| Literature DB >> 26131680 |
Dalia El Khaled1,2, Nuria Novas3,4, Jose A Gazquez5,6, Rosa M Garcia7,8, Francisco Manzano-Agugliaro7,8.
Abstract
The demand for improved food quality has been accompanied by a technological boost. This fact enhances the possibility of improving the quality of horticultural products, leading towards healthier consumption of fruits and vegetables. A better electrical characterization of the dielectric properties of fruits and vegetables is required for this purpose. Moreover, a focused study of dielectric spectroscopy and advanced dielectric sensing is a highly interesting topic. This review explains the dielectric property basics and classifies the dielectric spectroscopy measurement techniques. It comprehensively and chronologically covers the dielectric experiments explored for fruits and vegetables, along with their appropriate sensing instrumentation, analytical modelling methods and conclusions. An in-depth definition of dielectric spectroscopy and its usefulness in the electric characterization of food materials is presented, along with the various sensor techniques used for dielectric measurements. The collective data are tabulated in a summary of the dielectric findings in horticultural field investigations, which will facilitate more advanced and focused explorations in the future.Entities:
Keywords: dielectric; fruits; non-destructive; quality; sensing; vegetables
Year: 2015 PMID: 26131680 PMCID: PMC4541835 DOI: 10.3390/s150715363
Source DB: PubMed Journal: Sensors (Basel) ISSN: 1424-8220 Impact factor: 3.576
Figure 1Example of ε′ and ε″ variations with frequency on a logarithmic scale.
Dielectric techniques.
| Brief Description | Recommended Materials | Frequency Range | Advantages | Disadvantages | |
|---|---|---|---|---|---|
| Parallel plate | Material must be placed between two electrodes to form a capacitor | Material with the ability to be formed as a flat smooth sheet <100 MHz | <100 MHz | Inexpensive, high accuracy | Limited frequency range, sheet sample very thin (<10 mm thick) |
| Lumped circuit | Sample is a part of the insulator in a lumped circuit | All materials with the exception of gazes | <100 MHz | Liquid and solid materials can be measured | Limited frequency range, not suitable for very low loss materials |
| Coaxial probe | A coaxial line cut off forming a flat plane boundary in contact with food. A vector analyser is needed to measure the reflection | Liquids and semi-solids | 200 MHz–20 GHz, even >100 GHz | Easy to use, non-destructive for some materials, sample preparation is not required | Limited accuracy (±5%). Low loss resolution, large samples and solids must show a flat surface |
| Transmission line | Brick-shaped sample fills the cross section of an enclosed transmission line, causing an impedance change | Liquids and solids | <100 MHz | More accurate and sensitive than the probe method | Less accuracy than resonators, sample preparation is difficult and time-consuming |
| Cavity resonator | Sample is introduced in a cavity (a high Q resonant structure), which affects the centre frequency and quality factor of the cavity | Solids | 1 MHz–100 GHz | Easy sample preparation, adaptable for a wide range of temperatures | Broadband frequency data are not provided and analysis may be complex |
| Free space | Antennas are used to direct a MW beam at or through the material. A vector network analyser measures the reflection and transmission coefficients of solids | Solids | MW range | Non-destructive, high temperatures can be used | A large flat, thin, parallel-faced sample and special calibration are required |
| Time domain spectroscopy | Short pulses of THz radiation within a generation and detection scheme that is sensitive to the effect of both the amplitude and phase of the radiation | Homogeneous | 10 MHz–10 GHz. | Fast and high accuracy measurement, small sample | Expensive |
Figure 2Dielectric property measurement techniques.
Material measurement techniques.
| Illustration | Material Under Test | Frequency | Other Comments | |
|---|---|---|---|---|
| Coaxial Probe | Lossy Material (liquids and semi-solids) | Broadband | Non-destructive | |
| Transmission Line | Lossy to low loss material (machineable solids) | Broadband | ||
| Free Space | Best for flat sheets, powder high temperature | Broadband | ||
| Resonant Cavity | Low loss materials, small samples | Single Frequency | Accurate | |
| Parallel Plate | Flat sheets | Low Frequencies | Thin | |
| Inductance measurement | Toroidal structures required | Accurate, simple measurement |
Figure 3The material measurement fixtures.
Figure 4Frequency Ranges applied for fruit and vegetable measurements.
Parameter Variation overview (Δ & ∇ for parameter increases and decreases, respectively).
| Fruit/Vegetable | Frequency | Temperature | Storage Time | Conclusions | ||||||
|---|---|---|---|---|---|---|---|---|---|---|
| ε′ | ε″ | Others | ε′ | ε″ | Others | ε′ | ε″ | Others | ||
| Apple | ∇ | Impedance ∇ Reactance ∇ | No pattern | No pattern | Conductance Δ Firmness Δ pH Δ | Linear decrease with frequency | ||||
| Avocado | At low freq. Δ At high freq. ∇ | At low freq. Δ | Inflection point at Critical edge freq. 100 MHz | |||||||
| Carrot | ∇ | ∇ | Inflection point at Critical edge freq. 100 MHz | |||||||
| Coconut | ∇ | Linear decrease with frequency | ||||||||
| Eggplant | ∇ | Linear decrease with frequency | ||||||||
| Conductance Δ Capacitance Δ Impedance ∇ | Δ | Equ. Capacitance ∇ Equ. Parallel capacitance Δ conductance Δ | Linear increase with storage time | |||||||
| ∇ | Energy storage capability ∇ | Relative permittivity Δ | Relative permittivity Δ | Linear decrease with frequency | ||||||
| ∇ | ∇ | Dp ∇ | ∇ | Δ | Dp ∇ | ∇ | ∇ | Linear decrease with frequency | ||
| Frequency linear relationship between 10 and 500 MHz | ||||||||||
| At low freq.Δ | At low freq.Δ | Dispersion shift to higher freq. | Temperature linear increase below 50 MHz | |||||||
| ∇ & Std. < 2% | V type & Std. < 10% | Dp Δ High correlation of:LR & freq. and LR & fruit firmness | linear ∇ | Frequency and temperature linear decrease | ||||||
| ∇ | ∇ | From −20 °C to 0 °C Δ From 0 °C to 100 °C ∇ | From −20 °C to 0 °C Δ From 0 °C to 100 °C Δ then ∇ | Frequency linear decrease, varying temperature pattern | ||||||
| Exponential ∇ | ∇ | ∇ then Δ at 915 MHz | Exponential relationship with frequency | |||||||
Figure 5(a) Loss factor behaviour versus frequency for carrots and peaches on a logarithmic scale; (b) Dielectric Constant behaviour versus frequency for carrots and peaches on a logarithmic scale.