Method of measuring distribution of crystal grains in metal sheet and apparatus therefor

Abstract: In measuring a distribution of crystal grains in metal sheet, an exciting frequency (f) of ultrasonic wave is determined such that a wave length of the ultrasonic wave propagated in a direction of the sheet thickness of the grains each having an aimed orientation is set at a value of the doubled sheet thicknesses (2d) multiplied by about integral times or about half integral times, burst-­ like ultrasonic pulses having this frequency and including two or more waves are caused to incide into the direction of the sheet thickness by use of an ultrasonic probe moving relatively with a body (11) to be measured, multiple reflected waves generated from the bottom and top faces of the metal sheet upon the reflection from the sheet surface are caused to interfere with each other, the multiple reflected waves, which have interferred with each other, are detected, orientation of the grains in the metal sheet (11) are estimated from the magnitudes in amplitude of the interferent multiple reflected waves thus detected, and the distribution of the grains in orientation in various portions, into which the ultrasonic wave incides, is detected two-dimensionally.

Description: The present invention relates to a method of measuring a distribution of crystal grains in a metal sheet and an apparatus therefor. More particularly, the present invention relates to a highly practical method of measuring a distribution of crystal grains in a metal sheet and an apparatus therefor, suitable for use in producing an anisotropic silicon steel sheet high in electromagnetic properties in a rolling direction, capable of non-destructively measuring the distribution of crystal grains in orientation of the anisotropic silicon steel sheet on line. For the purpose of applying it to a core of an AC step-up transformer and the like, there has been produced an anisotropic silicon steel sheet high in electromagnetic properties in the rolling direction. This anisotropic silicon steel sheet is producted by obtaining the crystal grains directed in a so-called GOS orientation, in which a plane {110} is in parallel to the sheet surface and a direction 〈100〉 is in parallel to the rolling direction. The more the number of the grains close to the GOS orientation is, the higher the electromagnetic properties of the anisotropic silicon steel sheet are. However, in the actual manufacturing process, it is not necessarily possible to produce only grains close to the GOS orientation. Due to a change in the conditions of manufacture or a disturbance, grains greatly shifted from this GOS orientation, i. e. so-called abnormal grains, are formed. Fig. 14 shows an example of a product 10 including the abnormal grains 10A. A normal grain 10B close to the GOS orientation has a grain diameter as large as several mm - several 10 mm, however, the abnormal grain 10A has a grain diameter of several mm or less in general, the orientation of the grain is directed in random directions, and such grains are distributed along the rolling direction as shown in Fig. 14. In the manufacturing process of the above-described anisotropic silicon steel sheet, as instruments for detecting the electromagnetic properties of the product, an Epstein detector and a single sheet tester are used off line, while, a continuous iron loss tester is used on line, thus measuring an iron loss of the steel sheet and a density of magnetic fluxes. However, the aforesaid measuring instruments can measure only the mean electromagnetic properties in the widthwise direction of the steel sheet, but cannot measure the distribution of the abnormal grains 10A. On the other hand, as a method of measuring the distribution of the abnormal grains of the silicon steel sheet, there is a macro-etch method, wherein the product is cut into strip-like forms, an insulation coating film on the surface thereof is peeled off and the surface is etched by use of a Nital etchant, whereby the fact that etched effects are different in accordance with the orientations of the crystal grains is utilized, so that the distribution of the crystal grains is observed. However, application of this macro-etch method is limited to off line, and cannot be applied on-line. Morever, it is necessary to cut the product into the strip-like forms. Further, etching can be made only after the insulation coating film is peeled off. Thus, much labor is needed, and there is the problem of handling such as a treatment of chemicals. In addition, since this is a destructive test and a sampling inspection, the quality of the product over the total length thereof cannot be ensured. Further, such a problem is presented that the efficiency is low and so forth from the viewpoint of the type of working. On the other hand, as a technique relevant to the present invention, there has been proposed a method of non-destructively testing the characteristics of a steel sheet by the utilization of propagation characteristics of ultrasonic waves in the crystal grains. More specifically, in general, a sonic speed v of a longitudinal ultrasonic wave propagated in a direction 〈n₁ , n₂, n₃〉 of a body of equi-axed (equi-axial) crystal is given as a root of the following equation. ( ρ V ² - C ₄₄ ) ³ - a ( ρ V ² - C ₄₄ ) ² + c ( a + b ) ( n ₁ ² n ₂ ² + n ₂ ² n ₃ ² + n ₃ ² n ₁ ² ) ( ρ V ² - C ₄₄ ) - C ² ( a + 2 b ) n ₁ ² n ₂ ² n ₃ ² = O (1) where n₁, n₂, and n₃ are direction cosines between the propagation direction and the principal axis of the crystal, and a, b and c are shown in the following equations, respectively. a = C ₁₁ - C ₄₄ (2) b = C ₁₂ + C ₄₄ (3) c = C ₁₁ - C ₁₂ - 2 C ₄₄ (4) where Cij is an ij component of an elastic matrix. Accordingly, steel is supposed to be a body, and an elastic constant of steel is given, whereby a sonic speed v of the longitudinal ultrasonic wave propagated in a single crystal in various directions can be calculated from the equation (1). Fig. 15 shows examples of calculated results in the form of a stereo-projection drawing. The sonic speed v differs in accordance with the propagated directions of the ultrasonic wave, which is known from the results. Therefore, the sonic speed v is measured, so that the orientation of the crystals can be determined to a certain extent. For example, when the direction of the sheet thickness is given as Z-axis, a sonic speed v in the direction of Z-axis is measured and, when the measured value is 6500 m/s, it can be said that, in this body, an axis [111] of the crystal is laid in the direction of the sheet thickness. As a conventional example of the measurement of the characteristics of a material by the utilization of the characteristics of the ultrasonic wave propagated in a crystal as described above, there is a method of discriminating a cast structure by the ultrasonic wave as disclosed in Japanese Unexamined Patent Application Publication No. 126992/1978. According to this method, a propagation time of the ultrasonic wave in the direction of the sheet thickness of a poly crystalline body is measured, and from this measured value, a thickness of a columnar crystal and a thickness of an equi-axed crystal are estimated. When a sonic speed in the direction of sheet thickness of a body is to be measured in general, as shown in Fig. 16, an ultrasonic wave is introduced into a body 11 to be measured in the direction of sheet thickness by use of an ultrasonic probe 12, a time interval t of a row of bottom echoes B1, B2 and B3 which are produced thereby as shown in Fig. 17, for example, is measured, and the sonic speed v is calculated by the following equation. v = 2d / t (5) where d indicates a sheet thickness of the body 11. In addition, S denotes a signal produced by a surface reflected wave. However, also in this method, when the sheet thickness reaches a length close to a wave length of the ultrasonic wave, B1, B2 and B3 in the row of bottom echoes overlie one another, the problem that the time interval t cannot be measured is presented. For example, if a frequency of the ultrasonic wave is 10 MHz, the wavelength of the longitudinal wave is about 0.6 mm, and the steel sheet thickness d is 0.1 to 0.5 mm, then this method is not applicable. In order to apply this method, it is necessary to use short pulses and a frequency of the ultrasonic waves of 100 MHz or above, raising problems of costly electric circuits, large attenuation of the ultrasonic waves and the like, so that this method becomes impractical. On the other hand, as shown in Fig. 18 for example, a method not utilizing the series of bottom echoes has been proposed. In this method, the body 11 to be measured is interposed between a transmitting element 12A and a receiving element 12B and a penetration (transmission) time difference ti of the ultrasonic waves is measured. In this case, the relationship between the penetration time difference ti and the sonic speed v is shown by the following equations:- ti = d/v + (L₁ + L₂)/v₀ (6) Δti = dΔv/v² (7) Accordingly, when the sonic speed v is to be determined at an accuracy of 1% for example, the sonic speed v = 6000 m/s, sheet thickness d = 0.3 mm and Δv/v = 0.01 are substituted into the equation (7) to obtain Δti = 5 x 10⁻¹⁰ sec. In this example, it is necessary to keep the distance between the ultrasonic probes 12A and 12B constant to within only 0.75 µm. This value is not unachievable in a research laboratory; however, it is very difficult to achieve in practical use. EP-A-0 155 630 discloses an ultrasonic measurement method of the above type, for medical use. GB-A-2 144 551 discloses a method of determining grain size in steel, wherein ultrasonic waves are propagated through the steel and the diameter of grains demarcated at high-angle grain boundaries is determined. In this method,the reflected ultrasonic waves do not interfere and their amplitudes are measured separately. The present invention has been developed in view of the above-described disadvantages of the prior art. The inventors perceived a need to provide a practical method and apparatus for measuring the distribution of crystal grains in a metal sheet, in which it is possible to efficiently detect the distribution of abnormal grains non-destructively and on-line, and to ensure the quality over the total length of the sheet, without having to cut the sheet into strips and peeling off the insulation coating film as in the macro-etch method. According to a first aspect of the present invention, there is provided a method of measuring the two-dimensional distribution of crystal grain orientation in a metal sheet, as defined in claim 1. According to a second aspect of the present invention, there is provided a method of measuring the