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V. Vasauskas
DYNAMIC HARDNESS DURING DIFFERENT PHASES OF INDENTATION

The paper reports on the underlying concept for securing the measuring basis used in the method of dynamic hardness which employes one of the standard indentation methods and various shapes of indenter. The complete dynamic indentation cycle can be divided into the three following phases: starting phase, indentation phase and rebound phase. The value for several engineering metals obtained dynamic hardness in various phases of indentation was 1.12 – 1.40 higher than the static hardness.

Hiroshi Yamamoto, Takashi Yamamoto Hiroyuki Kawashima, Mikie Shibata
DEFINITION OF LOADING FOR HARDNESS BLOCKS

In a previous report, the authors investigated changes in hardness measurements when load rise time (LRT) was changed over a broad range in Vickers harness tests with loads of between 15 kgf and 150 kgf. As a result, we reported that hardness measurements varied according to the LRT value for every test load, while they remained almost constant between 15 kgf to 150 kgf if LRT was the same, although the indentation velocity of the indenter differed by more than three times between the two loads. It is very interesting that the considerable difference in indentation velocity due to varied test loads was not reflected much in hardness measurements. We, therefore, verified the effects of loading speed on hardness measurements theoretically from the strain rates of indentation deformation under the indenter and obtained some findings as follows. (1) It is necessary to define loading conditions to ensure the reliability of hardness blocks (2) The loading condition, namely the strain rate under indentation could be determined by the equation which was newly introduced by the authors. (3) According to this equation, loading conditions for general harness tests could be defined by loading time (LRT) regardless of load values. (4) Also considering that hardness measurements can vary according to load holding time, we may say that testing conditions can be "defined by time,". (5) Consequently, from the viewpoint of industrial practice, it would be reasonable to have rough criteria, that is, for how many seconds the test should be conducted, rather than to have scrutinized discussions on indentation velocity.

Vytautas Vasauskas, Vytautas Capas
ENERGY CONCEPT IN COMPARISON OF STATIC AND DYNAMIC HARDNESS

This paper outlines the development of a simple predictive model for comparison of static and dynamic hardness. The model is essentially based on the energy - balance considerations and uses work of indentation divided by deforming volume to define hardness. The dynamic hardness was evaluated from measurements of residual contact dimensions and continued force - displacement over the velocity range 1 to 10 m s-1, based on the energy loss models and the energy conservation principle. The total and reversible work of indentation, defined as the respective area under the loading and unloading curves, has also been studied. The correlation between the static and dynamic loading results is satisfying, indicating that the effect of velocity on the energy absorbing is negligible. The obtained value for several engineering metals of dynamic hardness was 1,12?1,40 higher than the static hardness.

Christian Ullner
CRITICAL POINTS IN ISO 14577 PART 2 AND 3 CONSIDERING THE UNCERTAINTY IN MEASUREMENT

Based on the estimation of uncertainty the present requirements of the standard are discussed. Additional requirements needed for improving the reliability and the reproducibility are proposed. Especially the compliance of the machine affects strongly the parameters EIT and HMs in the macro range.

Satoshi Takagi, Hjime Ishida, Takashi Usuda, Haruo Kawachi, Kazutomi Hanaki
DIRECT VERIFICATION AND CALIBRATION OF ROCKWELL DIAMOND CONE INDENTERS

The direct verification and the calibration of Rockwell diamond cone indenters in NMLT and JBI are described. Developed instrument can verify the roundness of the spherical part of the indenters, measure the radius of indenter tip and the cone angle by the optical methods. The regression analysis of the geometry of indenters and hardness value can determine the bias of each indenter in each hardness level. This bias can be used to correct the hardness value. To investigate the availability of the correction of hardness value, the experiments were carried out to analyze the relation between the indenters and other testing conditions. The results show that the effect of indenters are independent with other factors and the correction of hardness values are available. Hardness values were agreed within 0.04 HRC (standard deviation) after the correction is was applied.

Anton Stibler, Konrad Herrmann, Zoran Susteric
LONG-TERM STABILITY OF RUBBER HARDNESS REFERENCE BLOCKS

Methods for hardness measurement on elastomers are characterized by a set-up where indenters with various defined geometries are pressed under defined test forces into the surface of testing material. The hardness value represents the resistance of the material to the rigid indenter and is calculated from the indentation depth of the indenter in the to be tested material. The test methods IRHD and Shore are the most common methods used in the field of rubber hardness measurements. Appropriate hardness measuring instruments are spread world wide. A periodic verification has to be carried out to assure the accuracy of these measuring instruments. Direct and indirect verification methods are recommended to be used. For the indirect method rubber hardness reference blocks are used. This indirect verification method is especially appropriate for the daily check of hand held rubber hardness testers. On the other side the direct verification of test force, depth measuring system and indenter geometry is suited for the periodic calibration of rubber hardness testers. For the rubber hardness reference blocks their accurate hardness reference value and the long-term stability are the most important characteristics. In this paper the long-term behaviour of hardness of rubber blocks which at present are available on the market and are made by different producers is presented. For the measurements the Shore and IRHD hardness standard devices in the PTB have been used. In order to determine the relationship between hardness and time under the specified conditions a regression analysis of the obtained measurement results was carried out. The results of this analysis can be used for the improvement of quality assurance systems in the field of rubber hardness measurements.

