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Article

Compatibility Testing of New Insulating Fluids and Materials in Distribution Transformer

1
Department of Technologies and Measurement, Faculty of Electrical Engineering, University of West Bohemia, 301 00 Pilsen, Czech Republic
2
Independent Researcher, 331 52 Horni Bela, Czech Republic
*
Author to whom correspondence should be addressed.
Energies 2025, 18(7), 1831; https://doi.org/10.3390/en18071831
Submission received: 4 March 2025 / Revised: 21 March 2025 / Accepted: 27 March 2025 / Published: 4 April 2025
(This article belongs to the Section F: Electrical Engineering)

Abstract

:
The introduction of a new insulating oil or, for instance, a new type of insulation or sealing into a transformer necessitates tests for material compatibility. Compatibility tests of liquids with the structural internal materials of transformers are conducted to prevent undesired interactions between insulating fluids and the formation of products that could lead to the generation of undesirable ions, sediments, or chemical compounds that result in a reduction in the dielectric property performance of the fluid. This includes chemical reactions (hydrolysis, hydrogenation, oxidation, formation of sulfates or sulfides, etc.) and degradation, the formation of conductive suspensions, the generation of undesirable condensation, and alterations in other fluid properties, such as interfacial tension between oil and water, viscosity, flashpoint, etc. Changes must also not occur in the strength and hardness of gasket material, which could result in undesirable fluid leakage. This paper describes the novel methodology and results of several proposed tests, including the impact on oil viscosity, material hardness, FT-IR analysis of oils, partial discharges in different oils, dielectric properties, and more, conducted during compatibility and aging tests at 120 °C and 140 °C performed on materials used in particular distribution transformers being prepared for natural ester use. The results show notable differences in the behavior of insulating fluids and aged submerged materials. While mineral oils exhibit lower dissipation factors compared to natural esters, the latter demonstrate slower and less severe hardening effects on gaskets during high-temperature aging (e.g., Shore 35.25 in mineral oil vs. 21–22.5 in natural esters). The tensile strength of the tested cable ties decreased significantly (from 260 to approx. 60 N) in mineral oil but increased in natural ester (320 N/120 °C exposition). This study also highlights a novel insight into partial discharge mechanisms, where differences in viscosity, conductivity phenomena, and dielectric constants result in presented differences in inception voltages and prebreakdown activity.

1. Introduction

In the past, various fluids have been tested as substitutes for electrical insulating oils in transformers based on naphthenic or paraffinic mineral oils. These included fluids based on fluorinated or chlorinated biphenyls (1960s), silicone fluids (1970s), and synthetic esters (1980s). While some of these liquids were technically satisfactory, they posed a threat to ecosystems. Silicone liquids were expensive and immiscible, and the first synthetic esters were too expensive and produced toxic fumes when electrically arced [1].
In liquid-filled transformers, the oil serves two crucial features by providing electrical insulation and dissipating heat generated by Joule losses, primarily from the windings, but also from the magnetic core and insulating system itself. When selecting oil for high-voltage power or distribution transformers, key dielectric properties such as permittivity, dissipation factor, and electrical breakdown voltage strength are significant parameters [2,3,4,5,6] for, e.g., infrared spectroscopy [7].
Insulation quality tests are necessary both after transformer manufacturing and during their operational lifespan. In most instances, insulation faults are linked to partial discharges, which arise from various causes [8,9,10,11,12].
Currently, there is a strong emphasis on replacing mineral liquids with biodegradable liquids produced from renewable sources [4,5,6,13,14,15,16,17,18,19,20]. This is a strategic decision in countries without their own oil reserves to reduce dependence on imported petroleum products. Natural oils, such as rapeseed, soy, and sunflower, are increasingly preferred as insulation fluids in modern transformers due to their eco-friendly attributes and cost-effectiveness [4,17,18,19,21]. To ensure the compatibility of novel materials used in transformers, it is important to conduct a thorough investigation [2,13,22,23,24]. Previous studies have examined the interaction between insulating papers and various materials, including gaskets, varnishes, and core steel, with oils such as soy or corn oil [2,13,19,22].
The study in [22] conducted compatibility testing and addressed the compatibility of transformer mineral oil and gasket materials, including O-rings. The study found that approximately half of the gaskets did not meet the requirements, the silicone gaskets being the worst performers, as none of them passed. On the other hand, fluorocarbon gaskets were successful in all three cases. ASTM D 3455-11 Standard Test Methods for Compatibility of Construction Material with Electrical Insulating Oil of Petroleum Origin [25] was used for these tests.
The study presented in this paper specifically focuses on exploring the compatibility of PA cable ties, rubber-based gaskets, and essential components of transformer bushings—materials used in 400 V/22 kV (35 kV) distribution transformers. The overall subject of the test is a small oil-filled distribution transformer that is EU-manufactured typically in the performance series of 50, 100, 160, 250, 400, 630, 800, 1000, 1250, 1600, 2000, and 2500 kVA for voltage levels 22 and 35 kVA, e.g., [26]. All materials used in this transformer that could potentially interact with the natural ester have to been carefully tested using a pre-designed compatibility test procedure.