two-dimensional distribution of crystal grain orientation in a metal sheet, as defined in claim 2. According to a third aspect of the present invention, there is provided an apparatus for measuring the two-dimensional distribution of crystal grain orientation in a metal sheet, in combination with said metal sheet, as defined in claim 5. Preferably, the ultrasonic probe is a focus-type ultrasonic probe capable of converging (focusing) the ultrasonic waves to a focal position substantially coincident with the center of the sheet thickness. According to a fourth aspect of the present invention, there is provided an apparatus for measuring the two-dimensional distribution of crystal grain orientation in a metal sheet, in combination with said metal sheet, as defined in claim 6. Preferably, an ultrasonic wave reflecting portion of the reflecting plate is concave such that ultrasonic waves reflected by this concave surface are again focused at about the center of the sheet thickness. Recognising the disadvantages of the conventional ultrasonic wave method, the inventors of the present invention have realized that, without detecting the sonic speed of the ultrasonic wave per se, a change in the sonic speed can be revealed by the intensity of the interference when ultrasonic waves are allowed to interfere. This intensity can be detected, so that information corresponding to the speed of sound within the metal sheet can be extracted. More specifically, as shown in Fig. 2, when ultrasonic pulses vertically impinge on a sheet of thickness d from the probe 12 through a contacting medium (water for example), reflection and transmission of the pulses occur at both the upper and lower surfaces of the sheet, whereby multiple reflected pulses are observed. When the frequency of the ultrasonic waves is such that their wavelength and the sheet thickness d are about equal in magnitude, the multiple reflected pulses overlie each other, whereby interference occurs as shown in Fig. 3. In this interference, when the multiple reflected pulses are out of step, i.e. have a phase difference of 180°, they offset (cancel) each other (interferent multiple reflected pulses signal Bb'). On the other hand, when the multiple reflected pulses are in step, i.e. have a phase difference of 0°, they reinforce each other to a maximum extent (interferent multiple reflected wave signal Ba'). In Fig. 3, Sa' and Sb' each denote a surface reflected pulse signal. The condition of interference is established when an exciting frequency f of the ultrasonic wave satisfies the following equation:- f = v/2d (8) In order for the ultrasonic waves to interfere, the incident ultrasonic wave must include at least two periods, i.e. a burst-like pulse. The normal grains in a silicon steel sheet take the GOS orientation. In this case, the crystal axis in the direction of the sheet thickness is 〈110〉 and the sonic speed in this direction is 6200 m/s. Then, when the sheet thickness d is set at 0.3 mm, the exciting frequency of the ultrasonic wave f at 10. 33 MHz and the number of the burst periods at 10, if the relationship between the sonic speed v and the intensity of the interferent multiple reflected bursts is calculated, then the result as shown in Fig. 4 is obtained. The normal grains in the anisotropic silicon steel sheet take the GOS orientation, and shifts in orientation are within 10° at the most. When this is converted into a sonic speed in the direction of the sheet thickness, the distribution of 6200 ± 50 m/s is obtained. Accordingly, the intensity of the interferent multiple reflected waves is monitored, and, when it becomes lower than a certain value, it is possible to determine the presence of the abnormal grains. In actuality, as shown in Fig. 14, the abnormal grains 10A have very small grain diameters as compared with those of the normal grains 10B and the distribution thereof is concentrated, and the orientations of the respective grains are random. Accordingly, even if a threshold value for detecting only the grains having orientations 〈111〉 and 〈100〉 is adopted, the distribution of the abnormal grains can be detected. A first point to be noted in working the present invention is that, as shown in Fig. 3, the interferent multiple reflected bursts Ba' and Bb' occur after surface reflected bursts Sa' and Sb' which are first reflected waves of the incident wave at the boundary between the surfaces of a contact medium (water) and the body to be measured (metal sheet) and have high amplitudes, so that the surface reflected bursts should not be detected. The following methods permit the detection of only the interferent multiple reflected bursts without detecting the upper surface reflected burst of the body to be measured: (a) As shown in Fig. 5, a transmitting element 12A and a receiving element 12B located respectively above and below the body 11 to be measured, are provided for detecting the penetrating ultrasonic wave (Transmission method). With this arrangement, the surface reflected burst reflected at the upper surface of the body 11 and having high intensity do not reach the receiving element 12B. Accordingly, a received signal is limited to only an interferent multiple burst signal T1, and the peak thereof is easily detected, as shown in Fig. 6. As shown in Fig. 5, a focus type ultrasonic probe capable of converging the ultrasonic wave is used