Method for manufacturing glass base material and glass base material grinding apparatus

Information

  • Patent Grant
  • 6565417
  • Patent Number
    6,565,417
  • Date Filed
    Thursday, October 25, 2001
    23 years ago
  • Date Issued
    Tuesday, May 20, 2003
    21 years ago
Abstract
An apparatus for grinding a glass base material having a core and a clad comprising: a grinding wheel for grinding the clad; a measuring unit for measuring an eccentricity between a center position of the glass base material and a center position of the core at a plurality of positions along a longitudinal direction of the glass base material; a design unit for calculating target diameters substantially continuous throughout the longitudinal direction of the glass base material so that the eccentricity becomes substantially zero for each of the plurality of positions; and a control unit for controlling the grinding wheel to grind the clad so that a diameter of the glass base material to be the target diameter substantially continuous throughout the longitudinal direction of the glass base material based on the target diameters calculated by the design unit.
Description




This patent application claims priority from a Japanese patent application No. 2000-327262 filed on Oct. 26, 2000, the contents of which are incorporated herein by reference.




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates to a glass base material grinding apparatus and a method for manufacturing a glass base material. More particularly, the present invention relates to a grinding apparatus and a method for manufacturing a glass base material having an excellent degree of circularity and also having an excellent eccentricity of a core.




2. Description of the Related Art




A porous glass base material, which is a base material of an optical fiber, is usually manufactured by accumulating glass particles on a surface of a core member by using a method such as the VAD (Vapor-phase Axial Deposition) method, or the OVD (Outside Vapor Deposition) method. A glass base material is manufactured by dehydrating and sintering the porous glass base material. The core member becomes a core of a glass base material after the glass base material is dehydrated and sintered. A preform is formed by elongating a glass base material, and an optical fiber is manufactured by drawing a preform.




As a method for increasing an accumulation speed of the glass particles on the surface of the core member in the OVD method, there are a method of using a burner having a large bore diameter and a method of increasing the number of burners. The burner ejects glass particles and accumulates glass particles on a surface of a core member. Furthermore, as a method for increasing the productivity of porous glass base material in the OVD method, there is a method of increasing the length of the core member to increase the ratio of the straight body part in the glass base material product. The straight body part has a uniform diameter.




The method of increasing the accumulation speed of the glass particles by increasing the bore diameter of the burner has a problem that the accumulation speed does not increase because the attachment ratio of the glass particles to the core member is extremely low at the initial process of the accumulation. Furthermore, if a plurality of burners are used, accumulation efficiency does not increase because each flame of the burners interferes with each other.




On the other hand, the method for increasing the number of burners has a problem of causing unevenness of the surface of the accumulated body of glass particles. In particular, if increasing the amount of raw material gas supplied to the burner increases the accumulation speed, the unevenness of the surface of the accumulated body becomes very significant. As a result, the optical fiber drawn from the glass base material manufactured by the OVD apparatus using an increased number of burners does not have a good optical characteristic. For example, a single mode optical fiber cannot have a desired cutoff wavelength and a dispersion characteristic.




Furthermore, in a case of the method that increases the length of the core member, the core member may bend during accumulation of the glass particles because the length of the core member is long. Thus, the resulting product cannot be used as a glass base material.




As a method for decreasing the unevenness that occurs on the surface of the glass base material and matching the center position of the core with the center position of the glass base material, there is a method of grinding the glass base material. The method of grinding the glass base material to match the center position of the core member and the center position of the glass base material is disclosed in Japanese Patent Application Laying-Open No. H9-328328 and Japanese Patent Application Laying-Open No. 2000-47039.




However, the method disclosed in Japanese Patent Application Laying-Open No. H9-328328 and Japanese Patent Application Laying-Open No. 2000-47039 could not match the center position of the core member and the center position of the glass base material when the core member is bent throughout the longitudinal direction of the glass base material.




Furthermore, the methods disclosed in Japanese Patent Application Laying-Open No. H9-328328 and Japanese Patent Application Laying-Open No. 2000-47039 have a problem that a cutoff wavelength of the optical fiber, which is drawn from the glass base material, becomes uneven through the longitudinal direction of the glass base material according to the fluctuation of the diameter of a core member through the longitudinal direction of the glass base material. This problem occurs because the methods disclosed in Japanese Patent Application Laying-Open No. H9-328328 and Japanese Patent Application Laying-Open No. 2000-47039 grind the glass base material such that the diameter of the glass base material becomes constant throughout the longitudinal direction of the glass base material.




Furthermore, when the center position of the core member is different from the center position of the glass base material, the optical fiber obtained by drawing this glass base material causes a connection loss when each end of the two optical fibers are fused and connected to construct an optical fiber network.




SUMMARY OF THE INVENTION




Therefore, it is an object of the present invention to provide a method for manufacturing a glass base material and a glass base material grinding apparatus, which is capable of overcoming the above drawbacks accompanying the conventional art. The above and other objects can be achieved by combinations described in the independent claims. The dependent claims define further advantageous and exemplary combinations of the present invention.




According to the first aspect of the present invention, an apparatus for grinding a glass base material having a core and a clad comprises: a grinding wheel for grinding the clad; a measuring unit for measuring eccentricity between a center position of the glass base material and a center position of the core in a direction perpendicular to a longitudinal direction of the glass base material at a plurality of positions along a longitudinal direction of the glass base material; a design unit for calculating target diameters of the glass base material substantially continuous throughout the longitudinal direction of the glass base material by calculating the target diameters, a center position of said target diameter is the same as the center position of the core for each of said plurality of positions along a longitudinal direction of the glass base material, so that the eccentricity becomes substantially zero for each of the plurality of positions where the eccentricity is measured by the measuring unit; and a control unit for controlling the grinding wheel to grind the clad so that a diameter of the glass base material to be the target diameter, the center position of which is at the center position of the core, substantially continuous throughout the longitudinal direction of the glass base material based on the target diameters calculated by the design unit.




The design unit may calculate the target diameter substantially continuous throughout the longitudinal direction of the glass base material by calculating the target diameter at a position between the plurality of positions where the eccentricity is measured by the measuring unit based on the eccentricity measured at the plurality of positions by the measuring unit. The design unit may calculate the target diameter at a position between the plurality of positions using the least-squares method.




The control unit may grind the clad by moving the grinding wheel back and forth in the direction toward the center of the glass base material. The control unit may rotate the glass base material around the axis of the glass base material and may move the grinding wheel back and forth toward the center of the glass base material so that movement of the grinding wheel against the glass base material forms a sine curve with an increase in an amount of rotation of the glass base material.




A number of the plurality of positions for measuring the eccentricity along a longitudinal direction of the glass base material may be substantially more than twenty.




The design unit may calculate the target diameters at each of the plurality of positions and the positions between the plurality of positions so that a ratio between a diameter of the core and a diameter of the glass base material becomes substantially constant throughout a longitudinal direction of the glass base material.




