2019
DOI: 10.3390/s19245482
|View full text |Cite
|
Sign up to set email alerts
|

Synergetic Sensing Effect of Sodium Carboxymethyl Cellulose and Bismuth on Cadmium Detection by Differential Pulse Anodic Stripping Voltammetry

Abstract: In the present work, a novel electrochemical sensor was developed for the detection of trace cadmium with high sensitivity and selectivity in an easy and eco-friendly way. Firstly, a glassy carbon electrode (GCE) was modified with nontoxic sodium carboxymethyl cellulose (CMC) by a simple drop-casting method, which was applied to detect cadmium by differential pulse anodic stripping voltammetry (DPASV) in a solution containing both target cadmium and eco-friendly bismuth ions, based on a quick electro-codeposit… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
8
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 24 publications
(10 citation statements)
references
References 53 publications
0
8
0
Order By: Relevance
“…The peaks at 1588 and 1407 cm –1 can be attributed to the symmetric −CH stretching vibrations of −CH 2 and −CH 3 alkyl groups in CMC and symmetric −CO stretching vibrations. The peak at 1003 cm –1 is due to −C–O stretching vibrations. FTIR spectra of exfoliated hBN and bulk hBN (Figure S2) display two significant peaks at 808 and 1386 cm –1 , which can be attributed to the out-of-plane B–N–B and in-plane B–N stretching in hBN, respectively. In the FTIR spectra of 3D-printed hBN/CMC, the peak for asymmetric −CO stretching was shifted to 1711 cm –1 . Also, the peaks for symmetric −CH stretching vibrations and symmetric −CO stretching vibrations were shifted to 1572 and 1412 cm –1 .…”
Section: Resultsmentioning
confidence: 99%
“…The peaks at 1588 and 1407 cm –1 can be attributed to the symmetric −CH stretching vibrations of −CH 2 and −CH 3 alkyl groups in CMC and symmetric −CO stretching vibrations. The peak at 1003 cm –1 is due to −C–O stretching vibrations. FTIR spectra of exfoliated hBN and bulk hBN (Figure S2) display two significant peaks at 808 and 1386 cm –1 , which can be attributed to the out-of-plane B–N–B and in-plane B–N stretching in hBN, respectively. In the FTIR spectra of 3D-printed hBN/CMC, the peak for asymmetric −CO stretching was shifted to 1711 cm –1 . Also, the peaks for symmetric −CH stretching vibrations and symmetric −CO stretching vibrations were shifted to 1572 and 1412 cm –1 .…”
Section: Resultsmentioning
confidence: 99%
“…4. For genuine CMC and PVP polymers and caffeic acid, the main vibrational bands were determined and followed by literature [25][26][27][28].…”
Section: Resultsmentioning
confidence: 99%
“…FTIR spectra of GG show a peak at 3285 cm À 1 due to the presence of -OH stretching vibration, 2914 cm À 1 is due to CÀ H stretching vibration, 1647 cm À 1 is due to the carbonyl group, and 1015 cm À 1 is due to OÀ H bending vibration. [45] In CMC, peaks at 3306 cm À 1 indicate the OH stretching vibration, and peaks at 2914 cm À 1 , 1647 cm À 1 , and 1379 cm À 1 show the CÀ H stretching vibration, carbonyl group stretching vibration, and CÀ O stretching respectively, [46] whereas peaks at 1016 cm À 1 are due to its glycosidic linkage. In the case of GG/epi/CMC, there is an almost similar adsorption peak with similar intensity.…”
Section: Fourier Transform Infrared Spectroscopymentioning
confidence: 99%