text: fig1 illustrates a wind turbine 1 , comprising a wind turbine tower 2 on which a wind turbine nacelle 3 is mounted . a wind turbine rotor 4 comprising at least one wind turbine blade 5 is mounted on a hub 6 . the hub 6 is connected to the nacelle 3 through a low speed shaft ( not shown ) extending from the nacelle front . the wind turbine illustrated in fig1 may be a small model intended from domestic or light utility usage , or may be a large model , such as those that are suitable for use in large scale electricity generation on a wind farm for example . in the latter case , the diameter of the rotor could be as large as 100 meters or more . fig2 illustrates one example of an optical fibre for use in an optical fibre sensor system according to the invention . although in this example , the optical fibre described contains a plurality of gratings , it will be appreciated that the optical fibre according to the invention could be constructed with a plurality of lpgs , or indeed any other suitable wavelength - selective optical grating . the optical fibre 200 comprises a fibre core 201 , and a fibre cladding 202 . the fibre core is provided with two sets of fibre bragg gratings ( fbgs ) 203 , 204 , 205 , 206 and 207 in fbg set 208 , and fbgs 209 , 210 , 211 , and 212 in fbg set 213 . the fbg sets 208 and 213 correspond to fbgs a to d and f to i respectively in fig5 ( a ) and 5 ( b ), while fbg 203 corresponds to fbg e . each fbg is tuned in the sense that it will reflect a different wavelength of light determined by the grating dimensions . if the section of the optical fibre 200 having an fbg is placed next to or in contact with a wind turbine component , then the changes in the length of the optical fibre at that location ( for example , due to a temperature change of the component or a change in strain ), will result in a change in both the dimensions of the fbg and the refractive index of the optical fibre . both effects alter the wavelength of any light reflected and / or transmitted by the fbg , which can therefore be used as a measure of the temperature or strain of the component at that location . fig3 illustrates an embodiment of an optical fibre sensor system according to an example of the invention . the sensor 300 comprises a light emitting device 301 , such as an led , laser , halogen or metal halide source , a light collecting measuring device or detector 302 , such as a photo - sensor , and an optical fibre 200 ( for conciseness only fbg set 208 is shown ). the light emitting device is connected to one end of the fibre optic cable to input light into the fibre , and the light measuring device ( such as an interrogator ) is connected to the other to receive light transmitted along the fibre . an interrogator is a light detector that detects and measures light across a wide spread of wavelengths . a controller 303 is connected to both light emitting device 301 and light measuring device 302 , by connections 304 and 305 , such as wires or cables . components 301 to 305 may be housed in a mounting box , or the like , for easy attachment to the inside or outside of a wind turbine component . fig4 illustrates the controller 303 as described above with reference to fig3 . the controller comprises a light source controller 400 , coupled to the light source 301 . the light source controller is used to determine when the light source is operated . the controller also comprises a memory 401 for storing the output received from the light detector . an analyser 402 , such as a processor , and coupled to the memory , is provided to analyse the output from the light detector 302 stored in memory and determine the wavelengths of light reflected by the fbgs . there are two alternatives available for determining the wavelengths of light reflected by the fbgs . either the wavelengths are measured directly by having the light detector 302 positioned at the same end of the optical fibre 200 as the light source 301 , or by detecting the difference between the light profile provided by the light source , and the light received at the other end of the optical fibre . a calculation unit 403 is coupled to the analyser 402 to calculate the difference between the wavelength received from each fbg and a reference wavelength expected if there were no temperature or strain difference , for example , between the fbgs ( a , b , c or d ) and fbg e . the calculation unit 403 is also coupled to the memory 401 . the memory 401 is adapted to store a look - up table , and the look - up table is provided to allow the calculation unit to look - up the expected range of wavelengths for each fbg . the calculation unit then determines the value of the operating condition measured by fbg . the controller further comprises an input / output line 404 for receiving and transmitting instructions or data to and from a remote site , such as a monitoring station . the input / output line may be wired or wireless . additionally , error detection can be incorporated into the controller 303 . if no wavelength is detected within the expected range for a particular fbg , then this could be an indication of a fault . this could be the result of a breakdown in the coupling between the operating conditions being measured , or that the fbg itself is faulty . although the controller has been described in terms of separate hardware components , this is solely to illustrate the functionality of the controller in a clear manner . it would be possible in practice to provide the hardware components as software or hardware , or as any combination of single or combined components . the optical fibre 200 is mounted on or in a wind turbine component ( not shown in fig3 ) to measure the strain in the component , or indeed any other suitable operating