2. Materials and Methods

The experiment was performed with the goal of a natural ester oil behavior description in working-like conditions—a description of the interaction with other materials of the transformer using increased intensity by elevating the temperature and/or high electric field.
The tested materials were immersed in insulating oils, utilizing rapeseed-oil-based oil Envitrafol, rapeseed oil, and, for comparison, mineral oil Nynas Lyra X or Midel 7131 eventually. Subsequently, these materials underwent thermal aging in an oven for 2000 h at 120 °C and 1000 h at 140 °C.
A comprehensive analysis was conducted on all polymer samples and oils both before and after the aging process. The examination encompassed changes in weight and dimensions and Shore hardness, as well as electrical properties such as permittivity, resistivity, and dissipation factor if possible. Additionally, the viscosity of oils was a key aspect discussed in the evaluation. The oils after aging were subjected to the measurement of the dissipation factor, resistivity, Fourier transform infrared spectroscopy (FT-IR), and inhomogeneous field partial discharge testing.
A.
Compatibility test
Since numerous papers have been published describing the interaction of natural ester, cellulose papers, and copper [2,13,22], the testing of material compatibility was focused on auxiliary materials with natural ester. The tested materials were a rubber cork seal used for 400 V bushings, polymeric thermoset PA 6.6 (C12H22N2O2)n (melting point 268 °C) (marked as “bushing”) used as the inner part (immersed in oil) of the 20 and 35 kV bushing, auxiliary construction material (marked as “cable ties”) based on PA 6 (C6H11NO)n (melting point 220 °C), and a synthetic rubber seal (gasket).
The above-mentioned auxiliary materials have been used in small distribution transformers with mineral oils for decades. The thermal aging of the samples took place on two sets of samples at two temperatures. The first set of the samples (rubber cork seal and auxiliary construction material) was aged at 140 °C for 1000 h in both rapeseed and mineral oil. The samples were immersed in dark airtight glass containers. The second set was aged at 120 °C for 2000 h. At both temperatures, a construction material was immersed in rapeseed and mineral oil. The sets of oils-only samples were subjected to the same temperatures and times for comparison.
The main tests carried out on the samples subjected to compatibility tests and the testing of oil samples are described below.
B.
Mechanical test
The two methods were used to test mechanical properties of rubber seals: the maximum tensile stress recorded in extending the test piece to breaking point and the standard hardness test according to Shore. In the field of conventional mechanical testing, tensile tests based on the standard ISO 527 [27] were performed using the LabTest 3.030 testing machine LaborTech. Hardness was obtained using the procedures described in methods N, H, L, and M on test pieces of standard thickness and not less than the minimum lateral dimensions specified.
The Shore hardness test measures the indentation depth using a spring-loaded indenter made of hardened steel. The hardness value is determined on a scale ranging from 0 Shore (2.5 mm indentation depth) to 100 Shore (0 mm indentation depth). Different Shore scales (such as Shore A and D) are established based on variations in indenter forms and spring characteristics. Shore A is usually suitable for soft rubber, elastomers, and natural rubber, and Shore D is suitable for harder elastomers, plastics, and rigid thermoplastics.
C.
Electrical test
The dissipation factor tan δ serves as a measure of dielectric losses caused by polarization and conductivity phenomena within the tested liquid. Therefore, tan δ can indicate various issues, including the following:
-
Liquid contamination with, e.g., moisture, particles, or soluble polar contaminants.
-
Refining quality, where poor refining quality could also contribute to elevated tan δ values.
The dissipation factor was measured in accordance with IEC 60247 [28] at a temperature of 90 °C and 500 V/50 Hz, with a Tettex 2830/2831 dielectric analyzer along with a 2903 electrode system (both from Haefely).
An essential factor for ensuring the long-term performance of the EIS is the measurement of PD (partial discharge) activity [9,11,12]. In our study, we conducted partial discharge measurements using the electrode system depicted in Figure 1. Specifically, the high voltage (HV) was connected to the semisphere while the needle was grounded. For security reasons, we introduced a dielectric barrier (approximately 0.3 mm thick, with a relative permittivity of approximately 2.5) into the electrode system. The evaluation procedure for PD behavior is illustrated in Figure 2. The measurement circuit was calibrated prior to conducting the measurement (50 pC). Recorded parameters were collected at the end of the 3 min interval and continued until reaching the breakdown level. In the future, the transformer insulation will increasingly suffer from the converter load [3,29].
From the maximal intensity of the electrical field (Emax = 1.09·107 V/m), a Schwaiger factor (1) was calculated η = 0.11.
η = V d · 1 E m ,
where V is applied voltage (V) and d is the distance of electrodes (m). Maximal intensity was calculated based on the microcopy of the tungsten needle tip.
The Schwaiger factor is commonly used in order to assess both weakly and strongly inhomogeneous non-uniform electric fields and various electrode configurations [30,31]. The factor is defined as the ratio of the maximum electrical field to the mean value of the electrical field.
