and 14 due to their material properties and cross - sectional form , the collars form a heat barrier , so that removal of heat from the glass bulb to the sprinkler body can be at least suppressed as far as possible , and even , on the contrary , under certain circumstances heat may be conducted to the glass bulb . here glass bulbs which are not thickened , but which , as has been conventional hitherto , are relatively thin - walled , in particular have positive results , and thereby facilitate the flow of heat from the collector into the expensive liquid . in fig8 which shows a simplified section through fig7 along the line a -- a , the cross - section of the sprinkler stirrup parts 9a and 9b relative to an imaginary connecting line which connects them together by their centres and passes through the axis of the glass bulb 11 is here at an angle of approximately 60 ° c ., so that only little of the air or the burnt gases which has or have already cooled on the stirrup parts according to the direction of air flow also meets the triggering element , i . e . the glass bulb 11 , which according to fig5 b is highly advantageous for improving the rti and c - values . this principle can of course also be applied in the case of known three - armed or multi - armed stirrups . in the diagram of fig9 in which line 1 shows the constant burnt gas temperature of 200 ° c . and line 2 the intended triggering temperature of 68 ° c ., the triggering behaviour of a sprinkler is plotted , taking into account a waiting period which occurs after the nominal temperature is reached . this waiting period can be put down to the heat which has to be produced at the moment of melting in the case of soldered sprinklers . but even with glass bulb sprinklers this waiting period occurs to a considerable extent . this waiting period can be determined by measuring , sprinklers with different starting temperatures being caused to trigger under given test conditions of burnt gas temperature and speed , and their triggering , times being determined . if the moment of triggering is selected as the reference time and the starting temperatures of the sprinklers tested is entered at a point in time which is displaced to the left by the amount of triggering time , the true heating - up curve of the triggering element , shown as an example by curve 4a , is obtained at least up to the nominal temperature . it can be seen from this that the glass bulb sprinkler started from 0 ° c . does not trigger after 27 seconds ( line a ) but after a longer period of delay , here after 56 seconds ( line b ). in contrast , the glass bulb provided according to the invention with a predetermined breaking point already triggers at a considerably earlier point in time and at a lower temperature ( line c ). the cause of this delay has at present not been investigated in enough detail . however , it is attributed to the part of the energy which is required to build up the pressure in the glass bulb . furthermore , it is known that glass withstands higher stresses for a short time than in the long term . it can therefore perfectly well be assumed to be probable that the glass bulb withstands a higher temperature over a certain time span than the nominal temperature and the increased pressured connected therewith . attempts have been made to express this phenomenon of triggering delay with an activation parameter . this has the unit ° c . it can be imagined as if it represented the temperature difference between the actual triggering temperature of the glass bulb and the nominal triggering temperature . the triggering temperature is the bursting temperature of the glass bulb , which is determined in a liquid with a slowly increasing temperature . the bursting temperature is determined by the filling capacity , matched to the type of the material used for filling , and by the bursting pressure of the glass bulb . the activation parameter depends on the type of the liquid which is poured in and the bursting pressure of the glass bulb . at room temperature , the hermetically closed glass bulbs are not completely filled , but rather contain a cavity which looks like an air bubble , but which essentially is filled with vaporised expansive liquid as well as air which is enclosed in the glass bulb upon the hermetic closure thereof . with increasing temperature of the glass bulb , this cavity gradually disappears , and is no longer detectable at a few degrees celsius below the bursting temperature , whereby it may be assumed that the liquid now completely fills the interior of the glass bulb . for this operation which is connected with a pressure increase with simultaneous suppression of expansion , the energy must first be applied by the heat flowing to the glass bulb , which energy , in the given glass bulb , is greater , the greater the compressibility k and the lower the coefficient of expansion of the filling liquid and the greater the specific heat e spec which is related to the volume of the liquid . the energy required becomes less , the greater