Open Access

Spectroscopic determination of alkyl resorcinol concentration in hydroxyapatite composite

Journal of Analytical Science and Technology20167:9

DOI: 10.1186/s40543-016-0089-2

Received: 4 February 2016

Accepted: 8 March 2016

Published: 14 March 2016



Recently, alkyl resorcinol compounds showed remarkable improvements on dental implant restoration as well as anaesthetic, antiseptic, and anthelmintic applications. In this study, we prepared biologically functional composition of 4-hexylresorcinol (4HR)-loaded hydroxyapatite (HA).


Attenuated total reflectance (ATR) Fourier-transform infrared (FT-IR) spectroscopy fully assigned vibrational absorptions of 4-hexylresorcinol as well as the HA. The absorption coefficient of 4HR aqueous solution is estimated to be 1393 ± 61 cm−1 M−1 at highly diluted concentration. The 4HR was loaded with 0.018 % (wt/wt) in the 4HR-HA composite.


We quantitatively determined the micromolar concentration of 4HR loaded in the composite based on ultraviolet-visible (UV-Vis) absorption spectroscopy.


4-hexylresorcinol Hydroxyapatite ATR-FT-IR UV-Vis



Hydroxyapatite (HA) is the major component of bone material and a hexagonally packed crystal with hydroxyl end members (Pleshko et al. 1991). HA analogue materials have been extensively developed through a variety of chemical and physical routes (Ferraz et al. 2004; Bouyer et al. 2000; Cengiz et al. 2008). One of tremendous use of HA is bone grafting application via coating metallic dental implant surface, which stimulates bone healing and therefore improves implant integration rate and strength (Cook et al. 1987; Lange and Donath 1989). According to previous reports, however, HA-coated dental implants have often failed because of bacterial infection (Chang and Tanaka 2002; Destainville et al. 2003; Coates 2000). Hence, infection-resistant HA coating with bioinert antiseptic function is of great interest. Recently, a 4-hexylresorcinol (4HR)-treated HA-titanium dental implant showed significant improvement in both bone formation and bone-to-implant contact after implant surgery (Kim et al. 2011a).

Alkyl resorcinols, natural non-isoprenoid phenolic lipids found in plants (Tyman 1979), have attracted much attention due to a variety of biologic functions, such as being nonspecific antioxidants, antimutagens, and regulatory molecules (Kim et al. 2011b). Hexylresorcinol is an organic compound with well-known anaesthetic, antiseptic, and anthelmintic properties (Wilson and Gisvold 1954). By now, hexylresorcinol have been used in a variety of application areas, such as skincare products with anti-aging function, food additive with estrogenic activity (Amadasi et al. 2009), and anti-cancer activity by inhibiting NF-κB (Kim et al. 2011a). Hexylresorcinol inhibits the formation of graft-induced foreign body giant cells (Kweon et al. 2014). Therefore, hexylresorcinol has been used for bone substitute-related tissue engineering (Lee et al. 2015).

Several routes have been tried to deposit 4HR on the hydrophilic HA; however, precise control of 4HR loading amount is still challenging because of the amphiphilic character of 4HR (Kim et al. 2011b). Therefore, quantitative determination of the loading amount is importantly required to further optimize composite materials with a demanded function (Kweon et al. 2014; Lee et al. 2015). In this study, solution-processed 4HR-loaded HA composite were quantitatively characterized using Fourier-transform infrared (FT-IR) and ultraviolet-visible (UV-Vis) absorption spectroscopies. Infinitesimal amount of 4HR, which was loaded on HA powder, could be detected and precisely estimated based on UV-Vis absorption spectroscopy. Additionally, we entirely assigned IR absorption peaks of 4HR for the first time.

Material and methods

Chemicals and materials

Hydroxyapatite (reagent grade) and 4-hexylresorcinol (98 %) were used as received from Sigma Aldrich. 4HR-loaded HA composite (4HR-HA) was prepared in aqueous medium for FT-IR and UV-Vis absorption study. 0.5 g of hydroxyapatite was mixed with 50 ml of 0.1 M 4-hexylresorcinol aqueous solution and then stirred at 200 rpm for 1 h. The suspension was finally filtered and dried for 24 h.

Spectroscopic characterization

FT-IR absorption spectra were obtained using a Fourier-transform spectrometer (Vertex 80, Bruker Optics) equipped with an attenuated total reflectance (ATR) accessory (MIRacle, PIKE technologies). Spectrum was recorded in the spectral range of 600 to 4000 cm−1 at a resolution of 2 cm−1 with a mercury cadmium telluride detectors (MCT detector), and 128 repeated scans were averaged for each spectrum. The UV-Vis absorption spectra were obtained using a spectrophotometer (S-3100, Scinco).