The grinding wheel may include: a coarse grinding wheel having a coarse surface; a fine grinding wheel having a fine surface; and the control unit grinds the clad using the fine grinding wheel after grinding the clad using the coarse grinding wheel.




The apparatus may further comprise a plurality of the grinding wheels, wherein the grinding wheels are arranged parallel along a longitudinal direction of the glass base material.




According to the second aspect of the present invention, a method for manufacturing a glass base material having a core and a clad comprises: accumulating glass particles around a core member, which becomes the core, to form a porous glass base material; dehydrating and sintering the porous glass base material to form a glass base material; measuring an eccentricity between a center position of the glass base material and a center position of the core in a direction perpendicular to a longitudinal direction of the glass base material at a plurality of positions along a longitudinal direction of the glass base material; calculating target diameters of the glass base material substantially continuous throughout the longitudinal direction of the glass base material by calculating the target diameters, a center position of said target diameter is the same as the center position of the core for each of said plurality of positions along a longitudinal direction of the glass base material, so that the eccentricity becomes substantially zero for each of the plurality of positions where the eccentricity is measured by the measuring; and grinding the clad with a grinding wheel so that a diameter of the glass base material to be the target diameter, the center position of which is at the center position of the core, substantially continuous throughout the longitudinal direction of the glass base material based on the target diameters calculated substantially continuous throughout the longitudinal direction of the glass base material.




Calculating may calculate the target diameter substantially continuous throughout the longitudinal direction of the glass base material by calculating the target diameter at positions between the plurality of positions where the eccentricity is measured by the measuring based on the eccentricity measured at the plurality of positions. The calculating step may calculate the target diameter at positions between the plurality of positions using the least-squares method.




The grinding may grind the clad by moving the grinding wheel back and forth in the direction toward the center of the glass base material. The grinding may rotate the glass base material around the axis of the glass base material and may move the grinding wheel back and forth toward the center of the glass base material so that movement of the grinding wheel against the glass base material forms a sine curve with an increase of an amount of rotation of the glass base material.




The measuring may measure the eccentricity along a longitudinal direction of the glass base material for more than twenty places along a longitudinal direction of the glass base material. The calculating may calculate the target diameters at each of the plurality of positions and the positions between the plurality of positions so that a ratio between a diameter of the core and a diameter of the glass base material becomes substantially constant throughout a longitudinal direction of the glass base material.




The grinding may grind the clad by a fine grinding wheel, which has a fine surface, after grinding the clad by a coarse grinding wheel, which has a coarse surface. The grinding may grind the clad using a plurality of the grinding wheels arranged parallel along a longitudinal direction of the glass base material.




The summary of the invention does not necessarily describe all necessary features of the present invention. The present invention may also be a sub-combination of the features described above. The above and other features and advantages of the present invention will become more apparent from the following description of the embodiments taken in conjunction with the accompanying drawings.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

shows a configuration of an apparatus for manufacturing a porous glass base material of an embodiment of the present invention.





FIG. 2

shows a configuration of a glass base material grinding apparatus


50


of an embodiment of the present invention.





FIG. 3

shows the glass base material grinding apparatus


50


shown in

FIG. 2

from the direction where the longitudinal direction of the glass base material


40


can be seen.





FIGS. 4A and 4B

show a result of measuring the position of the center O


1


of the core


36


inside the glass base material


40


by the measuring unit


62


.





FIG. 5

shows a result of measuring the position of the center O


1


of the core


36


inside the glass base material


40


by the measuring unit


62


.





FIG. 6

shows target diameters T


A


-T


G


for each plurality of positions A-G along a longitudinal direction of the glass base material


40


.





FIGS. 7A and 7B

show an example of the result of the design of the design unit


66


.





FIG. 8

shows the state where the grinder


30


grinds the clad


32


based on the design of the design unit


66


.




FIG.


9


A and

FIG. 9B

show another embodiment of the configuration of the glass base material grinding apparatus


50


.





FIG. 10

shows a result of measuring the above-mentioned items.











DETAILED DESCRIPTION OF THE INVENTION




The invention will now be described based on the preferred embodiments, which do not intend to limit the scope of the present invention, but exemplify the invention. All of the features and the combinations thereof described in the embodiments are not necessarily essential to the invention.





FIG. 1

shows a configuration of an apparatus for manufacturing a porous glass base material of an embodiment of the present invention. The apparatus for manufacturing a porous glass base material shown in

FIG. 1

manufactures the porous glass base material using the OVD method.




A porous glass base material manufacturing apparatus comprises chucks


80


, a motor


18


, a plurality of burners


20


, a burner guide structure


22


, a burner moving motor


24


, a reaction furnace


28


, and an exhaust hood


26


.




Each end of the core member


12


is connected to the corresponding dummy rods


10


, and each of the chucks


80


hold the corresponding dummy rods


10


. The motor


18


rotates the chucks


80


. The burners


20


accumulate the glass particles on the core member


12


. The burner guide structure


22


and the burner moving motor


24


move the burners


20


in the longitudinal direction of the core member


12


. The reaction furnace


28


accommodates the elements of the porous glass base material manufacturing apparatus such as the core member


12


and the burners


20


. The exhaust hood


26


exhausts the exhaustion gas, which is generated inside the reaction furnace


28


.




The motor


18


rotates the core member


12


by rotating the chucks


80


. The burners


20


form a clad member


14


around the surface of the core member


12


to form a porous glass base material by ejecting and accumulating the glass particles on the core member


12


, which is rotated by the motor l


8


. The burners


20


generate glass particles by ejecting a raw material gas, such as SiCl


4


, and combustion gas and hydrolyzing the raw material gas and combustion gas in the oxyhydrogen flame.




Considering the attachment of the glass particles on the core member


12


, the speed of supplying the raw material gas and the combustion gas to the burners


20


is preferably increased gradually after starting the accumulation of the glass particles.




The burner guide structure


22


is arranged parallel to the longitudinal direction of the core member


12


. The burner moving motor


24


moves the burners


20


along the longitudinal direction of the burner guide structure


22


by driving the burner guide structure


22


. Therefore, the glass particles are accumulated around the core member


12


and accumulated along the longitudinal direction of the core member


12


. The glass particles are accumulated around the core member


12


until the porous glass base material


16


has a predetermined size. Then, the porous glass base material


16


is dehydrated and sintered to be a glass base material.





FIG. 2

shows a configuration of a glass base material grinding apparatus


50


of an embodiment of the present invention.

FIG. 2

shows the glass base material grinding apparatus


50


from the direction where the cross section of a glass base material


40


, which is cut along the direction perpendicular to the longitudinal direction of the glass base material


40


, can be seen.




The glass base material


40


has a core


36


and a clad


32


. In

FIG. 2

, the position of the center O


1


of the core


36


does not match the position of the center O


2


of the glass base material


40


. The glass base material grinding apparatus


50


grinds the clad


32


of the glass base material


40


using the grinding wheel


30


until the diameter of the glass base material


40


becomes the diameter of the target clad


34


shown by the hidden line in FIG.