as the ultrasonic probe 12, and the focal position thereof is made substantially coincident with the center of the sheet thickness of the body 11, so that a spatial resolution in measuring can be impoved. (b) As shown in Fig. 7, the ultrasonic probe 12 providing both the transmitting and the receiving elements is provided on one side and a reflecting plate 14 having a thickness not allowing the multiple reflected bursts to interfere therewith is provided on the other side, with the body 11 to be measured therebetween, whereby the ultrasonic wave is reflected by the reflecting plate 14, so that the magnitude of a signal obtained by the ultrasonic wave having penetrated through the body 11 again can be detected (Reflecting plate method). In this case, signals received by the ultrasonic probe 12 are shown in Fig. 8, and, out of these signals, R1 is a signal to be detected, and still, the surface reflected wave B reflected by the upper surface of the body 11 and having the high intensity is not included. Accordingly, by a gate signal B shown in the bottom stage in Fig. 8, it becomes easy to detect a peak of the aimed interferent multiple wave signal R1. In Fig. 8, Sa indicates a signal reflected by the surface of the body 11, and Ba denotes interferent multiple echoes occurring upon the occurrence of Sa. This Ba can be taken out by a gate signal A shown in the middle stage in Fig. 8. According to this reflecting plate method, as shown in Fig. 9, a portion of the reflecting plate 14, to which the ultrasonic wave is applied, is formed into a concave surface 14A, whereby the ultrasonic wave is focused at about the center of the sheet thickness of the body 11 again, so that the spatial resolution in measuring can be improved. According to the above-described two methods (a) (b), not only the interferent multiple reflected waves are easily detected, but also, when the present invention is applied to an on-line measurement, even if the body 11 is displaced vertically, the influence thereof can be advantageously minimized. In addition, when the influence of the surface reflected burst reflected by the upper surface of the body 11 and having high intensity is not a problem, or, when the influence can be removed by other means such as a gate circuit and the like, the simple arrangement of a reflection method as shown in Fig. 2 can be adopted. In the foregoing, there has been described the case of the condition where the wave length of the ultrasonic wave propagated in the direction of the sheet thickness of the crystal grains each having the normal direction is set at a value of the doubled sheet thicknesses multiplied by just integral times or just half integral times, so that the interference of the multiple reflected waves with the grains each having the normal orientation is increased, while, the interference with the grains each having the abnormal orientation is decreased. However, in the anisotropic silicon steel sheet, almost all of the grains are directed in the same orientation, and it was theoretically and experimentally ascertained that, when the orientation of the normal crystal grains was to be detected, it was preferable that the wave length of the ultrasonic wave was set at a value slightly shifted from the value of the doubled sheet thicknesses multiplied by the integral times. More specifically, in Fig. 4, a frequency (10.33 MHz) of the ultrasonic wave is determined so that the wave length of the ultrasonic wave propagated in the direction of [110] can be set at a value of the twice (0.6 mm) of the sheet thickness (0.3 mm). In this case, as against the sonic speed (6200 m/s) of the crystal grains in the normal orientation, the intensity of the interferent multiple reflected waves becomes maximal and a dwelling point thereof is formed, whereby a change in the reflected intensity is low against a very small change in the sonic speed, so that an unsatisfactory sensitivity is shown. In contrast thereto, an example of the relationship between the sonic speed and the intensity of the reflected waves when the frequency of the ultrasonic wave is slightly shifted to 10.66 MHz (0.58 mm in terms of the wave length) is shown in Fig. 10. As apparent from Fig. 10, against a change in the sonic speed of the grains in the normal orientation in the vicinity of 6200 m/s, a change in the intensity of the interferent multiple reflected waves is high, so that a measurement with high sensitivity of the grains in the normal orientation can be performed. A second point to be noted in working the present invention is that, in order to cause the interference to easily occur, it is necessary to adopt two or more continuous periods (burst-like pulse) as the incident wave as shown in Fig. 11, instead of a single period. In terms of the interference, the more the number of periods is, the better the influence condition is. However, there are the problems of the longer duration of the surface reflected waves and the longer measuring time, so that the number of periods in the burst can be set at about 10 to 20 waves actually. According to the present invention, the distribution ofthe grains in the abnormal orientation of the metal sheet can be detected non-contactingly, non-destructively and rapidly. Accordingly, the disadvantages of the conventional macro-etch method can be obviated, that is, the working of peeling off the