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9.5: Nanoparticle Deposition Studies Using a Quartz Crystal Microbalance

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    55931
  • Overview

    The working principle of a quartz crystal microbalance with dissipation (QCM-D) module is the utilization of the resonance properties of some piezoelectric of materials. A piezoelectric material is a material that exhibits an electrical field when a mechanical strain is applied. This phenomenon is also observed in the contrary where an applied electrical field produce a mechanical strain in the material. The material used is α-SiO2 that produces a very stable and constant frequency. The direction and magnitude of the mechanical strain is directly dependent of the direction of the applied electrical field and the inherent physical properties of the crystal.

    A special crystal cut is used, called AT-cut, which is obtain as wafers of the crystal of about 0.1 to 0.3 mm in width and 1 cm in diameter. The AT-cut is obtained when the wafer is cut at 35.25° of the main crystallographic axis of SiO2. This special cut allows only one vibration mode, the shear mode, to be accessed and thus exploited for analytical purposes. When a electrical field is applied to the crystal wafer via metal electrodes, that are vapor-deposited in the surface, a mechanical shear is produced and maintained as long as the electrical field is applied. Since this electric field can be controlled by opening and closing an electrical circuit, a resonance within the crystal is formed (Figure \(\PageIndex{1}\)).

    Figure \(\PageIndex{1}\) Schematic representation of the piezoelectric material: (a) a baseline is obtained by running the sensor without any flow or sample; (b) sample is starting to flow into the sensor; (c) sample deposited in the sensor change the frequency.

    Since the frequency of the resonance is dependent of the characteristics of the crystal, an increase of mass, for example when the sample is loaded into the sensor would change the frequency change. This relation \ref{1} was obtained by Sauerbrey in 1959, where Δm (ng.cm-2) is the areal mass, C (17.7 ngcm-2Hz-1) is the vibrational constant (shear, effective area, etc.), n in Hz is the resonant overtone, and Δf is the change in frequency. The dependence of the change in the frequency can be related directly to the change in mass deposited in the sensor only when three conditions are met and assumed:

    • The mass deposited is small compared to the mass of the sensor
    • It is rigid enough so that it vibrates with the sensor and does not suffer deformation
    • The mass is evenly distributed among the surface of the sensor

    \[ \Delta m\ =\ -C\frac{1}{n}\Delta f \label{1} \]

    An important incorporation in recent equipment is the use of the dissipation factor. The inclusion of the dissipation faster takes into account the weakening of the frequency as it travels along the newly deposited mass. In a rigid layer the frequency is usually constant and travels through the newly formed mass without interruption, thus, the dissipation is not important. On the other hand, when the deposited material has a soft consistency the dissipation of the frequency is increased. This effect can be monitored and related directly to the nature of the mass deposited.

    The applications of the QCM-D ranges from the deposition of nanoparticles into a surface, from the interaction of proteins within certain substrates. It can also monitors the bacterial amount of products when feed with different molecules, as the flexibility of the sensors into what can be deposited in them include nanoparticle, special functionalization or even cell and bacterias!

    Experimental Planning

    In order to use QCM-D for studing the interaction of nanoparticles with a specific surface several steps must be followed. For demonstration purposes the following procedure will describe the use of a Q-Sense E4 with autosampler from Biolin Scientific. A summary is shown below as a quick guide to follow, but further details will be explained:

    • Surface election and cleaning according with the manufacturer recommendations
    • Sample preparation including having the correct dilutions and enough samplke for the running experiment
    • Equipment cleaning and set up of the correct aparameters for the experiment
    • Data acquisition
    • Data interpretation

    Surface Election

    The decision of what surface of the the sensor to use is the most important decision to make fore each study. Biolin has a large library of available coatings ranging from different compositions of pure elements and oxides (Figure \(\PageIndex{2}\)) to specific binding proteins. It is important to take into account the different chemistries of the sensors and the results we are looking for. For example studying a protein with high sulfur content on a gold sensor can lead to a false deposition results, as gold and sulfur have a high affinity to form bonds. For the purpose of this example, a gold coated sensor will be used in the remainder of the discussion.

    Figure \(\PageIndex{2}\) From left to right, silica (SiO2), gold (Au), and iron oxide (Fe2O3) coated sensors. Each one is 1 cm in diameter.

    Sensor Cleaning

    Since QCM-D relies on the amount of mass that is deposited into the surface of the sensor, a thorough cleaning is needed to ensure there is no contaminants on the surface that can lead to errors in the measurement. The procedure the manufacturer established to clean a gold sensor is as follows:

    1. Put the sensor in the UV/ozone chamber for 10 minutes
    2. Prepare 10 mL of a 5:1:1 solution of hydrogen peroxide:ammonia:water
    3. Submerge in this solution at 75 C for 5 minutes
    4. Rinse with copious amount of milliQ water
    5. Dry with inert gas
    6. Put the sensor in the UV/ozone chamber for 10 minutes as shown in Figure \(\PageIndex{3}\).
    Figure \(\PageIndex{3}\) Gold sensors in loader of the UV/ozone chamber in the final step of the cleaning process.