2


. The position of the center of the target clad


34


is identical to the position of the center O


1


of the core


36


. Thereby, the position of the center O


1


of the core


36


matches the position of the center O


2


of the glass base material.




A cylindrical grinder as shown in

FIG. 2

is preferably used as a glass base material grinding apparatus


50


of the present embodiment. The cylindrical grinder rotates an object to be grinded and grinds the outside surface of the object. The glass base material grinding apparatus


50


comprises a grinding wheel


30


, a grinding wheel driving unit


64


, a control unit


60


, and a measuring unit


62


.




While the glass base material


40


is rotated around the center O


2


as an axis, the grinding wheel


30


grinds the clad


32


. The grinding wheel


30


is connected to the grinding wheel driving unit


64


via the axis


52


. The grinding wheel driving unit


64


rotates the grinding wheel


30


around the axis


52


and also moves the grinding wheel


30


back and forth towards the center O


2


of the glass base material


40


. Thus, the grinding wheel


30


grinds the clad


32


while the grinding wheel


30


is rotated around the axis


52


and also pressed against the clad


32


.




The measuring unit


62


measures an amount of eccentricity X between the position of the center O


2


of the glass base material


40


and the position of the center O


1


of the core


36


at a plurality of positions along the longitudinal direction of the glass base material


40


. As an example of a measuring instrument, a measuring instrument using a polarizing glass or a preform analyzer may be used. The preform analyzer irradiates laser light on the glass base material


40


and obtains a refractive index distribution inside the glass base material


40


by measuring a gap of the position of the light caused while the light transmits through the glass base material


40


. The position of the center O


1


of the core


36


inside the glass base material


40


can be found from the obtained refractive index distribution.




In a case of using the measuring instrument that uses a polarizing glass as the measuring unit


62


, the measuring unit


62


is provided to the glass base material grinding apparatus


50


as a part of the glass base material grinding apparatus


50


.




Because the measuring unit


62


is connected to the control unit


60


, the measuring unit


62


can directly output the measurement result to the control unit


60


. Because the measuring unit


62


and the control unit


60


are directly connected, the time and work taken for inputting the measurement result to the control unit


60


can be greatly reduced when compared to the time and work taken for inputting the measurement results to the control unit


60


by hand. Furthermore, mistakes, which may occur while inputting the measurement results to the control unit


60


, can be prevented.




In a case of using the preform analyzer as the measuring unit


62


, the measuring unit


62


is provided separately with the glass base material grinding apparatus


50


. Furthermore, the measuring unit


62


is connected to the control unit


60


so that the measuring unit


62


can directly output the measurement result to the control unit


60


. Because the measuring unit


62


and the control unit


60


are directly connected, the time and work taken for inputting the measurement result to the control unit


60


can be greatly reduced when compared to the time and work taken to input the measurement results to the control unit


60


by hand. Furthermore, mistakes, which may occur while inputting the measurement results to the control unit


60


, can be prevented.




When the preform analyzer is used for measuring the position of the center O


1


of the core


36


, the glass base material


40


is installed inside the preform analyzer. The measuring unit


62


measures the position of the center O


1


of the core


36


inside the glass base material


40


using the preform analyzer. Then, the measuring unit


62


directly outputs the measuring result to the control unit


60


of the glass base material grinding apparatus


50


.




The apparatus used for measuring the position of the center O


1


of the core


36


inside the glass base material


40


is not limited to a preform analyzer or a measuring instrument using polarizing glass, but other types of optical measuring instruments may be used.




The control unit


60


has a design unit


66


. The design unit


66


calculates target diameters T of the glass base material


40


at each of a plurality of places where the eccentricity X is measured by the measuring unit


62


. The position of the center of the target diameter T is the same as the position of the center O


1


of the core


36


. The design unit


66


calculates target diameters T such that the position of the center O


1


of the core


36


and the position of the center O


2


of the glass base material


40


matches. Thus, the amount of eccentricity X becomes substantially zero at each of the plurality of places where the eccentricity X is measured.




Furthermore, the design unit


66


calculates the target diameter T substantially continuous throughout the longitudinal direction of the glass base material


40


by calculating the target diameter T at a place between the plurality of positions where the amount of eccentricity X is measured. The place between the positions where the amount of eccentricity X is measured is the place where the amount of eccentricity X is not measured by the measuring unit


62


. For example, the design unit


66


may calculate the target diameter T at the place between the plurality of positions where the amount of eccentricity X is measured using a least-squares method. Furthermore, the method for calculating the amount of eccentricity X at the position between the plurality of positions is not limited to the least-squares method, but other methods may also be used.




Furthermore, the design unit


66


calculates the target diameter T such that the estimated cutoff wavelength of the optical fiber obtained from the glass base material


40


becomes substantially constant throughout the longitudinal direction of the optical fiber. The estimated cutoff wavelength of the optical fiber obtained from the glass base material


40


becomes substantially constant throughout the longitudinal direction of the optical fiber when the ratio between the diameter of the core


36


and the diameter of the clad


32


is constant throughout the longitudinal direction of the glass base material


40


.




If the outside diameter of the glass base material


40


is constant throughout the longitudinal direction of the glass base material


40


, and the diameter of the core


36


is not uniform throughout the longitudinal direction of the glass base material


40


, the ratio between the diameter of the core


36


and the diameter of the clad


32


is not constant throughout the longitudinal direction of the glass base material


40


. Therefore, the cutoff wavelength of the optical fiber manufactured from this glass base material


40


does not become constant throughout the longitudinal direction of the optical fiber, and this optical fiber thus cannot be used as a product.




Thus, the estimated cutoff wavelength of the optical fiber obtained from the glass base material


40


has to be constant throughout the longitudinal direction of the glass base material


40


. Therefore, the design unit


66


calculates the target diameter T at each of the plurality of places, where the amount of eccentricity X is measured, and each of the places between each of the plurality of places, where the amount of eccentricity X is measured, so that the ratio between the diameter of the core


36


and the diameter of the clad


32


becomes constant throughout the longitudinal direction of the glass base material


40


.




Therefore, if the diameter of the core


36


varies along the longitudinal direction of the glass base material


40


, the design unit


66


calculates the target diameter T such that the outside diameter of the glass base material


40


varies according to the change in the diameter of the core


36


. Thus, the design unit


66


calculates the target diameter T such that the target diameter T varies along the longitudinal direction of the glass base material


40


if the diameter of the core


36


varies along the longitudinal direction of the glass base material


40


.




The control unit


60


controls the grinding wheel driving unit


64


so that the grinding wheel


30


moves back and forth toward the center O


2


of the glass base material


40


. The control unit


60


grinds the clad


32


by controlling the rotation speed of the grinding wheel


30


and the amount of movement of the grinding wheel


30


toward the center O


2


of the glass base material


40


with the grinding wheel driving unit


64


.