D.
Viscosity
Electrical insulating fluid viscosity influences the heat transfer and therefore affects the increase in temperature in the transformer. Normally, the lower the viscosity, the easier the oil circulates from winding to the cooler, thus providing better heat transfer. Viscosity at lower temperatures is a critical factor for the cold start of, e.g., transformers. Dynamic viscosity refers to the frictional force that arises between two layers of flowing fluid when they come into contact with each other over an area of 1 m2, with a velocity difference of 1 m/s. Its measurement is possible using a vibrational viscometer (SV 10, A&D Instruments Limited), as shown in Figure 3. This type of viscometer measures viscosity by detecting the electrical current required for the resonance of two sensor plates at a constant frequency of 30 Hz and an amplitude of less than 1 mm. The usual levels of viscosity for mineral fluids are approx. 10 mm2s−1 at 40 °C and 40 mm2s−1 for esters, measured at 40 °C. When the fluid density is known, the conversion relation between dynamic and kinematic viscosity might be used along with ISO 3104:2023 [32].
The water content of the oil samples was measured by a Coulometer WTD (Diram) based on a Karl Fischer titration (Figure 4). The same device was used for an acid number measurement based on the volumetric determination of alkali blue B6 as a spectrophotometric indicator. The aging of oil and the oil–paper system increases the amount of acidic substances present in the oil as well as water (acid hydrolysis of cellulose). These parameters are suitable for assessing the condition and age of the oil. The definition of acidity number establishes it as the amount of potassium hydroxide (KOH) required to neutralize organic and inorganic acid-reacting components in 1 g of oil in a non-aqueous alcoholic environment. The determination of acidity number utilizes the method of spectrophotometric identification.
In coulometric titration, the titrant (hydroxide ions) is generated directly at the platinum cathode by the decomposition of water. Neutralization occurs in a closed cathodic compartment of the electrolytic cell without the presence of air, thus eliminating interference from atmospheric carbon dioxide. Spectrophotometric indication using an acid–base indicator is employed to determine equivalence. The titration solution consists of a mixture of alcohol and toluene (1:2) with a suitable indicator and an electrolyte salt. The result of the analysis is the equivalent amount of KOH in micrograms, expressed directly as the acidity value in mg KOH/g. Further details about the measurement can be found in the standard IEC 62021-1 [33].
E.
FT-IR
Fourier transform infrared spectroscopy (FT-IR) measurements were conducted using the Nicolet 380 spectrum analyzer. These measurements took place in the mid-infrared region and utilized both the attenuated total reflectance (ATR) technique and the transmission technique. The ATR spectrum of the sample is influenced by the wavelength of the infrared radiation, the ratio of the refractive indices of the measured sample and the ATR crystal, the angle of incidence of the radiation on the phase interface, and the efficiency of the contact between the measured sample and the ATR crystal. The resulting penetration depth of the radiation into the sample is defined by relationship (2).
d p = λ 2 π n k s i n 2 θ n v n k 2
where dp is the penetration depth of the radiation into the sample, λ is the wavelength of the radiation, θ is the angle of incidence of the radiation on the phase interface, and nv and nk are the refractive indices of the sample and the crystal, respectively. The result of the experimental effort is the infrared spectrum of the substance, representing the dependence of transmittance T, absorbance A, or reflectance R (optical properties of the sample) on the wavenumber (or wavelength or frequency) [21,34].
T = ϕ ϕ 0   ,   A = l o g ϕ ϕ 0 ,   R = ϕ r ϕ 0
where Φ0, Φ, and Φ0r represent the radiation flux before and after the cuvette and the radiation flux reflected by the sample. In infrared spectral studies [7,21,34], it is possible to detect chemical reaction byproducts dissolved in oil. This is a non-destructive analytical method that investigates the material’s response to infrared radiation with wavelengths between 780 nm and 300 µm. Infrared radiation is commonly divided into near (0.78–3 μm), mid (3–30 μm), and far (30–300 μm) infrared regions. Due to the logarithmic relationship between energy and wavelength, the wavenumber unit was introduced, expressed as the reciprocal of the wavelength. Its unit is expressed in cm−1. Photons of infrared radiation transfer energy to molecules, causing changes in their vibrational or rotational states. During molecular vibrational motion, energy is converted between potential and kinetic forms. Vibrational motions are categorized as valence and deformation vibrations. Valence vibrations involve periodic changes in bond length within the molecule (symmetric and asymmetric changes) while deformation vibrations refer to periodic changes in bond angles between atoms in the molecule. IR transmission measurements were performed by FT-IR Nicolet 380 using PIKE Demountable Liquid Cell Kits (PIKE Technologies, Cottonwood, Madison, USAú with BaF2 windows (optical path 1 mm). The spectra were acquired at 4 cm−1 resolution when a total of 32 scans were co-added for each measured spectrum.