insulation coating film and the working of treating the chemicals for etching become unnecessary. Furthermore, the processing time of the inspection is shortened considerably. In the past, there has been no practical technique to be applied to on-line, however, application of the present invention to on-line makes it possible to conduct the inspection over the total length relating to the abnormal grains of the product. Further, in a subsequent manufacturing step, e.g. a slitter step, portions having abnormal grains can be removed, whereby only portions having normal grains are accepted as the product, so that excellent products can be delivered. Reference is made, by way of example, to the accompanying drawings, in which like reference characters designate the same or similar parts throughout the figures thereof and wherein: Fig. 1 is a block diagram, partially including oblique view, showing the arrangement of one embodiment of the apparatus for measuring the distribution of the crystal grains in metal sheet according to the present invention; Fig. 2 is a typified view of the sonic speed measurement utilizing the interferent multiple reflections, for explaining the principle of the present invention; Fig. 3 is a chart showing an example of the measured wave forms by the interferent multiple reflection; Fig. 4 is a chart showing an example of the relationship between the intensity of the interferent multiple reflected waves and the sonic speed, for explaining the principle of the present invention; Fig. 5 is a sectional view showing the essential portion of an example of the method of the present invention utilizing the transmission method; Fig. 6 is a chart showing an example of the received wave forms obtainable by the method of the present invention as shown in Fig. 5; Fig. 7 is a sectional view showing the essential portion of another example of the method of the present invention utilizing the reflecting plate method; Fig. 8 is a chart showing an example of the received wave forms obtainable by the method of the present invention as shown in Fig. 7; Fig. 9 is a sectional view showing the essential portion of an improved example of the method of the present invention utilizing the reflecting plate method; Fig. 10 is a chart for showing the effects in the case where the frequency of the ultrasonic wave is slightly shifted in relation to the condition shown in Fig. 4; Fig. 11 is a chart showing an example of the burst-like pulse form of the incident pulse according to the present invention; Fig. 12 is a perspective view showing an example of the scanning method of the ultrasonic probe in the embodiment shown in Fig. 1; Fig. 13 is a chart showing an example of the result of measuring the distribution of the abnormal grains in the above embodiment; Fig. 14 is a perspective view showing the silicon steel sheet containing therein the abnormal grains in a typified manner; Fig. 15 is a stereo-projection view showing the changes in the sonic speed according to the orientations in the single crystal in the silicon steel; Fig. 16 is a sectional view showing the conventional sonic speed measurement utilizing the multiple reflections, in a typified manner; Fig. 17 is a chart showing examples of the measured wave forms by the sonic speed measurement utilizing the multiple reflections; and Fig. 18 is a sectional view showing the conventional sonic speed measurement utilizing the transmission method, in a typified manner. One embodiment of the present invention will hereunder be described in detail with reference to the accompanying drawings. The embodiment of the apparatus by the reflecting plate method according to the present invention is arranged as shown in Fig. 1. A timing control circuit 22 outputs repetition pulses at a rate of 1 - 10 KHz for example, in association with a probe scanning speed of a scanner 26. A pulser 20 produces an electric signal of about 10 burst waves having a frequency f given by an equation of f = v / 2d , in synchronism with pulses from the timing control circuit 22. An ultrasonic probe 12 combining transmitting and receiving elements as shown in Fig. 7 transduces the electric signal from the pulser 20 into an ultrasonic signal and directs the same into a body 11 to be measured. The ultrasonic probe 12 is generally immersed in water together with the body 11, for example. Further, the scanner 26 causes the ultrasonic probe 12 to scan the surface of the body 11 in the two-dimensional directions. A reflecting sheet 14 as shown in Fig. 7 is disposed beneath the body 11. Ultrasonic reflected waves from the top and bottom faces of the body 11 are reflected by the reflecting plate 14 and return again to the ultrasonic probe 12 to be converted into electric signals therein. A receiver 28, upon receiving the electric signals from the ultrasonic probe 12, suitably amplifies the electric signals and outputs the same into a gate circuit 30. The gate circuit 30, in synchronism with a pulse from the timing control circuit 22, opens the gate circuit 30 with a predetermined delay, to thereby allow only the interferent multiple reflected signal R1 shown in Fig. 8 to be passed to a peak hold circuit 32. The peak hold circuit 32, in synchronism with a pulse from the timing control circuit 22, detects a peak value of the signals from the gate circuit 30 during one repetition time until the following