FIG. 3

shows the glass base material grinding apparatus


50


shown in

FIG. 2

from the direction where the longitudinal direction of the glass base material


40


can be seen. The glass base material grinding apparatus


50


comprises the elements explained in FIG.


2


. The glass base material grinding apparatus


50


further comprises chucks


44


A and


44


B, chuck supporting units


42


A and


42


B, and a motor


90


.




The chucks


44


A and


44


B hold each end of the glass base material


40


. The chuck supporting units


42


A and


42


B support the chucks


44


A and


44


B. The motor


90


rotates the chuck supporting units


42


A and


42


B around the center O


2


of the glass base material


40


. Therefore, the glass base material


40


is rotated around the center O


2


by the motor


90


.




While the glass base material


40


is rotated around the center O


2


, the grinding wheel


30


grinds the clad


32


. As explained in

FIG. 2

, the grinding wheel


30


rotates around the axis


52


and also moves back and forth toward the center O


2


of the glass base material


40


. Furthermore, the glass base material grinding apparatus


50


moves the glass base material


40


to the direction shown in the arrow of

FIG. 3

along the longitudinal direction of the glass base material


40


.




Thus, the grinding wheel


30


can grind the clad


32


so that the center O


1


of the core


36


and the center O


2


of the glass base material


40


substantially matches throughout the longitudinal direction of the glass base material


40


. Therefore, the grinding wheel


30


can grind the clad


32


so that the amount of eccentricity X between the position of the center O


1


of the core


36


and the position of the center O


2


of the glass base material


40


becomes substantially zero throughout the longitudinal direction of the glass base material


40


.





FIGS. 4A and 4B

show a result of measuring the position of the center O


1


of the core


36


inside the glass base material


40


by the measuring unit


62


.

FIG. 4B

shows a result of measuring the position of the center O


1


of the core


36


in the state where the glass base material


40


is rotated 90 degrees from the position of the glass base material


40


shown in FIG.


4


A.




A preform analyzer is used for the measuring unit


62


. A marking


70


is provided on the predetermined position on the surface of the clad


32


. In

FIG. 4A

, the measuring unit


62


irradiates a laser light to the glass base material


40


from the position of the marking


70


and measures the gap of the position of the light that pass through the glass base material


40


. Thereby, the measuring unit


62


can measure the refractive index distribution inside the glass base material


40


as shown in each lower part of

FIGS. 4A and 4B

. As shown in

FIGS. 4A and 4B

, the refractive index of the core


36


is higher than the refractive index of the clad


32


. Thus, the position of the center O


1


of the core


36


inside the glass base material


40


can be measured.




Furthermore, because the diameter D of the clad


32


can be obtained from the refractive index distribution shown in

FIGS. 4A and 4B

, the position of the center O


2


of the glass base material


40


can be found. The amount of eccentricity X


1


between the position of the center O


2


of the glass base material


40


and the position of the center O


1


of the core


36


can be calculated based on the position of the center O


2


of the glass base material


40


and the position of the center O


1


of the core


36


measured by the measuring unit


62


. Then, the distance r


1


from the surface of the clad


32


to the center O


1


of the core


36


is calculated based on the diameter D of the clad


32


and the amount of eccentricity X


1


.




Then, as shown in

FIG. 4B

, the glass base material


40


is rotated clockwise 90 degrees around the center O


2


of the glass base material


40


from the state shown in FIG.


4


A. Then, the position of the center O


1


of the core


36


inside the glass base material


40


is measured again. The amount of eccentricity X


2


between the position of the center O


2


of the glass base material


40


and the position of the center O


1


of the core


36


can be obtained by this measurement. Furthermore, the distance r


2


from the surface of the clad


32


to the center O


1


of the core


36


is calculated based on the diameter D of the clad


32


and the amount of eccentricity X


2


.




Thus, the position of the center O


1


of the core


36


inside the glass base material


40


is determined based on the amounts of eccentricity X


1


and X


2


between the position of the center O


2


of the glass base material


40


and the position of the center O


1


of the core


36


.





FIG. 5

shows a state of measuring an amount of eccentricity X


1


, as explained in

FIG. 4

, at a plurality of positions along the longitudinal direction of the glass base material


40


. In

FIG. 5

, the amounts of eccentricity X


1A


-X


1G


and the diameters D


1A


-D


1G


are measured at seven places from A to G, which are positioned at equal intervals along the longitudinal direction of the glass base material


40


. Therefore, the distances r


1A


-r


1G


from the surface of the clad


32


to the center O


1


of the core


36


for each measurement place from A to G can be calculated from the diameters D


1A


-D


1G


and the amounts of eccentricity X


1A


-X


1G


.




Next, similar to

FIG. 4B

, the glass base material grinding apparatus


50


rotates the glass base material


40


90 degrees around the center O


2


. The glass base material grinding apparatus


50


then measures the amounts of eccentricity X


2A


-X


2G


and the diameters D


2A


-D


2G


at seven places from A to G along the longitudinal direction of the glass base material


40


. Thus, the distances r


2A


-r


2G


from the surface of the clad


32


to the center O


1


of the core


36


for each of the measurement places from A to G are calculated based on the diameters D


2A


-D


2G


and the amounts of eccentricity X


2A


-X


2G


.




In

FIG. 5

, the amounts of eccentricity X


1


and X


2


are measured for each of seven places A to G along the longitudinal direction of the glass base material


40


as an example. However, the places for measuring the amounts of eccentricity X


1


and X


2


are not limited to the seven places. If the total length of the glass base material


40


is of a normal length, such as from 1200 mm to 1500 mm, for example, the measurement places for the amounts of eccentricity X


1


and X


2


along the longitudinal direction of the glass base material


40


is preferably more than 20 places.




If the measurement places are fewer than 20 places, the accuracy of the alignment between the position of the center O


2


of the glass base material


40


and the position of the center O


1


of the core


36


becomes worse. Furthermore, the number of places for measuring the amounts of eccentricity X


1


and X


2


are preferably more than 30 places. The numbers of the measurement places are preferably determined according to the total length of the glass base material


40


and the accuracy required for the glass base material product.




For example, if the length of the glass base material


40


is 1500 mm, the amounts of eccentricity X


1


and X


2


are measured at 50 mm intervals along the longitudinal direction of the glass base material


40


. In this case, the amounts of eccentricity X


1


and X


2


are measured at 31 places along the longitudinal direction of the glass base material


40


. Because the amounts of eccentricity X


1


and X


2


are measured for two degrees of 0 degrees and 90 degrees as shown in

FIGS. 4A and 4B

, the amounts of eccentricity X


1


and X


2


are measured at a total of 62 places.





FIG. 6

shows target diameters T


A


-T


G


for each plurality of positions A-G along a longitudinal direction of the glass base material


40


. The target diameters T


A


-T


G


are designed based on the measuring results shown in FIG.