    Once the sensors are clean, extreme caution should be taken to avoid contamination of the surface. The sensors can be loaded in the flow chamber of the equipment making sure that the T-mark of the sensor matches the T mark of the chamber in order to make sure the electrodes are in constant contact. The correct position is shown in Figure \(\PageIndex{4}\).

    Figure \(\PageIndex{4}\) Correct position of the sensor in the chamber.

    Sample Preparation

    As the top range of mass that can be detected is merely micrograms, solutions must be prepared accordingly. For a typical run, a buffer solution is needed in which the deposition will be studied as well as, the sample itself and a solution of 2% of sodium dodecylsulfate [CH3(CH2)10CH2OSO3Na, SDS]. For this example we will be using nanoparticles of magnetic iron oxide (nMag) coated with PAMS, and as a buffer 8% NaCl in DI water.

    • For the nanoparticles sample it is necessary to make sure the final concentration of the nanoparticles will not exceed 1 mM.
    • For the buffer solution, it is enough to dissolve 8 g of NaCl in DI water.
    • For the SDS solution, 2 g of SDS should be dissolved very slowly in approximate 200 mL of DI water, then 100 mL aliquots of DI water is added until the volume is 1 L. This is in order to avoid the formation of bubbles and foam in the solution.

    Instrument Preparation

    Due to the sensitivity of the equipment, it is important to rinse and clean the tubing before loading any sample or performing any experiments. To rinse the tubing and the chambers, use a solution of 2% of SDS. For this purpose, a cycle in the autosampler equipment is program with the steps shown in Table \(\PageIndex{1}\).

    Step Duration (min) Speed (μL/min) Volume (mL)
    DI water (2:2) 10 100 1
    SDS (1:1) 20 300 6
    DI water (1:2) 10 100 1
    Table \(\PageIndex{1}\) Summary of cleaning processes.

    Once the equipment is cleaned, it is ready to perform an experiment, a second program in the autosampler is loaded with the parameters shown in Table \(\PageIndex{2}\).

    Step Duration (min) Speed (μL/min) Volume (mL)
    Buffer (1:3) 7 100 0.7
    Nanoparticles 30 100 3.0
    Table \(\PageIndex{2}\) Experimental set-up

    The purpose of flowing the buffer in the beginning is to provide a background signal to take into account when running the samples. Usually a small quantity of the sample is loaded into the sensor at a very slow flow rate in order to let the deposition take place.

    Data Acquisition

    Example data obtained with the above parameters is shown in Figure \(\PageIndex{5}\). The blue squares depict the change in the frequency. As the experiment continues, the frequency decreases as more mass is deposited. On the other hand, shown as the red squares, the dissipation increases, describing the increase of both the height and certain loss of the rigidity in the layer from the top of the sensor. To illustrate the different steps of the experiment, each section has been color coded. The blue part of the data obtained corresponds to the flow of the buffer, while the yellow part corresponds to the deposition equilibrium of the nanoparticles onto the gold surface. After certain length of time equilibrium is reached and there is no further change. Once equilibrium indicates no change for about five minutes, it is safe to say the deposition will not change.

    Figure \(\PageIndex{5}\) Data of deposition of nMag in a gold surface.

    Instrument Clean-up

    As a measure preventive care for the equipment, the same cleaning procedure should be followed as what was done before loading the sample. Use of a 2% solution of SDS helps to ensure the equipment remains as clean as possible.

    Data Modeling

    Once the data has been obtained, QTools (software that is available in the software suit of the equipment) can be used to convert the change in the frequency to areal mass, via the Sauerbrey equation, \ref{1}. The correspondent graph of areal mass is shown in \ref{1}. From this graph we can observe how the mass is increasing as the nMag is deposited in the surface of the sensor. The blue section again illustrates the part of the experiment where only buffer was been flown to the chamber. The yellow part illustrates the deposition, while the green part shows no change in the mass after a period of time, which indicates the deposition is finished. The conversion from areal mass to mass is a simple process, as gold sensors come with a definite area of 1 cm2, but a more accurate measure should be taken when using functionalized sensors.

    Figure \(\PageIndex{6}\) Areal mass of deposition of nMag into gold surface.

    It is important to take into account the limitations of the Saubery equation, because the equation accounts for a uniform layer on top of the surface of the sensor. Deviations due to clusters of material deposited in one place or the formation of partial multilayers in the sensor cannot be calculated through this model. Further characterization of the surface should be done to have a more accurate model of the phenomena.

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