Anton Stibler, Samuel Low, Robert Ellis
COMPARATIVE MEASUREMENTS OF SLOVENIAN AND USA ROCKWELL C HARDNESS SCALES

A national scale is set up for each hardness scale representing the reference hardness values in each country. From metrological and international trade aspects agreement between the national scales is very important. Good agreement makes possible good industrial cooperation. Therefore comparison between national scales is necessary. Comparison between national hardness scales and hardness scales set up by the producers of the reference blocks is necessary as well. The Rockwell measurement method is the most widely used hardness measurement method throughout the world. The measurement is practical, relatively easy to carry out and the measurement result is quickly and simply indicated on the indicator. Among the different Rockwell scales, the C scale is very useful. It satisfies demands for accurate hardness measurement especially during hardening process of steel, which is often applied in industry. In this paper comparative measurements between the Rockwell C national scales of Slovenia as measured by Zavod za gradbeni?tvo Slovenije (ZAG) and USA as measured by the National Institute of Standards and Technology (NIST) and the scale set up by a producer of reference blocks, David L. Ellis Co., Inc., are presented.

David Shuman; Margareth S. Andrade
USING NEWATOMIC FORCEMICROSCOPE SOFTWARE TO MEASURE THE HARDNESS OF GRAINS AND MICROCONSTITUENTS

It is desirable to measure the hardness of individual grains and microconstituents to have control over the mechanical properties of materials. An ultra-micro or nanoindenter is required to make indents small enough to fit inside a single grain or phases that is smaller than 10 mm diameter. Because the indents are too small for an optical microscope an atomic force microscope was used to view the location and measure the contact area. Measuring the contact area of indents from an atomic force microscope image is unreliable because it is difficult to manually locate the indent edge. To solve this problem computerized image analysis software called NanoMc was used to measure the residual indent contact area. This software digitally reconstructed the residual indent back into the fully loaded indentation shape and then measures the contact area and depth. This method avoids the complicated tip rounding and load-frame compliance problems. As an example this method was used to measure the hardness of pearlite and ferrite microconstituents in SAE 1020 steel.

Nicholas X. Randall
DIRECT MEASUREMENT OF RESIDUAL CONTACT AREA AND VOLUME DURING THE NANOINDENTATION OF COATED MATERIALS AS AN ALTERNATIVE METHOD OF CALCULATING HARDNESS

The mechanical properties of thin films can be measured by a variety of different techniques, with nanoindentation being one of the most recent developments in this growing field. By using a depthsensing indentation method it is possible to obtain quantitative values for the hardness and modulus, and thus gain better insight into the response of a material to controlled deformation at such small scales. However, previous work has shown that the effects of pile-up, particularly in soft films deposited on hard substrates, can produce significant overestimation of the hardness and modulus due to an underestimation of the true contact area by common nanoindentation analysis procedures. By measuring the topography of the residual indent using Scanning Force Microscopy (SFM) and combining this information with the indentation data, it is possible to gain a fuller understanding of the indentation method and its effects on the material being tested. In addition, the true contact area can be directly measured from the SFM images and subsequently used to recalculate the hardness of the material more accurately. Moreover, the SFM allows the plastic volume of indentation to be measured, from which hardness can also be calculated in terms of plastic work. Experimental results are presented for two types of thin film deposited on hard substrates where SFM analysis of indentations at varying depths gives significant additional information concerning the true response of the system to instrumented indentation at a nanometric scale. Pile-up effects can be precisely monitored as a function of depth and correlated to hardness variations encountered across the coating/substrate interface.

George D. Quinn, Robert Gettings, and Lewis K. Ives
A STANDARD REFERENCE MATERIAL FOR VICKERS HARDNESS OF CERAMICS AND HARDMETALS

Standard Reference Material (SRM) 2831 was developed to improve Vickers hardness testing of Ceramics and Hardmetals. It may be used with conventional hardness testing machines that make indentations that are measured with an optical microscope. The SRM is a hot-isostatically pressed tungsten carbide with 12 % cobalt disk which has five indentations made at a load of 9.8 N (1 kgf). Each SRM is individually certified for the size of each of the 5 indentations, the average diagonal length ( 35.0 m), and the average hardness HV1. The HV1 is nominally 15 GPa which is in middle of the hardness range for most ceramics and cutting tool carbides.

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