Results and discussion

We performed FT-IR absorption study to evaluate the loading amount of 4HR in HA composite powder. Figure 1 shows IR absorption spectrum of the bare HA powder, which presented the phosphate band between 900 and 1200 cm−1. In Fig. 1, there are PO4 3− ν1 mode at 962 cm−1 (Chang and Tanaka 2002; Kim et al. 2011a; Han et al. 2006) and PO4 3− ν3 mode at 1028 (Chang and Raynaud et al. 2002; Destainville et al. 2003; Kim et al. 2011b; Han et al. 2006; Kim et al. 2012), 1088 (Chang and Raynaud et al. 2002; Destainville et al. 2003; Kim et al. 2011a; Han et al. 2006; Kim et al. 2012), and 870 cm−1 (Destainville et al. 2003; Han et al. 2006) band for HPO4 3− and labile PO4 3− mode at 632 cm−1 (Chang and Tanaka 2002; Kim et al. 2011b). Adsorbed water shows relatively wide stretching vibrational absorption in mid-IR region from 3600 to 3000 cm−1 with a distinct peak at 3572 cm−1. The absorption peak observed at 3572 cm–1 indicates the presence of the –OH group (Kim et al. 2011a; Raynaud et al. 2002; Han et al. 2006; Kim et al. 2012). Summarized data are shown in Table 1.
Fig. 1

FT-IR absorption spectra of the HA and the 4HR-loaded HA

Table 1

Characteristic IR absorptions of hydroxyapatite

Wavenumber (cm−1)







(Kim et al. 2011a; Raynaud et al. 2002; Han et al. 2006; Kim et al. 2012)




(Meejoo et al. 2006)

1028, 1088

PO4 3− (ν3)

3, 4

(Chang & Raynaud et al. 2002; Destainville et al. 2003; Kim et al. 2011b; Han et al. 2006; Kim et al. 2012)


PO4 3− (ν1)


(Chang and Tanaka 2002; Kim et al. 2011a; Han et al. 2006)


HPO4 3−


(Destainville et al. 2003; Han et al. 2006)


Labile PO4 3−


(Chang and Tanaka 2002; Kim et al. 2011b)

Figure 2 shows the FT-IR absorption spectrum of 4-hexylresorcinol. The vibrational absorption peak at 3039 cm−1 corresponds to the aromatic hydrocarbon, and the absorbance peaks at 3340 and 3419 cm−1 are assigned to hydrogen bonding between hydroxyl groups in benzene ring (Kim et al. 2012). The characteristic C–H stretching vibrations for saturated aliphatic species occur between 3000 and 2800 cm−1, and the corresponding simple bending vibrations nominally occur between 1500 and 1300 cm−1. The absorption peaks at 2960, 2922, 2873, and 2856 cm–1 are corresponding to the well-known asymmetric and symmetric stretching modes of aliphatic hydrocarbons (Coates 2000; Kim et al. 2011b; Kim et al. 2012; Krimm et al. 1956). Aromatic ring stretching vibration was observed at 1620 and 1527 cm−1 (Coates 2000). The absorption at 1452 cm–1 and the two weak peaks at 1435 and 1377 cm−1 are corresponding to the bending mode and the asymmetric and symmetric stretching modes of the aliphatic hydrocarbons, respectively (Coates 2000; Krimm et al. 1956). The phenolic OH bending mode of phenol species occurs at 1398 cm−1 (Coates 2000). The absorption peak at 1304 cm−1 reveals aliphatic CH2 wagging mode in disordered phase (Krimm et al. 1956). The intense absorptions at 1234, 1217, 1192, 1155, and 924 cm−1 are responsible for the C–O stretching modes in phenol species (Silverstein et al. 1991; Choo et al. 2011). The absorption peak at 1116 cm−1 can be assigned to the C–C–H bending mode (Cui et al. 2013). The absorption peaks at 1095, 974, 891 and 740, and 725 cm−1 were assigned to the C–C stretching mode (Krimm et al. 1956; Gómez-Sánchez et al. 2011), the CH2 wagging or twisting mode (Hallos 1984), the CH3 rocking mode (Krimm et al. 1956), and the CH2 rocking mode (Coates 2000; Krimm et al. 1956) of aliphatic hydrocarbons, respectively. The absorption peaks at 1047 cm−1 are for the OH deformation stretching mode (Frost et al. 2007). The IR absorption peaks at 864, 839, 800, 791, and 779 cm−1 can be assigned to the aromatic C–H out-of-plane bending mode (Coates 2000; Silverstein et al. 1991). The peaks at 696 and 617 cm−1 are assigned to the out-of-plane ring C=C bending and OH out-of-plane bending modes, respectively (Silverstein et al. 1991). Detailed assignments are fully summarized in Table 2.
Fig. 2

FT-IR absorption spectrum of 4-hexylresocinol

Table 2

Characteristic IR absorptions of 4-hexylresorcinol

Wavenumber (cm−1)




3340, 3419

Hydrogen bonded OH stretching

1, 2

(Kim et al. 2012)


Aromatic CH stretching


(Kim et al. 2012)


Aliphatic CH3 asymmetric stretching


(Coates 2000; Kim et al. 2012)


Aliphatic CH2 asymmetric stretching


(Coates 2000; Kim et al. 2011a; Kim et al. 2012)