condition of the component , such as temperature . in one example , this may be achieved by mounts attached to the outside or inside surface of the component . other mounting methods would be acceptable as would be known to the skilled person . if the sensor were to be installed in a wind turbine to measure the strain in the wind turbine blades , it is likely that the mounting box would be situated in the hub 6 , and the optical fibre 200 would extend internally within the blade from the hub to the relevant region of the blade to be assessed . in this way , the aerodynamic properties of the blades are not affected by the presence of the sensor . in other locations , the optic fibre sensor may be mounted on the outside of the component . the optical fibre sensor system described can therefore be utilised to measure a number of operating conditions , one operating condition per fbg . however , it is required that those operating conditions are coupled ( i . e . that an increase in one operating condition results increase in the other operating conditions , and vice versa ). for example , the operating conditions could be the temperature of a number of components housed within the electrical housing of a wind turbine since it would be expected that a rise in temperature of one component would lead to a rise in temperature of another component , and vice versa . the overall range of temperatures that could be measured can be large , for example from − 40 degrees c . to 60 degrees c . the operation of the optical fibre sensor system will now be described in more detail , and with reference to fig2 , 5 a and 5 b . in this example , the use of the sensor to detect temperature only will be described . the operation of the sensor will be the same for other operating conditions that are to be measured . furthermore , in this example , it is assumed that the fbgs are configured to reflect light back to the detector , rather than transmit light to a remote detector at the end of the optical fibre 200 . in practice , either or both configurations are acceptable . as shown in fig2 , optical fibre 200 comprises a number of fbg &# 39 ; s a to i , each tuned to a different wavelength and each located at a different location on the component where measurements are to be taken . as shown in fig5 a , fbg e is tuned to a first default wavelength , lying in the middle of the range of wavelengths of light that can be transmitted along the optical fibre 200 and detected by the light detector 302 . also as shown in fig5 a , a first range of measurement wavelengths is allocated to fbg e for use , which corresponds to the range of temperatures that fbg e will be used to detect . in fig5 a , the range of wavelengths is illustrated as extending between λemin and λemax , with λemid signifying the middle value of the range . in practice , therefore , if the fbg e is required to detect temperatures in the range of say − 40 to 60 degrees c ., the fbg e will be constructed in the optical fibre 200 so that when the optical fibre 200 at fbg e is at − 40 degrees c ., the wavelength of light reflected by the fbg e will equal λemin , and so that when the optical fibre 200 at fbg e is at 60 degrees c ., the wavelength of light reflected by the fbg e will equal λemax . assuming linear variation of the fbg wavelength with temperature therefore fbg e will reflect light at λemid at 10 degrees . using fbg sensors in this way is well known , and the appropriate wavelengths to correspond to the desired temperature can be calculated , read off product sheets for the optical fibre , or determined by simple experiment . as shown in fig5 a , fbg e is allocated a unique and distinct range of wavelengths for the expected range of the operating parameter being measured . thus , if a light signal is received having a wavelength in the range of λemin and λemax , the controller 303 can unambiguously recognise that signal as being representative of the temperature of fbg e ( and therefore the temperature of the component at that location ) and no other . as the light signals from fbg e can always be detected unambiguously , fbg e shall be referred to as a calibration fbg . similarly , fbgs a to d and f to i are allocated respective ranges of wavelengths between λnmin and λnmax ( where n is representative of a , b , c , d , f , g , h and i ). it is assumed that each of the fbgs will operate over the same range of temperatures as fbg e , and in this example therefore , each fbg will be used to detected temperatures in the range − 40 to 60 degrees c . but at different locations of the component . as above , each fbg will be constructed so that as the temperature of the fbg varies , the wavelength of light reflected varies between the maximum and minimum allotted wavelength values . in the prior art example discussed above with reference to fig8 , each of the fbgs a to d and f to i would therefore require a unique range of operating wavelengths to be distinguished from one another and provide unambiguous temperature measurements in the manner described for fbg e . however in this case , as illustrated in fig5 a , the respective ranges of wavelengths of the fbgs a to d and f to i are overlapped with at least one adjacent fbg ( excluding fbg e ). this advantageously provides a reduction in the total range of wavelengths that must be accommodated by the fibre and the sensor system , but does mean that in certain scenarios the signals provided by each of the fbgs a to d and f to i are no longer unambiguous . as the ranges of adjacent wavelengths overlap with one another , it is possible that a light signal received from the optical fibre 200 corresponds to more than one possible value of temperature and location . calibration fbg e is therefore used to determine