pulse comes, and holds the peak value for one repetition time. Because a duration of the ultrasonic signal is only in 1 micro second order, a duration of the detected signals is lengthened in this peak hold circuit 32, so that analog-digital (A/D) conversion by an A/D converter 34 is facilitated. The A/D converter 34 converts an analog signal from the peak hold circuit 32 into a digital signal in synchronism with a pulse from the timing control circuit 22 and outputs the same into a micro-processor 36. The micro-processor 36 receives the digital signal from the A/D converter 34 and a probe position signal from the scanner 26, determines whether the grains are normal or abnormal from the magnitude of the interferent multiple reflected wave signal R1, and outputs the result into a display unit 38. Preferably, the apparatus for measuring the distribution of the crystal grains in orientation according to the present invention is assembled into a controller used for a preceding or following manufacturing step, whereby on-line control can be directly performed in accordance with the result of measuring. In this case, the display unit 38 may be dispensed with. The operation of this embodiment will hereunder be described with reference to an example where a silicon steel sheet having a sheet thickness d = 0.3 mm is measured. In this embodiment, the scanner 26 causes the ultrasonic probe 12 to scan the surface of the steel sheet 11 in the two-dimensional directions as shown in Fig. 12. Now, when a relative speed during scanning is set at 1 m/s, a scanning pitch at 0.5 mm and the repetition frequency of the pulse from the timing control circuit 22 at 2 KHz, the ultrasonic wave enters into the steel sheet 11 at a rate of one per square of 0.5 mm by 0.5 mm. The grain diameter of the crystal grain in the sheet plane of the anisotropic silicon steel sheet in the abnormal grain portion is 0.5 - 1 mm, and that in the normal grain portion is more than this. Therefore one or more ultrasonic pulses pass through almost all the crystal grains, so that the magnitude of the interferent multiple reflected wave signal for all of the grains can be measured. Furthermore, when the focus type ultrasonic probe capable of converging the ultrasonic wave is used as the ultrasonic probe 12 and the focal position is made substantially coincident with the center of the sheet thickness of the steel sheet 11 , an ultrasonic wave beam having a diameter of about 0.5 mm can be easily obtained, and further, the distance between the steel sheet 11 and the probe 12 can be made as much as the focal length (several mm - several ten mm). Next, while the scanning of this type is being performed, the intensities of the interferent multiple reflected bursts R1, are successively detected by this embodiment. When the frequency f of the ultrasonic wave is set at 10.33 MHz, the relationship between the intensity of reflection and the sonic speed in each of the crystal grain is the same as that shown in Fig. 4. Accordingly, when this intensity of reflection is displayed in synchronism with the scanning portion, this distribution pattern of the intensity represents the distribution of the crystal grains in orientation. Accordingly, determination can be made whether the product is good or bad in quality from the distribution of the measured values. Fig. 13 shows a case in which, when the number of burst waves of the ultrasonic wave is set at 10, only the portions having abnormal grains are drawn black as an example of the result of measuring according to this embodiment. It can be ascertained that this result of measuring corresponds well to the result of measuring by the conventional macro-etch method. As described above, according to the present invention, the portion of the abnormal grains can be detected with high accuracy and non-destructively. This embodiment is arranged such that a single ultrasonic probe 12 is combined with the reflecting plate 14 for use as shown in Fig. 7 (reflecting plate method), whereby, it is possible to measure from one side, so that it is advantageous in on-line measurement in particular. Incidentally, the arrangement for transmitting and receiving the ultrasonic wave is not limited to this, and such an arrangement that, as shown in Fig. 5 for example, an ultrasonic probe functioning as the transmitting element 12A and an ultrasonic probe functioning as the receiving element 12B are provided at positions opposed to each other, with the body 11 to be measured therebetween (transmission method). Furthermore, as shown in Fig. 2, an arrangement wherein the reflecting sheet 14 is dispensed with (simple reflection method) may be adopted. Furthermore, in the above embodiment, one ultrasonic probe 12 has been used, however, when the body 11 to be measured is moved as in the on-line measurement and high speed measurement is required, a plurality (or a plurality of pairs) of ultrasonic probes may be used to increase the speed of measuring. Incidentally, in the above embodiment, the frequency f of the ultrasonic wave has been determined such that the phases agree with each other when the speed is in the direction 〈110〉. However, the frequency f may be determined such that the phases are shifted from each other by 180° , or, on the contrary, the frequency f may be determined in conformity with the speed of the abnormal orientation.