5


.




The design unit


66


calculates the target diameters T


A


-T


G


, the position of the center of which is located at the position of the center O


1


of the core


36


, based on the amounts of eccentricity X


1A


-X


1


measured at a plurality of places A-G by the measuring unit


62


. The design unit


66


calculates the target diameters T


A


-T


G


so that each of the amounts of eccentricity X


1A


-X


1G


becomes substantially zero when the outside diameter of the clad


32


is grinded to be a target diameter T.




In

FIG. 6

, the target diameters T


A


-T


G


are shown by the hidden line. The target diameters T


A


-T


G


are the diameters of the target clad


34


at each plurality of places A-G. If the diameter of the core


36


is different for each plurality of places A-G, each of the target diameters T


A


-T


G


are also different.




Furthermore, the design unit


66


calculates target diameters T


x


at the positions between each plurality of places A-G. In

FIG. 6

, the design unit


66


calculates target diameters T


x


, the position of the center of which is at the position of the center O


1


of the core


36


, at the desired position between the measuring places A and B. The target diameters T


x


, the position of the center of which is at the position of the center O


1


of the core


36


, are also calculated at the desired positions between the measuring places B and D, C and D, D and E, E and F, and F and G.




Therefore, the design unit


66


calculates the target diameter T such that the amount of eccentricity X becomes substantially zero substantially continuous throughout the longitudinal direction of the glass base material


40


as shown by the hidden line in FIG.


6


. The design unit


66


may calculate the target diameters T


x


at the position between the plurality of places by a least-square method. The method for calculating the target diameters T


x


between the plurality of places is not limited to the least-square method, and other methods may be used.




Furthermore, it is preferable that the design unit


66


calculates the target diameters T


A


-T


G


and T


x


so that the estimated cutoff wavelength of the optical fiber obtained from the glass base material


40


becomes substantially constant throughout the longitudinal direction of the glass base material


40


. Therefore, the design unit


66


calculates the target diameters T


A


-T


G


and T


x


such that the ratio between the diameter of the core


36


and the diameter of the clad


32


becomes constant throughout the longitudinal direction of the glass base material


40


.





FIGS. 7A and 7B

show an example of the result of the design of the design unit


66


.

FIG. 7A

shows the distances r


1


and r


2


, the diameters d


1


-d


2


of the glass base material


40


, and the target diameter T at each measuring place A-G. The values of the distances r


1


and r


2


, the diameters d


1


and d


2


of the glass base material


40


, and the target diameter T shown in

FIG. 7A

are shown merely as an example and are not limited to the values shown in FIG.


7


A.




The control unit


60


inputs the values of the distances r


1


and r


2


, the diameters d


1


and d


2


, and the target diameter T from the measuring unit


62


. Thus, the control unit


60


controls the grinding wheel


30


based on the distance r


1


and r


2


, the diameters d


1


and d


2


, and the target diameter T.




The clad


32


before the clad


32


is grinded is shown by a solid line, and the target clad


34


is shown by a hidden line in FIG.


7


B. As shown in

Fig. 7B

, the value of target diameter T is determined by the distance Z. The distance Z is a distance from the position of the center O


1


of the core


36


to the position of the surface of the glass base material


40


, which is nearest from the center O


1


of the core


36


. The value of the half of the target diameter T is substantially the same as the distance Z or smaller.




The glass base material grinding apparatus


50


grinds the clad


32


so that the clad


32


shown by the solid line becomes the shape and size of the target clad


34


shown by the hidden line in FIG.


7


B. To accomplish this purpose, the control unit


60


recognizes the position of the center O


1


of the core


36


based on the distances r


1


and r


2


and grinds the clad


32


by controlling the grinding wheel


30


. The control unit


60


grinds the clad


32


such that the diameter of the glass base material


40


becomes the target diameter T, the position of the center of which is at the position of the center O


1


of the core


36


.





FIG. 8

shows the state where the grinder


30


grinds the clad


32


based on the design of the design unit


66


. The top part of

FIG. 8

shows the relationship between the position of the glass base material


40


and the position of the grinder


30


. The bottom part of

FIG. 8

shows a trail of movement of the grinder


30


.




The control unit


60


moves the grinding wheel


30


back and forth toward the position of the center O


2


of the glass base material


40


based on the target diameter T, the center of which is at the center O


1


of the core


36


, calculated by the design unit


66


. While the clad


32


is grinded, the glass base material


40


is rotated around the center O


2


of the glass base material


40


. As shown in the bottom part of

FIG. 8

, the control unit


60


moves the grinding wheel


30


so that the trace of the movement of the grinding wheel


30


against the glass base material


40


draws a sine curve according to the increase of the amount of rotation of the glass base material


40


.




To match the position of the center O


1


of the core


36


with the position of the center O


2


of the glass base material


40


, the clad


32


has to be grinded until the shape and the size of the clad


32


shown by the solid line becomes the shape and the size of the target clad


34


shown by the hidden line. Because the position of the center O


1


of the core


36


and the position of the center O


2


of the glass base material


40


is different, the center O


1


of the core


36


draws a circle having a radius of X around the center O


2


of the glass base material


40


when the glass base material


40


is rotated around the center O


2


of the glass base material


40


.




The amount of clad


32


to be grinded shown in

FIG. 8

is approximately zero in the direction about 45 degrees clockwise from the Y-axis. The amount of clad


32


to be grinded becomes approximately equal to the maximum value of 2X in the direction about 225 degrees clockwise from the Y-axis. The amount of clad


32


to be grinded becomes approximately zero again in the direction about 45 degrees clockwise from the Y-axis when the glass base material


40


is rotated in a complete circle.




In this way, the amount of clad


32


to be grinded changes periodically according to the amount of rotation of the glass base material


40


around the center O


2


. In

FIG. 8

, the rotation of the glass base material


40


for one complete circle corresponds to one period of the trace of the movement of the grinding wheel


30


shown in the bottom part of FIG.


8


.




Therefore, the control unit


60


moves the grinding wheel


30


back and forth against the glass base material


40


such that the sine curve, which shows the trace of the movement of the grinding wheel


30


, draws one period when the glass base material


40


is rotated in a complete circle around the center O


2


. The control unit


60


also sets the amplitude 2X of the sine curve according to the amount of eccentricity X between the position of the center O


1


of the core


36


and the position of the center O


2


of the glass base material


40


.




Furthermore, if it is difficult to complete the grinding process of the clad


32


during one rotation of the glass base material


40


, the control unit


60


may move the grinding wheel


30


such that the grinding wheel


30


gradually approaches the center O


2


of the clad


32


for every one rotation of the glass base material


40


. For example, the movement of the grinding wheel


30


may draw the sine curve such that the turning point of the sine curve gradually moves closer to the center O


2


of the glass base material


40


with the progress of the grinding process.