Aliphatic CH3 symmetric stretching


(Coates 2000; Kim et al. 2012)


Aliphatic CH2 symmetric stretching


(Coates 2000; Kim et al. 2011b; Kim et al. 2012)

1620, 1527

Aromatic ring C–C stretching

8, 9

(Coates 2000)


Aliphatic CH2 bending


(Coates 2000; Krimm et al. 1956)


Aliphatic CH3 asymmetric bending


(Coates 2000)


Phenolic OH bending


(Coates 2000)


Aliphatic CH3 symmetric bending


(Coates 2000; Krimm et al. 1956)


Aliphatic CH2 wagging (disordered phase)


(Krimm et al. 1956)

1234, 1217, 1192, 1155

C–O stretching


(Silverstein et al. 1991; Choo et al. 2011)


C–C–H bending


(Hallos 1984)


C–C stretching


(Krimm et al. 1956; Frost et al. 2007)


OH deformation stretching


(Evanoff and Chumanov 2004)


CH2 wagging or twisting


(Kozubek and Tyman 1999)


C–O stretching


(Cui et al. 2013; Gómez-Sánchez et al. 2011)


CH3 rocking


(Krimm et al. 1956)

864, 839, 800, 791, 779

Aromatic C–H out-of-plane bending


(Coates 2000; Silverstein et al. 1991)

725, 740

CH2 rocking


(Coates 2000; Krimm et al. 1956)


Out-of-plane ring C=C bending


(Silverstein et al. 1991)


OH out-of-plane bending


(Silverstein et al. 1991)

FT-IR spectrum of the 4HR-HA composite showed the majority absorptions for the HA without any distinct change (Fig. 1). Additionally, very weak C–H stretching absorption corresponding to the 4HR is observed in the region of 2800–3000 cm−1 (asterisk indicated). After 4-hexylresorcinol treatment, the 4HR-HA composite showed enhanced absorption at 3260 cm−1 (arrow indicated). This can be attributed to hydrogen bonding between 4HR and HA. However, it is still ambiguous to precisely estimate 4HR concentration in this composite.

From the absorption spectrum in the UV-Vis region (Fig. 3), the 4HR aqueous solution showed the characteristic absorption at ~270 nm, corresponding to π–π* electronic transition (Silverstein et al. 1991). As a function of concentration, absorption coefficient value is decreased (inset of Fig. 3a). According to the previous reports, alkyl resorcinols with a long hydrocarbon tail easily tend to aggregate to form micelles in an aqueous medium (Kozubek and Tyman 1999), hence, inevitably reducing absorption efficiency. Therefore, the absorption coefficient of 4HR aqueous solution is estimated at a highly diluted concentration, which enabled the absorption coefficient of 1393 ± 61 cm−1 M−1.
Fig. 3

UV-Vis absorption spectra of the 4HR (a) and the 4HR-loaded HA composite powder (b). Inset of a is the absorption coefficients of 4HR as a function of concentration. Inset of b is the absorption spectrum of the HA powder aqueous mixture (5 mg/ml)

The additional absorption was also shown at ~430 nm, which is attributed to the scattering of HA powder. A colloidal powder suspension typically scatters light in the visible region. The scattering absorption can vary as a function of colloidal particle size (Evanoff and Chumanov 2004; Chae et al. 2009). In this study, the bulk HA powder showed a broad scattering with a maximum at 535 nm. As the HA was treated with 4HR, the scattering peak was observed at 430 nm. This blue-shifted scattering seems to be attributed to the fragmentation of the HA powder after 4HR treatment.

It is noteworthy that the absorption spectrum of the 4HR-loaded HA powder clearly reveals the presence of 4HA. The measured absorbance of 0.0065 is corresponding to 4.7 μM concentration and 3.5 μg 4HR in a standard cuvette. Regarding the total 4HR-HA composite powder mass of 19 mg for the UV-Vis measurement, the 4HR was loaded with 0.018 % (wt/wt) in the 4HR-HA composite. This small loading amount reasonably explains why IR spectroscopy need to take extra special care on sampling to determine the 4HR concentration even in ATR mode with a typical detection limit of ~0.1 wt % or 10−4 M.


We estimated an amount of 4-hexylresorcinol compound from its composite form with hydroxyapatite using FT-IR and UV-Vis absorption spectroscopies. Because of the majority IR absorptions of HA, the precise estimation of 4HR concentration in the 4HR-HA composite is a little ambiguous using FT-IR spectroscopy. On the other hand, the 4HR-HA composite showed clear absorption for 4HR in the ultraviolet region. Based on UV-Vis absorption spectroscopy, we effectively estimated the micromolar quantity of the loaded 4HR in the 4HR-HA composite.



This research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (NRF-2015R1D1A1A01058935).

Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors’ Affiliations

Analysis Research Division, Daegu Center, Korea Basic Science Institute
Space-Time Resolved Molecular Imaging Research Team, Korea Basic Science Institute
Department of Oral and Maxillofacial Surgery, College of Dentistry, Gangneung-Wonju National University


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