the characteristic number formed from these values ## equ4 ## which is for instance 100 for mercury , 27 for benzene and silicone fluid and 20 for glycerine and glycol . by selecting suitable substances , but also by suitable mixing , one thus has it well in hand to influence , i . e . reduce , the activation parameter . the activation parameter can however also be reduced to a considerable extent by suitable configuration of the glass bulbs . the glass bulbs need to be permanently stable against longitudinal forces which occur which serve to hold the sealing member closed . likewise , they need to be stable against bending forces . however , they do not need to be stable against increasing internal pressure , as this only increases in the case of heating , whereby the glass bulb upon heating to a predetermined triggering no longer has to withstand the internal pressure corresponding thereto , but rather is intended to trigger by self - destruction and to activate the sprinkler by opening the seal . in fig1 a , a conventionally constructed glass bulb 11 with an even wall thickness over its entire extent is shown on a greatly enlarged scale and in a cross - section in a top view . according to fig1 d , the pressure in the glass bulb first only increases very slowly with increasing heating and progressing time , then increases greatly relatively suddenly , i . e . within an additional , relatively small temperature range , until finally the relatively high bursting pressure p berst , at which the glass bulb then is broken as intended , is reached at the temperature t berst . in fig1 b the glass bulb 11 is shown in the same way as in fig1 a , but now provided with the predetermined breaking point 17 . according to fig1 e , the predetermined breaking point results in a very much lower bursting pressure p berst and hence also a lower energy which is required to build up the pressure . also the excessive increase in temperature which otherwise occurs in the event of a rapid temperature increase is considerably reduced . one example of the configuration of the predetermined breaking point 17 is shown in the greatly enlarged longitudinal section through the glass bulb 11 in fig1 c . the predetermined breaking point is thereby constructed as a groove - like recess which is crescent - shaped when viewed , so that the occurrence of notch stresses is avoided . other forms of the predetermined breaking point than those shown in fig1 b and 10c are of course conceivable and producible . likewise , two or more predetermined breaking points , preferably regularly spaced across the periphery of the glass bulb , may be provided instead of a single predetermined breaking point . in the embodiment in fig1 , in which the same parts again are provided with the same references , the spray disc 10 is attached to the collar 6 , which is provided with the threaded journal 7 , by the stirrup arms 9a and 9b . the glass bulb 11 is supported on the collar 6 by means of the heat - insulating component 12 , which is again sealed at one end and provided with the ribs , plates or the like 12a via the disc spring 13 , which acts as a sealing member , and on the spray disc 10 via the inside flanging 18 of the thermal collector which passes through the central opening 19 in the spray disc 10 and is constructed as a hollow cylinder 20 with an external , thin disc 21 having a large surface area . of course , a particularly suitable material such as copper or the like is used for the thermal collector 20 , 21 and , of course , here too secure sealing is ensured by the disc spring 13 , optionally by using additional sealing means . within the scope of the invention , instead of the sprinklers shown in fig6 to 8 by way of example , one is moved to use other configurations of sprinklers in conjunction with heat - insulating components which are constructed in other ways , without or with ribs , plates , discs or the like which may optionally act as thermal collectors , as long as the above - mentioned criteria which are essential to the invention are correctly taken into account in so doing .
a thermal triggering device for sprinklers for stationary fire - extinguishing systems . the demands made on sprinklers for stationary fire - extinguishing systems are to the effect that increasingly shorter triggering times are demanded in order to be able to fight fire more quickly and more effectively . the novel triggering device should therefore have such a short triggering time that the response thereof in case of fire takes place as extactly as possible at the predetermined triggering temperature . the triggering element which is constructed as a glass bulb is at least supported on the sealing member of the sprinkler via a heat - insulating component , made from a corrosion - resistant material of high strength and low heat conductivity and also great heat absorption but low heat storage capacities , the component having a low mass and a large surface area and a small cross - section in the direction of the flow of heat .