Furthermore, as shown in

FIG. 6

, the values of the target diameter T


A


-T


G


may be different for each position A-G in the longitudinal direction of the glass base material


40


. Therefore, the control unit


60


may change the amplitude 2X of the movement of the grinding wheel


30


based on the target diameter T when the glass base material


40


is moved along the longitudinal direction of the glass base material


40


.




FIG.


9


A and

FIG. 9B

show another embodiment of the configuration of the glass base material grinding apparatus


50


.

FIG. 9B

shows a top view of the glass base material grinding apparatus shown in FIG.


9


A. The glass base material grinding apparatus


50


has the same configuration as the configuration of the glass base material grinding apparatus


50


shown in

FIG. 3

except the glass base material grinding apparatus


50


shown in

FIG. 9

has a plurality of types of grinding wheels


30


A,


30


B, and


30


C.




Each plurality of the grinding wheels


30


A,


30


B, and


30


C has teeth, each of which has a different coarseness. By using a plurality of types of grinding wheels


30


A,


30


B, and


30


C, the time taken for grinding the clad


32


can be greatly reduced. As shown in

FIGS. 9A and 9B

, the plurality of types of grinding wheels


30


A,


30


B, and


30


C may be arranged along the longitudinal direction of the glass base material


40


. Furthermore, the plurality of grinding wheels


30


may be arranged in parallel along the longitudinal direction of the glass base material


40


to increase the grinding speed.




The grinding wheels


30


may include a grinding wheel


30


A having coarse teeth and a grinding wheel


30


C having fine teeth. The grinding wheel


30


B having coarseness between the grinding wheel


30


A and


30


C may be used. Moreover, the types of coarseness are not limited to the three types, but more than three types of the grinding wheels


30


may be used according to the contents of the grinding work.




A plurality of the grinding wheels


30


A and a plurality of the grinding wheels


30


C may be arranged in parallel along the longitudinal direction of the glass base material


40


. As an example of the grinding wheel


30


, a diamond wheel, which is a grinding wheel


30


using diamond, may be used. Also, a grinding wheel


30


using cubic boron nitride (CBN) may be used.




The control unit


60


of the glass base material grinding apparatus


50


shown in

FIG. 9A

controls the movement of each plurality of grinding wheels


30


A,


30


B, and


30


C, respectively, based on the target diameter T calculated by the design unit


66


. For example, the control unit


60


selects the type of grinding wheels


30


A,


30


B, and


30


C for grinding the clad


32


according to the amount of eccentricity X between the position of the center O


1


of the core


36


and the position of the center O


2


of the glass base material


40


.




The control unit


60


controls the movement of the grinding wheels


30


A-


30


C such that the control unit


60


grinds the clad


32


using the grinding wheel


30


A for coarse grinding and grinds the clad


32


using the grinding wheel


30


B for fine grinding and further grinds the clad


32


using the grinding wheel


30


C for the finest grinding.




First, the control unit


60


grinds the clad


32


deeply using the grinding wheel


30


A having coarse teeth. Secondly, the control unit


60


changes the grinding wheels


30


from the grinding wheel


30


A to the grinding wheel


30


B, which has finer teeth than the grinding wheel


30


A, and grinds the clad


32


. Finally, the control unit


60


smoothes the surface of the clad


32


using the grinding wheel


30


C having the finest teeth. Moreover, the control unit


60


may perform the coarse grinding and fine grinding at the same time by using the plurality of grinding wheels


30


A,


30


B, and


30


C at the same time.




To obtain a glass base material having a further smooth surface and an accurate core/clad ratio, a finishing grinding may be performed on the glass base material. The finishing grinding does not have to be performed using the plurality of grinding wheels


30


. A single grinding wheel


30


may be used to perform finishing grinding. Furthermore, the finishing grinding may be performed once or performed a plurality of times according to necessity.




The glass base material


40


grinded by the glass base material grinding apparatus


50


of the present embodiment is elongated to be a preform. Then, the preform is drawn to be an optical fiber.




The optical fiber obtained by drawing the glass base material, which is grinded by the glass base material grinding apparatus


50


of the present embodiment, has a good optical characteristic. In particular, a single-mode optical fiber obtained by drawing the glass base material, which is grinded by the glass base material grinding apparatus


50


of the present embodiment, has a good optical characteristic such as a good cutoff wavelength and a good dispersion characteristic.




The single-mode optical fiber obtained by drawing the glass base material, which is grinded by the glass base material grinding apparatus


50


of the present embodiment, also does not cause a connection loss when each end of two optical fibers are fused and connected to construct an optical fiber network.




EXAMPLE




A quarts glass for a single mode optical fiber having an outside diameter of 25 mmφ and a length of 1200 mm was used as a core member


12


. Both ends of the core member


12


were welded to the dummy rods


10


. Then, the core member


12


was installed to the chucks


80


provided inside the reaction furnace


28


as shown in FIG.


1


. Next, the core member


12


was rotated around the axis at the speed of 40 rpm by the motor


18


.




Next, 75 L/min of oxygen gas, 150 L/min of hydrogen gas, 9 L/min of oxygen gas as a career gas, and 40 g/min of SiCl


4


as a raw material gas were supplied to the burner


20


. A multiple-tube type oxyhydrogen flame burner was used for the burner


20


.




Furthermore, the burner moving motor


24


moved the burner


20


back and forth at the speed of 150 mm/min in a range of 1600 mm along the burner guide structure


22


. The raw material gas and the combustion gas ejected from the burner


20


were hydrolyzed with flame generated glass particles. The glass particles, which were generated by hydrolyzing SiCl


4


with flames, were accumulated on the core member


12


. The exhaust gas inside the reaction furnace


28


was emitted from the exhaust hood


26


.




The porous glass base material manufacturing apparatus increased the amount of raw material gas supplied to the burner


20


with the progress of the accumulation of the glass particles on the core member


12


. Twenty four hours after the accumulation of the glass particles had started, the porous glass base material having an outside diameter of the 240 mmφ was obtained. 180 L/min of oxygen gas, 360 L/min of hydrogen gas, 20 L/min of oxygen gas as a career gas, and 100 g/min of SiCl


4


as a raw material gas were supplied to the burner


20


just before the accumulation of the glass particles had ended. The average accumulation speed of the glass particles accumulated on the core member


12


was 31 g/min.




An uneven part existed helically around the surface of the obtained porous glass base material. By installing this porous glass base material in the furnace and dehydrating and sintering this porous glass base material, a transparent glass base material


40


having an outside diameter of 135 mmφ was obtained. When observing the surface of the glass base material


40


with the naked eye, an uneven part remained helically on the surface of the glass base material


40


. The maximum depth of the uneven part was 1.05 mm.




Next, the glass base material


40


was installed to the chucks


44


A and


44


B of the glass base material grinding apparatus


50


shown in FIG.


3


. Then, the glass base material


40


was rotated around the axis by rotating the chucks


44


A and


44


B by the motor


90


.