3. Results

The dissipation factor (Figure 5) and resistivity (Figure 6) of the fluids after aging were measured, since any diluted substance will probably dissociate in the fluid and cause an increase in the dissipation factor, reducing the resistivity.
The results show a significant increase in the dissipation factor after aging at 120 °C, as well as at 140 °C. In this mass ratio and at these high temperatures, the degradation of fluids’ dielectric properties is evident. The different impacts of tested material on different oils were not observed.
The result of measured resistivity shows the impact of the tested materials on fluid resistivity. The impact is slightly negative. Again, based on this result, we do not consider new types of adverse effects of the tested material in ester fluid.
As mentioned, the proper feature for a gasket compatibility test is measurement of the hardness. If the seal hardens due to the interaction with oil, then it stops fulfilling its role and the container will not be sealed; otherwise, when it is softened by the oil, the container will not seal again. This will lead to oil leaks, and the windings and oil voltage of the transformer may become wet due to air moisture.
The synthetic rubber seal was submerged in mineral (Nynas) and natural esters (Envitrafol, rapeseed oil) in sealed containers for 2000 h at 120 °C and 1000 h at 140 °C. The results of the measured harness are given in the following Figure 7.
As seen, the hardness of the tested transformer seal after the test (120 °C) changed most when thermally aged without the fluid (20.5 to 44), and then in mineral oil (20.5 to 35). The hardness of the sample almost did not change in Envitrafol oil (20.5 vs. 21). In rapeseed oil, an increase to 22.5 was observable. Similar results can be seen when exposed to 140 °C.
Changes in the tensile strength of PA 6 cable ties were measured using a tensile strength measuring device from LabTest (LaborTech, Opava, Czech Republic). In the initial position between the jaws, a distance of 8 cm was set, and the measurement rate was 60 mm/min. The results can be seen in the following Table 1. At first glance, it is evident that the cable ties aged in mineral oil lost their tensile strength (the tensile strength before the test was 260 N). These cable ties were almost impossible to secure between the jaws, and they would be classified as brittle (they broke in the hand with minimal effort). The maximum force (Fmax) increased for cable ties aged in rapeseed oil 120 °C. From the results, it is, however, evident that, at the same time, the PA in rapeseed became more brittle. These cable ties reached maximum tensile strength but lost their elasticity.
For compatibility testing, it is important to check whether the fluid can penetrate and, for example, soften the tested seal. The weight of the samples was therefore measured efore and after the test, with a result of no increase in weight; Figure 8.
The viscosities of the oils aged by temperature (120 and 140 °C) and oils with a submerged rubber seal are presented in the following picture (Figure 9). Again, the results prove that no significant changes occurred in the oil due to interaction with the gasket.
The results of the measured water content of oil samples after testing are not so easy to explain. It was proved by [14] that both an acid hydrolysis and hydrogenation reaction occur in ester oil when exposed to high temperatures since mineral oil is determined by the acid hydrolysis of paper, which is not present in this experiment. The results of the effect of the seal on the formation of water in the oil can be marked as inconclusive based on the findings shown in Figure 10. We expected a hydrogenation reaction of natural oil while subjected to 120 °C [13].
In the following figures, the measured FT-IR spectra of tested fluids are presented. First, the overall spectra of rapeseed oil, Figure 11, and mineral oil, Figure 12, are presented. In Table 2, wavenumbers are assigned to main functional groups of tested oils.
Figure 11 and Figure 12 show the results obtained by the ATR technique. This is a basic measurement that, however, does not have sufficient sensitivity to identify weakly contained components connected with oxidation-related changes. For this reason, transmission measurements were performed. This technique is described, for example, in “Comparison of the mineral oil lifetime estimates obtained by differential scanning calorimetry, infrared spectroscopy, and dielectric dissipation factor measurements” [7], where a comparison with fresh oil samples is also provided.
In the spectral analysis depicted in Figure 11 and Figure 12, discernible differences emerge. Notably, variations in spectral intensity occur within the hydroxyl region at 3475 cm−1 (associated with H2O, ROH, and ROOH), indicating the oxidation of oils. Specifically, for rapeseed oil, heightened spectral intensity correlates with increased oil oxidation.
Furthermore [6], the aging process of mineral oil manifests as a reduction in the spectral band related to low-temperature antioxidants. This reduction is attributed to the stretch vibration of a non-hydrogen-bonded O-H group, spanning the spectral range from 3600 to 3700 cm−1 (as illustrated in Figure 13 and detailed in Figure 14). As mineral oil ages, the gradual depletion of total antioxidants leads to a corresponding decrease in the intensity of the spectral band centered around 3650 cm−1.
Figure 15 gives a detailed depiction of the vibrational region of the detected oil antioxidant.
Other alterations in spectral intensity arising from the aging process become evident within the wavenumber range of 1650–1800 cm−1 (associated with the C=O stretching vibration), see Figure 16. These variations can be attributed to the oxidative reactions occurring in the oil. Specifically, the presence of this spectral band indicates the accumulation of carbonyl (C=O) or hydroperoxide (-OOH) groups. Notably, the strong spectral bands within this range suggest the presence of oxidation products such as ketones, aldehydes, and carboxylic acids. These compounds exhibit a significant dipole moment, where the accumulation of such polar compounds leads to a higher dielectric loss and a reduction in the insulation performance of the oil, as they increase electrical conductivity [6,7].
In Figure 17 and Figure 18, the polarity of a bond influences the intensity of an absorption band. Bonds with greater polarity produce more intense absorption bands. Additionally, the intensity is affected by the number of bonds contributing to the absorption. Based on the Beer–Lambert law, absorption bands involving more bonds exhibit higher intensity.
Due to the need to analyze the less abundant components, the optical path had to be increased during the measurement. Thus, the intensity of the more abundant components had to be significantly increased. In these cases, they enter a state of so-called total absorption, which is manifested by an oscillation curve.
From the measurement results of the PD activity, it is evident that the breakdown is likely caused by charges located in the positive polarity. An intriguing observation arises from the situation at the PDIV (partial discharge inception voltage) level. Notably, PDs initiate in different polarities for Midel 7131 and Nynas when compared to natural ester (organic-based ester). This discrepancy could potentially be attributed to variations in the internal structure of the investigated oils [9].
The PD analysis reveals intriguing findings. When examining the natural ester fluid, we observe that there are only a few voltage steps leading to the BDV (breakdown voltage), as depicted in Figure 19. In contrast, for the other two fluids, the PD charge increment is gradual as the voltage approaches the BDV. The breakdown mechanism in the case of FR3, an ester fluid, is attributed to the injection of electrical charge carriers. However, for Nynas Taurus (a mineral oil) and Midel 7131 (synthetic ester fluid), the breakdown results from the generation of air bubbles, as indicated by the phase-resolved PD patterns (PRPD) in Figure 20 and Figure 21 [11,12].