Claims: A method of measuring the two-dimensional distribution of normal and abnormal crystal grain orientation in a metal sheet (11), comprising steps of:- scanning an ultrasonic generator (12) two-dimensionally over one surface of the sheet whilst generating burst-like ultrasonic pulses, each burst having a plurality of periods and producing multiple reflected bursts reflected at the surfaces of the sheet, the ultrasonic frequency f and number of periods of each burst being chosen to cause interference between the multiple reflected bursts, wherein said frequency f is determined as: f = n.v/(2.d) or as a value slightly shifted therefrom, where n = integer or half-integer, v = speed of sound in a normal or abnormal crystal grain orientation, and d = thickness of the metal sheet; detecting the signal (T₁) effected by the interfering multiple reflected bursts caused by one incident burst and exiting through the other surface of the sheet (11); measuring the amplitude of the detected signal (T₁), said amplitude representing the measured speed of sound in the metal sheet, which speed depends on the orientation of grains in the metal sheet; and determining from said amplitude the grain orientation in the portion of the metal sheet (11) currently being scanned, whereby the two-dimensional distribution of grain orientation is constructed. A method of measuring the two-dimensional distribution of normal and abnormal crystal grain orientation in a metal sheet (11), comprising steps of:- scanning an ultrasound generator (12) two-dimensionally over one surface of the sheet whilst generating burst-like ultrasonic pulses, each burst having a plurality of periods and producing multiple reflected bursts reflected from the surfaces of the sheet, the ultrasonic frequency f and number of periods of each burst being chosen to cause interference between the multiple reflected bursts, wherein said frequency f is determined as: f = n.v/(2.d) or as a value slightly shifted therefrom, where n = integer or half-integer, v = speed of sound in a normal or abnormal crystal grain orientation, and d = thickness of the metal sheet; detecting the signal (S, B, R₄, R₂) effected by the interfering multiple reflected bursts caused by one incident burst and exiting through said surface of the sheet (11), and processing the detected signal (S, B, R₁, R₂) to remove a signal (S) representing a wave reflected directly from said surface; measuring the amplitude of the processed detected signal (B, R₁), said amplitude representing the measured speed of sound in the metal sheet, which speed depends on the orientation of grains in the metal sheet; and determining from said amplitude the grain orientation in the portion of the metal sheet (11) currently being scanned, whereby the two-dimensional distribution of grain orientation is constructed. A method as claimed in claim 1 or 2, wherein the presence of abnormal grains having random grain orientation is determined when said measured amplitude is lower than a predetermined value. A method as claimed in any preceding claim, wherein each burst of ultrasonic pulses contains between ten and twenty periods. An apparatus for measuring the two-dimensional distribution of normal and abnormal crystal grain orientation in a metal sheet (11), in combination with said metal sheet, the apparatus comprising:- an ultrasonic probe comprising a transmitting element (12A) and a receiving element (12B) facing each other at opposite sides of the metal sheet (11); means (26) for scanning the ultrasonic probe in a two-dimensional scan pattern so as to cause the transmitting and receiving elements in unison to scan respective surfaces of the metal sheet (11); generating means (20) arranged to supply pulse signals to said transmitting element (12A) so as to generate therefrom burst-like ultrasonic pulses, each burst having a plurality of periods and producing multiple reflected bursts reflected from the surfaces of the sheet (11), the ultrasonic frequency f and number of periods of each burst being chosen to cause interference between the multiple reflected bursts, wherein said frequency f is determined as: f = n.v/(2.d) or as a value slightly shifted therefrom, where n = integer or half-integer, v = speed of sound in a normal or abnormal crystal