Compressive creep testing of refractories at elevated loads—Device, material law and evaluation techniques

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Abstract

In order to cost-effectively characterize the high temperature compressive creep behaviour of refractories a testing device was designed for application at elevated loads. Special measures have been taken necessary to enable an even stress distribution within the specimen. To identify Norton-Bailey strain hardening creep law parameters a general inverse procedure using a Levenberg–Marquardt algorithm was developed. Satisfying experimental results could be received from the creep measurement in a wide range of temperatures and loads for both shaped and unshaped materials. By fitting the strain/time curves the creep law parameters of refractories under various temperatures can be precisely identified. The measurements also reveal that at elevated loads all three creep stages can be observed.

Introduction

During service refractories are frequently exposed to intense thermomechanical loads resulting from the collaborative effects of severe thermal shock, thermal expansion of refractories and external mechanical constraints.1, 2 Under these conditions refractories may respond in elastic or inelastic manner which depends on the magnitudes and types of loads as well as on the material behaviour at high temperatures. Both material failure under Mode I–III conditions and creep may account for this inelastic behaviour and bring about an irreversible deformation of refractories.3, 4, 5, 6, 7

To characterize the creep behaviour of refractories, conventionally two types of testing procedures are employed. One is so called creep-in-compression (abbreviated as CIC) which applies the same equipment as the testing procedure for refractoriness-under-load (abbreviated as RUL). The standards of CIC in Europe, USA, Japan and China are more or less similar and mainly differ in specimen dimension, testing load and heating rate.8 According to the European standard EN 993-9,9 a fixed compressive stress of 0.2 MPa is loaded on the specimen during the heating-up and dwell periods. The change in length of the specimen is measured from the differential displacement of two corundum tubes through linear variable differential transducers (LVDTs). The deformation at certain dwell time relative to the maximum expansion occurring during the heating-up period is determined. This method is applied to compare the creep resistance capacity of refractories and to receive guidance for material selection and development in a rather phenomenological manner.10, 11, 12, 13 However, a deeper understanding of the creep mechanisms of refractories is demanded as well as extracting creep data for further thermomechanical modelling. For this purpose various loading conditions were also considered.14, 15, 16, 17, 18, 19 Formulating the secondary creep rate in dependence of temperature and stress offers one way to reveal the creep mechanisms of refractories, from which measures for material improvement may follow.

What are the tasks a satisfactory creep testing equipment should fulfil? The CIC measurement according to the European standard EN 993-9 is not suitable for determination of creep laws. One reason is that the onset of creep is not defined. Creep will start during the heating up procedure before the beginning of the dwell time because the specimen is heated up under load. Moreover the restriction of the maximum load to 0.2 MPa does not allow investigation of load levels significant for practical use of refractories in many cases. A newly designed testing equipment should especially allow the following features of the measurement: The start of the loading under isothermal conditions must be defined exactly. Moreover, displacement has to be measured on the specimen surface itself, preferably at least at two diametrical locations, in order to assess even creep of the material. Further alignment of the specimen and the testing machine is of high importance: the line of action of the imposed load has to coincide with the specimen axis. Otherwise a bending moment would be caused and result in an uneven stress distribution within the specimen. Moreover a homogenous load distribution will depend on the quality of the specimen preparation; especially parallel end faces perpendicular to the specimen axis are desired. Furthermore the application of sufficiently high stresses related to service conditions is necessary. Only sufficiently high load levels will allow observing secondary and tertiary creep in reasonable testing times.

To fulfil these missions a testing device for high temperature compressive creep application was newly developed and is presented in this paper. Efficient inverse procedure to identify the creep law parameters is also introduced with two case studies of shaped and unshaped materials.

Section snippets

Construction and main features of the testing machine

A schematic diagram of the device for high temperature compressive creep testing is shown in Fig. 1. The whole setup is based on a spindle-driven universal testing machine of sufficient stiffness. An electrical furnace is inserted and equipped with silicon carbide heating elements. The furnace is composed of two symmetrical parts, held together by means of hinges in the rear and can be closed tightly with two buckles in the front. Two platinum-rhodium thermocouples are used to measure the

Norton-Bailey creep law and inverse estimation procedure

Generally a complete creep strain/time curve under a constant load and temperature can be divided into three stages. As illustrated in Fig. 3, the first stage is called primary creep and characterized by time-dependent creep strain rate (ε˙cr) which decreases with time (ε¨cr<0). Following it the secondary creep shows a constant creep strain rate which is the minimum one of all three stages. Tertiary creep is characterized by a rising strain rate (ε¨cr>0) and leads to failure.

Many suggestions

Creep of burnt refractory bricks

Cylinder specimens as defined above have been prepared from commercially available burnt magnesia-chromite bricks (56.6 wt% MgO, 25.5 wt% Cr2O3). During the heating-up period, 100 N (equivalent to 0.1 MPa) was loaded axially on the specimen in order to fix it. Once the target temperature was reached, the extensometers were attached to the specimen before the loading procedure started. A total strain/time curve under constant load was obtained after 5 h. The measurements were carried out at 1100–1550 

Conclusions

The new high temperature compressive creep testing device can be used to characterize the creep behaviour of shaped and unshaped materials at elevated loads. A preload of 0.2 MPa as applied for CIC measurements cannot be used during the heating up procedure for unshaped materials since these materials show inferior creep resistance especially at intermediate temperatures if they have not been fired before. Creep law parameters inversely identified by Levenberg–Marquardt method imply that both

Acknowledgements

Financial support by the Austrian Federal Government and the Styrian Provincial Government (Grant no. A4.15) (Österreichische Forschungsförderungsgesellschaft and Steirische Wirtschaftsförderungs-gesellschaft) within the K2 Competence Centre on Integrated Research in Materials, Processing and Product Engineering (MCL Leoben) in the framework of the Austrian COMET Competence Centre Programme is gratefully acknowledged.

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