the expected range of temperatures measured at fbgs a to d and fbgs f to i ( this can be achieved as it assumed that the locations where the fbgs are located are thermally coupled , meaning that there will be some correspondence between temperatures at different locations ) as well as distinguish the values of the different fbgs from one another . for this reason fbgs a to d and f to i will be referred to as subsidiary fbgs , to indicate their dependence on calibration fbg e . as shown in fig5 a , fbg e is constructed to operate over wavelengths λemin to λemax . fbgs a to d are allocated lower ranges of wavelengths in comparison to the range allocated to fbg e , while fbgs f to i are allocated higher ranges . in this example therefore the range of wavelengths allocated to fbgs d and f are adjacent to that allocated to fbg e . the minimum allocated wavelength of fbg f λfmin and the maximum allocated wavelength of fbg d λdmax are separated from the range for fbg e by a tolerance value α . this tolerance value is intended to accommodate any imprecision in the manufacturing technique and allow for possible deviations in the constructed wavelength of the respective fbgs . each allocated range of wavelengths will necessarily have a midpoint λnmid around which the range is centered . taking the calibration fbg e initially , the maximum expected variation of wavelengths for fbg e is the range of wavelengths between the midpoint λemid and either λemin or λemax . in this example , the difference in the base wavelengths of each of the ranges for fbgs a to d or fbgs f to i ( that is the difference between λamin and λbmin for example ) is set to be this maximum variation for fbg e plus the tolerance alpha . this ensures that the overlapping ranges of wavelengths are not spaced out too much ( in which case the reduction in bandwidth is diminished ), but are also not too close together ( in which case the accuracy of the sensor could be impaired ). referring now to fig5 b , it can be seen that this results in ranges of wavelengths that overlap , but that for each range of wavelengths there is a central portion that remains unambiguous , and overlapping portions where for the expected range of operating temperatures , a single wavelength could fall in the range of wavelengths allocated to both of two adjacent fbgs . a number of different example modes of operation will now be explained , to illustrate how the controller 303 processes the light signals received from the optical fibre 200 and resolves any ambiguities between signals received from different fbgs . in the first example , it is assumed that the temperature of the optical fibre 200 is the same at each of the different fbg locations a to i . light source controller 400 instructs light source 301 to input light into the optical fibre 200 , and as a result light is reflected back from each of the fbgs a to i and is detected at light detector 302 . analyser 402 scans through the nine signals received from the respective fbgs a to i to detect the signal reflected back by calibration fbg e . the signal from fbg e can be distinguished from the other fbgs as ( assuming the temperature of the component has not gone outside of the expected range of temperatures ) it will always lie in the dedicated range of unique wavelengths λemin or λemax . from the measurement λe the temperature of the component at location e can be determined by analyser 402 and calculation unit 403 . this value will also be stored in memory 401 with a time stamp information . referring to fig5 b , this first temperature is denoted as t1 . as the relationship between the wavelength ranges of fbg e and fbgs a to d and f to i is known , the wavelength of the light signals reflected by the fbgs a to d and f to i when those fbgs are all at the same temperature can be calculated by the analyser and calculation unit 403 . the wavelength of light that corresponds to the same temperature as the fbg e shall be referred to as the reference wavelength for the fbg ( it will be appreciated that this will vary with variations in temperature ). as the size of the wavelength range is the same for each fbg , the difference in expected wavelengths between fbgs e and d at the same temperature can be given by the difference in the centre of the ranges ( λemid − λdmid ) for example ( the minimum or maximum values of the ranges could also be used ). similarly , the difference in expected wavelengths between fbgs e and c at the same temperature can be given by the difference in the centre of the ranges ( λemid − λcmid ) for example ( again the minimum or maximum values of the ranges could also be used ). thus , as shown in fig5 b , once the value of t1 is determined absolutely from fbg e , the wavelengths for the same temperature t1 at each of the different locations a to d and f to i can be readily determined by subtraction or addition of a respective predetermined interval . this interval will be different for each fbg range , and may be measured relative to the adjacent fbg range or to the range of wavelengths for fbg e . further , as shown in fig5 b , it will be appreciated that assuming the optical fibre is uniformly disposed at a second lower temperature t2 , the respective wavelengths of the signals reflected back by the fbgs in this case will be lower , but that the interval between the respective wavelengths will be the same in both cases . this is illustrated in fig6 a and 6 b for temperatures t1 and t2 . in use therefore , if the analyser 402 and calculation unit 403 , having determined the temperature at e also determine the regular spacing of wavelengths indicated in fig6 a and 6 b it can deduce that the optical fibre is at a uniform temperature . in fig5 b , the horizontal bars a , b c and d