4. Discussion

Analyzing the dielectric properties, we observe that thermal stress leads to the formation of ionic impurities, which adversely impact the oil’s dissipation factor. As anticipated, mineral oil consistently exhibits a lower dissipation factor compared to natural oils due to its polar nature. Throughout testing and aging, this difference remains consistent. Notably, the gaskets’ effect on mineral oil versus natural-origin oils is indistinguishable.
The tensile strength measurement of PA cable ties reveals that, while tensile strength increases in natural ester during aging, it decreases fourfold in mineral oil during the same aging process.
As seen from the test results of the mechanical properties of the tested gasket, and contrary to expectations, the harsh effect on the aging of the transformer seal has thermal aging (120 °C) itself (Shore 44 after test vs. 20.5 new) and aging in mineral oil (Shore 35.25 after test). When submerged in rapeseed oil or Envitrafol, the change in hardness for the same condition is lower (Shore 21 and 22.5 vs. 20.5 new). Similar results are seen for 140 °C aging. The results shown in Figure 7 indicate that natural esters (contrary to expectations) cause less hardening than mineral oil in both cases of thermal aging. Also, expected softening did not occur.
The behavior of natural ester and mineral oil differs significantly from the perspective of water content observations. While natural ester undergoes both hydrolysis and hydrogenation, mineral oil experiences drying due to temperature. This effect was also noted in [13] and requires further investigation.
Weight measurement of the gasket samples shows no significant changes when comparing the weight before and after aging in oils. The same results were obtained when measuring the viscosity of oils. This corresponds with dissipation and resistivity measurements.
From the FT-IR measurement, it is evident that the oil samples have been significantly aged by temperature. The oxidation processes and products of thermal aging are clearly discernible from the results. In particular, Figure 16 illustrates the observable impact of the tested material on the thermal aging of the entire oil system, including the material under test. By closely examining the vibration of antioxidants, we can appreciate the precision of the FT-IR analyses, with no expected changes in this peak.
From the PD measurement, it is evident that different chemical constitutions of the oils lead to different mechanisms of oil conductivity in the inhomogeneous electric field, and thus to the different PD activity inceptions and different voltage dependances until electric breakdown. Different conductivity phenomena, different viscosities, and a higher dielectric constant of esters lead to completely different mechanisms of the first streamer in different fluids. This difference is increased with the voltage, as can be seen when comparing [29,35]. Regarding the low voltages, the viscosity probably plays a significant role.
The overall conclusion is that auxiliary materials react with the insulating fluid and that this interaction is detectable. As anticipated, due to the distinct chemical composition of mineral and ester fluids, degradation processes behave differently. Further focus is needed in this area for future research. Lastly, some of the expected adverse processes in natural esters occur at a slower rate than anticipated. More diagnostic data from real operations need to be gathered to predict technical life correctly, e.g., [4,12].

Author Contributions

Validation, M.T. and J.L.; Formal analysis, J.H. and Z.M.; Investigation, P.T., J.K., P.P. and Z.F.; Data curation, O.M. and P.S.; Writing—original draft, P.T. All authors have read and agreed to the published version of the manuscript.

Funding

This research has been supported by the National Centre for Energy II (NCE II) TN02000025 and he Student Grant Agency of the University of West Bohemia in Pilsen, grant No. SGS-2024-008 “Materials and Technologies for Electrical Engineering” and the OP JAK Czech Incubator of Technologies for Energy Networks.

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author(s).