The measuring unit


62


measured the position of the center O


1


of the core


36


inside the glass base material


40


for each of the 50 places along the longitudinal direction of the glass base material


40


while the glass base material


40


was rotated. An optical measuring instrument using a polarizing glass was used as a measuring unit


62


.




Next, the designunit


66


calculated the position of the center O


1


of the core


36


inside the glass base material


40


substantially continuous along the longitudinal direction of the glass base material


40


. The design unit


66


calculated the position of the center O


1


of the core


36


for each place, which locates between the places where the position of the core


36


were measured, along the longitudinal direction of the glass base material


40


with estimation using the least-squares method. Therefore, the position of the center O


1


of the core


36


can be obtained substantially continuous along the longitudinal direction of the glass base material


40


by the measurement performed by the measuring unit


62


and the calculation performed by the design unit


66


.




Next, the design unit


66


calculates the target diameter T, the position of the center O


1


of which is at the position of the center O


1


of the core


36


, along the longitudinal direction of the glass base material


40


such that the estimated cutoff wavelength of the optical fiber, which is obtained by drawing the glass base material


40


, becomes 1.27 μm.




The design unit


66


output the calculated results to the control unit


60


. The control unit


60


grinded the clad


32


based on the position of the center O


1


of the core


36


measured by the measuring unit


62


and the target diameter T calculated by the design unit


66


.




As a grinding wheel


30


A for coarse grinding, a diamond wheel having a coarseness of JIS (Japanese Industrial Standards) #60 was used. The control unit


60


set the maximum grinding depth of the clad


32


by the grinding wheel


30


A to be 0.75 mm. Furthermore, as a grinding wheel


30


B, a diamond wheel having a coarseness of JIS (Japanese Industrial Standards) #140 was used. The control unit


60


set the maximum grinding depth of the clad


32


grinded by the grinding wheel


30


B to be 0.3 mm deeper than the grinded face of the clad


32


grinded by the grinding wheel


30


A.




Furthermore, as a grinding wheel


30


C, a diamond wheel having a coarseness of JIS (Japanese Industrial Standards) #600 was used. The control unit


60


set the maximum grinding depth of the clad


32


grinded by the grinding wheel


30


C to be 0.05 mm deeper than the grinded face of the clad


32


grinded by the grinding wheel


30


B.




The glass base material grinding apparatus


50


grinded the glass base material


40


once by moving the glass base material


40


with the sending speed of 50 mm/min and moving the grinding wheels


30


A-


30


C back and forth toward the center O


2


of the glass base material


40


based on the design of the design unit


66


.




The glass base material grinding apparatus


50


cooled the grinded part of the glass base material


40


with water while the glass base material grinding apparatus


50


grinded the glass base material


40


. In the above grinding process, the glass base material grinding apparatus


50


grinds the glass base material


40


such that the diameter of the glass base material


40


becomes the target diameter T, the position of the center of which is at the position of the center O


1


of the core


36


, substantially continuous along the longitudinal direction of the glass base material


40


.




The surface of the glass base material


40


became substantially smooth by this grinding process. The position of the center O


1


of the core


36


became substantially matched to the position of the center O


2


of the glass base material


40


.




Next, similar to the above-mentioned grinding process, the design unit


66


determined the finishing size of the glass base material


40


along the longitudinal direction of the glass base material


40


. The control unit


60


grinded the glass base material


40


based on the design of the design unit


66


. At this time, the diamond wheel having a coarseness of JIS (Japanese Industrial Standards) #600 was used for the grinding wheel


30


. The control unit


60


grinded the glass base material


40


once with the maximum grinding depth set to be 0.05 mm and the sending speed of the glass base material


40


to be 50 mm/min. The depth of the uneven part on the surface of the glass base material


40


obtained by this grinding was maximum 0.01 mm.




A preform was obtained by elongating the glass base material


40


, which was obtained by the above-mentioned grinding process, with the electric furnace so that the diameter of the preform was to be 45 mmφ. Furthermore, an optical fiber having an outside diameter of 125 μm was manufactured by drawing the preform.




A connection loss of this optical fiber, the eccentricity of the core


36


, and the fluctuation range of the cutoff wavelength λc along the longitudinal direction of the optical fiber were measured. The connection loss of the optical fiber was measured using the optical time domain refractometory (OTDR) method. The eccentricity of the core


36


was measured using an optical fiber structure measuring apparatus of a MODEL 2400 manufactured by Photon Kinetics Inc. The fluctuation range of the cutoff wavelength λc was measured using a cutoff wavelength measuring apparatus. ITU-T G650 was applied for measuring the fluctuation range of the cutoff wavelength λc.





FIG. 10

shows a result of measuring the above-mentioned items. As shown in

FIG. 10

, the example of the present embodiment shows better results than the results obtained by the comparative example explained below.




COMPARATIVE EXAMPLE




First, the porous glass base material manufacturing process, and the dehydrating and sintering process, the same as described in the EXAMPLE, were applied to obtain a transparent glass base material


40


having an outside diameter of 135 mmφ. The maximum depth of the uneven part on the surface of the glass base material was 1.03 mm.




Furthermore, the position of the center O


1


of the core


36


inside the glass base material


40


was measured for each 50 places along the longitudinal direction of the glass base material


40


.




The position of the center O


1


of the core


36


inside the glass base material


40


was estimated along the longitudinal direction of the glass base material


40


from the average value of the measuring result. Also, the finishing size of the glass base material


40


was determined so that the cutoff wavelength of the optical fiber obtained from this glass base material became 1.27 μm.




Next, the glass base material was installed in the glass base material grinding apparatus. The glass base material grinding apparatus grinded the glass base material so that the position of the center O


1


matched the position of the center O


2


of the glass base material. However, contrary to the EMBODIMENT, each diamond wheel did not move back and forth toward the center O


2


of the glass base material


40


while the grinding wheel grinded the glass base material. Therefore, the grinding wheel kept a constant position against the glass base material during the grinding process.




Next, similar to the EMBODIMENT, the finishing size of the glass base material was determined for the glass base material obtained by the grinding process, and the glass base material was grinded based on the determined finishing size. The diamond wheel having a coarseness of JIS (Japanese Industrial Standards) #600 was used for grinding the glass base material. The grinding depth was set to 0.05 mm, and the sending speed of the glass base material was set to 50 mm/min. The glass base material was grinded once according to the setting. The depth of the uneven part on the surface of the glass base material obtained by this finishing grinding was maximum 0.01 mm.




A preform was obtained by elongating the glass base material, which was obtained by the above-mentioned grinding process, with the electric furnace so that the diameter of the preform was 45 mmφ. Furthermore, an optical fiber having an outside diameter of 125 μm was manufactured by drawing this preform.