underneath the wavelength axis indicate how the ranges of wavelengths that can be detected at the fbgs a to d will change with temperature . as the temperature at fbg e varies the other fbg &# 39 ; s usable measurement range of wavelengths slides up or down the wavelengths available . for temperature t1 for example the analyser 402 and calculation unit 403 assume that each of the fbgs a to d are operating in the unshaded unambiguous wavelength range indicated directly underneath the wavelength axis . for , temperature t2 , those ranges of unambiguous wavelengths are shifted down . due to the assumed thermal coupling between fbg e and the other fbgs , once the temperature at fbg e is determined , the expected operating range at the other subsidiary fbgs can be readily determined . in practice , the temperature at the locations being monitored by the other fbgs a to d and i to f will not be identical to fbg e , and the signals reflected back to the light detector 302 and the analyser 402 will not exhibit the regular spacing illustrated in fig6 a and 6 b , but will be spaced irregularly as shown in fig7 . in this case , the irregular spacing is indicative of the temperature differences at each location . to determine the actual temperature of each of the fbgs , the calculation unit therefore determines the difference between the reference wavelength ( referred to as λn_ref ) of fbg n , assuming that fbg n is at the same temperature as fbg e , and the actual signal that is detected from fbg n . λn_ref is calculable once te is known , as explained above , and calculating the difference to give a temperature reading at fbg n is therefore simply a matter of subtraction or addition as shown in fig7 . this case assumes that the actual wavelengths reflected back from the various fbgs all lie in the unshaded ranges of fbg wavelengths illustrated in fig5 b . these unshaded wavelengths are unambiguous as once they are calibrated with respect to fbg e , it is possible to assume to a high degree of confidence that a received signal in that range was reflected from a particular fbg and no other . it will be appreciated for example that if the light signal falling into that wavelength range had in fact been reflected by the fbg ( n + 1 / n − 1 ) adjacent to the expected fbg n , it would indicate a very great deviation in temperature at the adjacent fbg from that which is expected . this is unlikely given the requirement that the fbg locations be thermally coupled . where signals received from the optical fibre 200 lie in the shaded region on the wavelength axis , the sensor system has two choices . in one implementation , the system simply disregards the sensor readings and gives an error message indicating that the received light signal wavelength no longer indicates an unambiguous wavelength but instead indicates one of at least two temperatures depending on which of the fbgs are believed to reflected the signal . alternatively , the analyser 402 can process the signal falling into the shaded ambiguous wavelength regions and see if the originating fbg ( and therefore the correct temperature and location can be determined ). this can be achieved in a number of ways . first , the sensor system is configured to record the temperature and wavelength indications continuously over time . in this way , a received wavelength that falls in the shaded ambiguous portion of the wavelength axis can be compared against the received wavelengths for the immediately preceding time intervals . assuming that historic values of the received wavelength originated in the unshaded region of the wavelength axis and then drifted into the shaded ambiguous region as the temperature changed , potentially ambiguous wavelength values can be resolved simply be inspection and comparison of previous values . this does however assume that the wavelengths are sampled often enough for successive values to be relatable to one another . in a more simple configuration , the analyser may simply assume that wavelength values in the ambiguous region of the wavelength range belong to the unambiguous fbg wavelength range to which they are closest . this introduces more room for error , but does mean that the analysis and processing overhead of the sensor is less . in practice , using the wavelength values in the ambiguous regions of the wavelength axis will be desirable or unnecessary depending on the degree of overlap between the adjacent ranges . it will be appreciated that taking the wavelength value that is closest to the reference value occurs ordinarily when the wavelength that is received lies in the unambiguous range of wavelengths . operating based on the closest wavelength therefore allows the system to disregard the distinction between the unambiguous and ambiguous ranges altogether . similarly , it will be appreciated that the dedicated range of wavelengths of fbg e may overlap by a small amount ( for example , by an amount less than the overlap of the wavelength ranges allocated to fbgs a and b ). again , because it is assumed that the fbg locations are thermally coupled , even when the measured wavelength for fbg e lies in a range that is also allocated to fbg d ( or fbg f ) by analysing the wavelengths of light reflected by the other fbgs the temperature at fbg can be unambiguously determined . the invention has been described with reference to example implementations , purely for the sake of illustration . the invention is not to be limited by these , as many modifications and variations would occur to the skilled person . the invention is to be understood from the claims that follow . each feature disclosed in the description , and ( where appropriate ) the claims and drawings may be provided independently or in any appropriate combination .