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Fofana, I.; Rao, U.M. Engineering Dielectric Liquid Application. Energies 2018, 11, 2756. [Google Scholar] [CrossRef]
  2. Huang, Q.; Song, H.; Li, Z.; Wang, W.; Huang, H. Compatibility Test of Coatings with Natural Ester at Elevated Temperature. In Proceedings of the 2022 IEEE Conference on Electrical Insulation and Dielectric Phenomena (CEIDP), Denver, CO, USA, 30 October–2 November 2022; pp. 297–300. [Google Scholar]
  3. Mentlík, V.; Trnka, P.; Svoboda, M.; Hornak, J.; Totzauer, P.; Harvánek, L. Aging phenomena of paper-oil insulating system under different voltage stress. In Proceedings of the 2015 IEEE 11th International Conference on the Properties and Applications of Dielectric Materials (ICPADM), Sydney, Australia, 19–22 July 2015; pp. 548–551. [Google Scholar]
  4. Shen, Z.; Wang, F.; Wang, Z.; Li, J. A critical review of plant based, insulating fluids for transformer: 30-year development. Renew. Sustain. Energy Rev. 2021, 141, 110783. [Google Scholar] [CrossRef]
  5. Beroual, A.; Alkuhayli, A.; Mahmoud, M.M.; Khaled, U. A Review on Electrical Breakdown of Natural Ester-Based Nanofluids Under Different Voltage Waveforms. IEEE Access 2024, 12, 75610–75624. [Google Scholar] [CrossRef]
  6. Raymon, A. Transesterification Approaches to Natural Esters for Transformer Insulating Fluids: A Review. IEEE Trans. Dielectr. Electr. Insul. 2024, 31, 607–614. [Google Scholar] [CrossRef]
  7. Polansky, R.; Prosr, P.; Vik, R.; Moravcova, D.; Pihera, J. Comparison of the mineral oil lifetime estimates obtained by differential scanning calorimetry, infrared spectroscopy, and dielectric dissipation factor measurements. Thermochim. Acta 2017, 647, 86–93. [Google Scholar] [CrossRef]
  8. IEC 62975; Natural Esters—Guidelines for Maintenance and Use in Electrical Equipment. International Electrotechnical Commission: Geneva, Switzerland, 2021; pp. 1–73.
  9. Trnka, P.; Hornak, J.; Svoboda, M.; Pihera, J. Partial discharges under DC voltage in paper-oil insulating system. In Proceedings of the 2015 IEEE 11th International Conference on the Properties and Applications of Dielectric Materials (ICPADM), Sydney, Australia, 19–22 July 2015; pp. 436–439. [Google Scholar]
  10. IEEE Std C57.91-2011; IEEE Guide for Loading Mineral Oil-Immersed Transformers and Step-Voltage Regulators. IEEE Standards Association: Piscataway, NJ, USA, 2012; pp. 1–123.
  11. Korobeynikov, S.; Ovsyannikov, A.; Ridel, A.; Karpov, D.; Lyutikova, M.; Kuznetsova, Y.; Yassinskiy, V. Study of partial discharges in liquids. J. Electrost. 2020, 103, 103412. [Google Scholar] [CrossRef]
  12. Pattanadech, N.; Haller, R.; Kornhuber, S.; Muhr, M. Partial Discharges (PD); Wiley: Hoboken, NJ, USA, 2023; ISBN 9781119568452. [Google Scholar] [CrossRef]
  13. Li, R.; Ban, Y.; Cheng, L.; Liu, W. Investigation of the Compatibility between Mechanical Fixing Tapes and Impregnation Fluid of Power Capacitors. In Proceedings of the 2023 IEEE 4th International Conference on Electrical Materials and Power Equipment (ICEMPE), Shanghai, China, 7–10 May 2023; pp. 1–4. [Google Scholar]
  14. Trnka, P.; Hornak, J.; Prosr, P.; Michal, O.; Wang, F. Various Aging Processes in a Paper-Natural Ester Insulation System in the Presence of Copper and Moisture. IEEE Access 2020, 8, 61989–61998. [Google Scholar]
  15. Fox, N.J.; Stachowiak, G.W. Vegetable oil-based lubricants—A review of oxidation. Tribol. Int. 2007, 40, 1035–1046. [Google Scholar] [CrossRef]
  16. Kurzweil, P.; Schell, C.; Haller, R.; Trnka, P.; Hornak, J. Environmental Impact and Aging Properties of Natural and Synthetic Transformer Oils under Electrical Stress Conditions. Adv. Sustain. Syst. 2021, 5, 2100079. [Google Scholar]
  17. Mentlik, V.; Trnka, P.; Hornak, J.; Totzauer, P. Development of a biodegradable electro-insulating liquid and its subsequent modification by nanoparticles. Energies 2018, 11, 508. [Google Scholar] [CrossRef]
  18. IEC 60296; Fluids for Electrotechnical Applications—Unused Mineral Insulating Oils for Transformers and Switchgear. International Electrotechnical Commission: Geneva, Switzerland, 2003.
  19. Oommen, T.V. Vegetable oils for liquid-filled transformers. IEEE Electr. Insul. Mag. 2002, 18, 6–11. [Google Scholar] [CrossRef]
  20. Altay, R.; Santisteban, A.; Olmo, C.; Renedo, C.J.; Fernandez, A.O.; Ortiz, F.; Delgado, F. Use of Alternative Fluids in Very High-Power Transformers: Experimental and Numerical Thermal Studies. IEEE Access 2020, 8, 207054–207062. [Google Scholar] [CrossRef]
  21. Lu, Y.J. Characterization of Rapeseed Oil Using FTIR-ATR Spectroscopy. J. Food Sci. Eng. 2014, 4, 244–249. [Google Scholar]
  22. Lewand, L. Material compatibility of gasket materials in insulating liquids. In Proceedings of the 80th International Conference of Doble Clients; 2013. [Google Scholar]
  23. ASTM D 3455-11; Standard Test Methods for Compatibility of Construction Material with Electrical Insulating Oil of Petroleum Origin. ASTM International: West Conshohocken, PA, USA, 2011.
  24. IEC 60270; High-Voltage Test Techniques—Partial Discharge Measurements. International Electrotechnical Commission: Geneva, Switzerland, 2000.
  25. ASTM D 3455-11; Standard Test Methods for Compatibility of Construction Material with Electrical Insulating Oil of Petroleum Origin. American Society for Testing and Materials: West Conshohocken, PA, USA, 2019; p. 34.
  26. Technical Materials. 2023. Available online: http://www.trafocz.cz (accessed on 23 May 2023).
  27. ISO 527-1; Plastics—Determination of Tensile Properties—Part 1: General Principles. International Organization for Standardization: Geneva, Switzerland, 2019.
  28. IEC 60247:2004; Insulating Liquids—Measurement of Relative Permittivity, Dielectric Dissipation Factor (tan d) and d.c. Resistivity. IEC (International Electrotechnical Commission): Geneva, Switzerland, 2004.
  29. Haller, R.; Hornak, J.; Trnka, P.; Hlavacek, J.; Gamil, A. Dielectric behaviour of natural and synthetic esters at inhomogeneous field condition. In Proceedings of the 21st International Symposium on High Voltage Engineering, Budapest, Hungary, 26–30 August 2019; Volume 599, pp. 308–319. [Google Scholar]