grain orientation, and d = thickness of the metal sheet; receiving means (28) for receiving a signal generated at the receiving element (12B); means (30) for taking out a signal (T₁) representing the interfering multiple reflected bursts of one incident burst, from signals received by the receiving means; means (32, 34) for determining the amplitude of said signal (T₁) representing the measured speed of sound in the metal sheet, which speed depends on the orientation of grains in the metal sheet; and processing means (36) arranged to determine from said amplitude the grain orientation in the portion of the metal sheet (11) currently being scanned, and to construct therefrom the two-dimensional distribution of grain orientation. An apparatus for measuring the two-dimensional distribution of normal and abnormal crystal grain orientation in a metal sheet (11), in combination with said metal sheet, the apparatus comprising:- an ultrasonic probe (12) for transmitting and receiving ultrasonic pulses and provided at one side of the metal sheet; means (26) for scanning the ultrasonic probe in a two-dimensional scan pattern over the metal sheet (11); generating means (20) arranged to supply pulse signals to said ultrasonic probe so as to generate therefrom burst-like ultrasonic pulses, each burst having a plurality of periods and producing multiple reflected bursts reflected from the surfaces of the sheet, the ultrasonic frequency f and number of periods of each burst being chosen to cause interference between the multiple reflected bursts, wherein said frequency f is determined as: f = n.v/(2.d) or as a value slightly shifted therefrom, where n = integer or half-integer, v = speed of sound in a normal or abnormal crystal grain orientation, and d = thickness of the metal sheet; a reflecting plate (14) provided at the other side of the metal sheet (11) opposite said ultrasonic probe (12) receiving means (28) for receiving a signal (S a , B a , R₁, R₂) generated at said ultrasonic probe (12); means (30) for excluding from said signal a direct reflection signal (S a ) and extracting a signal (R₁) representing those interfering multiple reflected bursts of one incident burst which are generated upon reflection from said reflection plate; mean (32, 34) for determining an amplitude of said signal representing the measured speed of sound in the metal sheet, which speed depends on the orientation of grains in the metal sheet; and processing means (36) arranged to determine from said amplitude the grain orientation in the portion of the metal sheet (11) currently being scanned, and to construct therefrom the two-dimensional distribution of grain orientation. An apparatus as claimed in claim 5, wherein the ultrasonic probe (12) is a focus-type ultrasonic probe, adapted to focus the burst of ultrasonic waves at a point near the middle of the sheet (11) in the thickness direction. An apparatus as claimed in claim 6, wherein the reflecting plate (14) has a concave portion adapted to focus ultrasonic waves reflected thereby at a point near the middle of the sheet (11) in the thickness direction. An apparatus as claimed in any of claims 5 to 8, wherein said receiving means comprises:- a gate circuit (30) for extracting only a signal (B a , R₁, T₁) produced by the interference between the multiple reflected bursts whilst excluding other signals such as signals (S) generated by direct reflections from the sheet surface, in synchronism with a pulse (A) emitted from a timing control circuit (22) used to control said generating means (20); a peak hold circuit (32) for holding a peak value of the extracted signal for a predetermined period of time; and an analog/digital converter (34) for analog/digital conversion of an output from the peak hold circuit (32). An apparatus as claimed in any of claims 5 to 9, wherein the whole propagation course of the ultrasonic waves is immersed in water.

Inventors: ASANO KAZUYA TECHNICAL RESEARC, ICHIKAWA FUMIHIKO TECHNICAL RE, TAKADA HAJIME TECHNICAL RESEAR, ASANO, KAZUYA TECHNICAL RESEARCH DIVISION, ICHIKAWA, FUMIHIKO TECHNICAL RESEARCH DIVISION, TAKADA, HAJIME TECHNICAL RESEARCH DIVISION
Applicants: KAWASAKI STEEL CO, KAWASAKI STEEL CORPORATION
Application year: 1988
Main classification: G01N29
IPC codes: G01N29, G01N33