A connection loss of this optical fiber, the eccentricity of the core


36


, and the fluctuation range of the cutoff wavelength λc along the longitudinal direction of the optical fiber were measured as being similar to the EMBODIMENT. As shown in

FIG. 10

, the connection loss, the eccentricity of the core


36


, and the fluctuation range of the cutoff wavelength λc of the COMPARATIVE EXAMPLE became larger than those of the EXAMPLE.




As apparent from the above explanation, a glass base material having a smooth surface and an excellent core eccentricity can be manufactured in a short time according to the present invention. Therefore, the optical fiber obtained by drawing the manufactured glass base material has good optical characteristics. In particular, the single mode optical fiber obtained by drawing the glass base material manufactured by the present embodiment has a low connection loss, low core eccentricity, and good uniformity of the cutoff wavelength.




Although the present invention has been described by way of exemplary embodiments, it should be understood that those skilled in the art might make many changes and substitutions without departing from the spirit and the scope of the present invention which is defined only by the appended claims.



Claims
  • 1. An apparatus for grinding a glass base material having a core and a clad comprising:a grinding wheel for grinding said clad; a measuring unit for measuring an eccentricity between a center position of said glass base material and a center position of said core in a direction perpendicular to a longitudinal direction of said glass base material at a plurality of positions along a longitudinal direction of said glass base material; a design unit for calculating target diameters of said glass base material substantially continuous throughout the longitudinal direction of said glass base material by calculating said target diameters, a center position of said target diameter is the same as the center position of said core for each of said plurality of positions along a longitudinal direction of said glass base material, so that said eccentricity becomes substantially zero for each of said plurality of positions where said eccentricity is measured by said measuring unit; and a control unit for controlling said grinding wheel to grind said clad so that a diameter of said glass base material to be said target diameter, center position of which is at said center position of said core, substantially continuous throughout the longitudinal direction of said glass base material based on said target diameters calculated by said design unit.
  • 2. An apparatus as claimed in claim 1, wherein said design unit calculates said target diameter substantially continuous throughout the longitudinal direction of said glass base material by calculating said target diameter at a position between said plurality of positions where said eccentricity is measured by said measuring unit based on said eccentricity measured at said plurality of positions by said measuring unit.
  • 3. An apparatus as claimed in claim 2, wherein said design unit calculates said target diameter at a position between said plurality of positions using the least-squares method.
  • 4. An apparatus as claimed in claim 1, wherein said control unit grinds said clad by moving said grinding wheel back and forth in the direction toward said center of said glass base material.
  • 5. An apparatus as claimed in claim 4, wherein said control unit rotates said glass base material around the axis of said glass base material and moves said grinding wheel back and forth toward said center of said glass base material so that movement of said grinding wheel against said glass base material forms a sine curve with an increase of an amount of rotation of said glass base material.
  • 6. An apparatus as claimed in claim 1, wherein a number of said plurality of positions for measuring said eccentricity along a longitudinal direction of said glass base material is substantially more than twenty.
  • 7. An apparatus as claimed in claim 2, wherein said design unit calculates said target diameters at each of said plurality of positions and said positions between said plurality of positions so that a ratio between a diameter of said core and a diameter of said glass base material becomes substantially constant throughout a longitudinal direction of said glass base material.
  • 8. An apparatus as claimed in claim 1, wherein said grinding wheel includes:a coarse grinding wheel having a coarse surface; a fine grinding wheel having a fine surface; and said control unit grinds said clad by said fine grinding wheel after grinding said clad by said coarse grinding wheel.
  • 9. An apparatus as claimed in claim 1, further comprising a plurality of said grinding wheels, wherein said grinding wheels are arranged parallel along a longitudinal direction of said glass base material.
  • 10. A method for manufacturing a glass base material having a core and a clad comprising:accumulating glass particles around a core member, which becomes said core, to form a porous glass base material; dehydrating and sintering said porous glass base material to form glass base material; measuring an eccentricity between a center position of said glass base material and a center position of said core in a direction perpendicular to a longitudinal direction of said glass base material at a plurality of positions along a longitudinal direction of said glass base material; calculating target diameters of said glass base material substantially continuous throughout the longitudinal direction of said glass base material by calculating said target diameters, a center position of said target diameter is the same as the center position of the core for each of said plurality of positions along a longitudinal direction of the glass base material, so that said eccentricity becomes substantially zero for each of said plurality of positions where said eccentricity is measured by said measuring; and grinding said clad with a grinding wheel so that a diameter of said glass base material to be said target diameter, said center position of which is at said center position of said core, substantially continuous throughout the longitudinal direction of said glass base material based on said target diameters calculated substantially continuous throughout the longitudinal direction of said glass base material.
  • 11. A method as claimed in claim 10, wherein said calculating calculates said target diameter substantially continuous throughout the longitudinal direction of said glass base material by calculating said target diameter at positions between said plurality of positions where said eccentricity is measured by said measuring based on said eccentricity measured at said plurality of positions by said measuring.
  • 12. A method as claimed in claim 11, wherein said calculating calculates said target diameter at positions between said plurality of positions using the least-squares method.
  • 13. A method as claimed in claim 10, wherein said grinding grinds said clad by moving said grinding wheel back and forth in the direction toward said center of said glass base material.
  • 14. A method as claimed in claim 13, wherein said grinding rotates said glass base material around the axis of said glass base material and moves said grinding wheel back and forth toward said center of said glass base material so that movement of said grinding wheel against said glass base material forms a sine curve with an increase of an amount of rotation of said glass base material.
  • 15. A method as claimed in claim 10, wherein said measuring measures said eccentricity along a longitudinal direction of said glass base material for more than twenty places along a longitudinal direction of said glass base material.
  • 16. A method as claimed in claim 10, wherein said calculating calculates said target diameters at each of said plurality of positions and said positions between said plurality of positions so that a ratio between a diameter of said core and a diameter of said glass base material becomes substantially constant throughout a longitudinal direction of said glass base material.
  • 17. A method as claimed in claim 13, wherein said grinding grinds said clad by a fine grinding wheel, which has a fine surface, after grinding said clad by a coarse grinding wheel, which has a coarse surface.
  • 18. A method as claimed in claim 13, wherein said grinding grinds said clad using a plurality of said grinding wheels arranged parallel along a longitudinal direction of said glass base material.
Priority Claims (1)
Number Date Country Kind
2000-327262 Oct 2000 JP
US Referenced Citations (7)
Number Name Date Kind
4053237 Casey Oct 1977 A
5111571 Ciboldi et al. May 1992 A
5741172 Trionfetti et al. Apr 1998 A
5909530 Ohkubo et al. Jun 1999 A
6257964 Helgren Jul 2001 B1
6273783 Kim Aug 2001 B1
6411861 Clewes et al. Jun 2002 B1
Foreign Referenced Citations (3)
Number Date Country
0 976 689 Feb 2000 EP
9-328328 Dec 1997 JP
2000-47039 Feb 2000 JP
Non-Patent Literature Citations (1)
Entry
European Search Report dated Feb. 26, 2002.