  30. Arora, R.; Prem, S. Experimental Estimation of Schwaiger Factor Limit (ηLIM) in Atmospheric Air. In Gaseous Dielectrics VIII; Springer: Boston, MA, USA, 1998; pp. 325–330. [Google Scholar] [CrossRef]
  31. Mehta, D.; Kundu, P.; Chowdhury, A. Discussion on methodology to study the dielectric performance of insulating liquids in view of Schwaiger factor. Model. Meas. Control A 2020, 92, 110–116. [Google Scholar] [CrossRef]
  32. ISO 3104; Petroleum Products—Transparent and Opaque Liquids—Determination of Kinematic Viscosity and Calculation of Dynamic Viscosity. International Organization for Standardization: Geneva, Switzerland, 2020.
  33. IEC 62021-1:2003; Insulating Liquids—Determination of Acidity—Part 1: Automatic Potentiometric Titration. International Electrotechnical Commission: Geneva, Switzerland, 2003.
  34. Uncu, O.; Ozen, B.; Tokatli, F. Use of FTIR and UV–visible spectroscopy in determination of chemical characteristics of olive oils. Talanta 2019, 201, 65–73. [Google Scholar] [CrossRef] [PubMed]
  35. Wang, K.; Wang, F.; Zhao, Q.; Li, J.; Lou, Z.; Han, Q.; Hu, K. Thermal Aging Characteristics of Newly Synthesized Triester Insulation Oil. IEEE Access 2019, 7, 175576–175583. [Google Scholar] [CrossRef]
Figure 1. Electrode system used to create inhomogeneous electric field for PD testing.
Figure 1. Electrode system used to create inhomogeneous electric field for PD testing.
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Figure 2. Voltage ramp used for PD testing.
Figure 2. Voltage ramp used for PD testing.
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Figure 3. Vibration viscometer SV-10 with thermostat.
Figure 3. Vibration viscometer SV-10 with thermostat.
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Figure 4. Diram (a) water content and (b) Coulometer KOH/USB.
Figure 4. Diram (a) water content and (b) Coulometer KOH/USB.
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Figure 5. Temperature dependence of dissipation factor for aged oils and for compatibility testing.
Figure 5. Temperature dependence of dissipation factor for aged oils and for compatibility testing.
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Figure 6. Temperature dependence of volume resistivity for aged oils and for compatibility testing.
Figure 6. Temperature dependence of volume resistivity for aged oils and for compatibility testing.
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Figure 7. Measured hardness of transformer synthetic rubber seal after aging in different oils at 120 °C, 2000 h and 140 °C, 1000 h.
Figure 7. Measured hardness of transformer synthetic rubber seal after aging in different oils at 120 °C, 2000 h and 140 °C, 1000 h.
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Figure 8. Weight of synthetic rubber seal after test at 120 and 140 °C.
Figure 8. Weight of synthetic rubber seal after test at 120 and 140 °C.
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Figure 9. Viscosity of mineral and Envitrafol oil test after test at 120 and 140 °C with and without submerged synthetic rubber.
Figure 9. Viscosity of mineral and Envitrafol oil test after test at 120 and 140 °C with and without submerged synthetic rubber.
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Figure 10. Water content of insulations liquids before and after aging test at 120 and 140 °C with and without submerged synthetic rubber: (a) Envitrafol, (b) Nynas Lyra.
Figure 10. Water content of insulations liquids before and after aging test at 120 and 140 °C with and without submerged synthetic rubber: (a) Envitrafol, (b) Nynas Lyra.
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Figure 11. ATR spectra of rapeseed oil.
Figure 11. ATR spectra of rapeseed oil.
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Figure 12. ATR spectra of mineral oil.
Figure 12. ATR spectra of mineral oil.
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Figure 13. ATR spectra of rapeseed oil.
Figure 13. ATR spectra of rapeseed oil.
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Figure 14. ATR spectra of mineral oil—detail.
Figure 14. ATR spectra of mineral oil—detail.
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Figure 15. Detailed view of the vibration of antioxidant.
Figure 15. Detailed view of the vibration of antioxidant.
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Figure 16. Detailed view of carbonyl area.
Figure 16. Detailed view of carbonyl area.
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Figure 17. Detailed view of the vibration of antioxidant of rapeseed oil.
Figure 17. Detailed view of the vibration of antioxidant of rapeseed oil.
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Figure 18. Detailed view of the vibration of antioxidant of mineral oil.
Figure 18. Detailed view of the vibration of antioxidant of mineral oil.
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Figure 19. Comparison of measured PD charge over voltage increments in different fluids: NE—blue, MIDEL—red, Nynas—green.
Figure 19. Comparison of measured PD charge over voltage increments in different fluids: NE—blue, MIDEL—red, Nynas—green.
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Figure 20. PRPD diagram for the first and last step of the test procedure for FR3—(a) PDIV level, (b) level before the breakdown.
Figure 20. PRPD diagram for the first and last step of the test procedure for FR3—(a) PDIV level, (b) level before the breakdown.
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Figure 21. PRPD diagram for the first and last step of test procedure for Nynas Taurus—(a) PDIV level, (b) level before the breakdown.
Figure 21. PRPD diagram for the first and last step of test procedure for Nynas Taurus—(a) PDIV level, (b) level before the breakdown.
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Table 1. Tensile strength of PA.
Table 1. Tensile strength of PA.
Fmax (N)140 °C/1000 h120 °C/2000 h
PA in rapeseed oil232.29360.21
PA in Nynas Lyra57.7864.22
Table 2. Assignments of main functional groups of rapeseed oil.
Table 2. Assignments of main functional groups of rapeseed oil.
Wavenumber (cm−1)Functional Group
3009stretching of olefinic double bonds attributed to unsaturated fatty acid
2924 and 2854

1745

1654

1464–983

1462

1377

1125–1095

723
methylene absorbance peaks are associated with antisymmetric and symmetric stretching vibrations of aliphatic
stretching vibration of carbonyl groups of the triacylglycerols
stretching vibration of cis-olefin

fingerprint region—bending vibrations of aliphatic groups as well as rocking vibrations
scissoring vibration

methyl symmetrical bending vibration

stretching vibration of ester groups and CH2 wag

overlapping of the (CH2)n rocking vibration and out-of-plane vibration (-CH wag) of cis-di-substituted olefins
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MDPI and ACS Style

Trnka, P.; Hornak, J.; Trnkova, M.; Michal, O.; Mokra, Z.; Slama, P.; Kopriva, J.; Prosr, P.; Leffler, J.; Frana, Z. Compatibility Testing of New Insulating Fluids and Materials in Distribution Transformer. Energies 2025, 18, 1831. https://doi.org/10.3390/en18071831

AMA Style

Trnka P, Hornak J, Trnkova M, Michal O, Mokra Z, Slama P, Kopriva J, Prosr P, Leffler J, Frana Z. Compatibility Testing of New Insulating Fluids and Materials in Distribution Transformer. Energies. 2025; 18(7):1831. https://doi.org/10.3390/en18071831

Chicago/Turabian Style

Trnka, Pavel, Jaroslav Hornak, Magdalena Trnkova, Ondrej Michal, Zdislava Mokra, Pavel Slama, Jiri Kopriva, Pavel Prosr, Jan Leffler, and Zdenek Frana. 2025. "Compatibility Testing of New Insulating Fluids and Materials in Distribution Transformer" Energies 18, no. 7: 1831. https://doi.org/10.3390/en18071831

APA Style

Trnka, P., Hornak, J., Trnkova, M., Michal, O., Mokra, Z., Slama, P., Kopriva, J., Prosr, P., Leffler, J., & Frana, Z. (2025). Compatibility Testing of New Insulating Fluids and Materials in Distribution Transformer. Energies, 18(7), 1831. https://doi.org/10.3390/en18071831

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