Dynamic Light Scattering (DLS) is one of the most commonly used techniques for size determination of nanoparticles (NPs) in suspension solution. DLS determines hydrodynamic size of the NPs in the suspension by measuring fluctuating intensities of scattered light induced by the Brownian motion of the NPs. Depending on the refractive index and structure of the NPs, DLS can theoretically measure NPs with hydrodynamic size in the range of 0.3 nm - 10 um, but usually NPs with a hydrodynamic size between 2 – 3,000 nm is recommended[1]. Concentration of samples in DLS measurements is about 108 – 1012 particles per mL which can be up to 1000 times higher than concentration of samples in another scattering based method - Nanoparticle Tracking Analysis (NTA)[8]. Theoretically, DLS is able to resolve particles in mixture when their diameters ratio is 1:3 (i.e. 100 nm particles can be resolved from 300 nm particles). In practice, that ratio is 1:4. In comparison with the NTA technique, DLS can measure hydrodynamic sizes of NPs in a wider size range, higher concentration range, and lower size resolution[1]. Additionally, the intensity of scattered light is related to the refractive index of the NPs and proportion to the sixth power of the diameter. Hence, DLS is sensitive to impurities, especially large particles with high refractive indices, and is not suitable for measuring samples containing other interfering NPs.
DLS is used to measure the hydrodynamic size of the particles in suspension solutions. The particles undergo Brownian motion at different velocities in the suspension depending on their size. The variation of scattered laser beam by these particles is measured over time. This intensity fluctuation of laser light can be used to analyze the hydrodynamic size of a particle from its correlation function of intensity fluctuations (small particles have faster Brownian motion than large particles, so the correlation function decreases faster). The diffusion coefficient can be determined by measuring the decreasing rate of the correlation function according to the size of particles. The hydrodynamic diameter of a particle can be calculated by substituting the value of diffusion coefficient into the Stokes-Einstein equation .
Stokes-Einstein equation
The Stokes-Einstein equation, where D(H) is the hydrodynamic diameter, kB is the Boltzmann constant, T is the absolute temperature, η is the viscosity, and D is the diffusion coefficient. The particle diffusion coefficient is obtained through the reduction rate of the correlation function and the spherical hydrodynamic diameter is derived from the above equation. Therefore, an error may occur if the sample is not spherical.
ii. Set a sample name. The sample name may include sample type, manufacturing size, solvent, and time.
iii. Select a material. Some materials are already defined in the software. If the material to be measured is not in the software list, the refractive index and absorption should be added to the list using the “Add” button.
iv. Select a dispersant for solvent setting. Some solvents with specific temperature and viscosity are already defined in the software. If the solvent you are using is not in the software list, you can add viscosity at a specific temperature using the “Add” button.
v. Leave it to default.
vi. Set the measurement temperature (generally at room temperature-25℃). Select Equilibrium time(the equilibrium time is the time to stabilize the sample temperature and is set to 120 seconds by default; user can change this values, for example 30s, typical value is 30s).
vii. The cuvette DTS0012 is suitable for large sample volume (> 2mL). The cuvette ZEN0118 is used when the sample volume is small (approx. 50uL).
b. Setting the measurement duration affects the accuracy and repeatability of the results. For Automatic setting, the software automatically determines the appropriate duration time. Most samples are left as default. The automatic measurement is divided into a minimum of 10 seconds.
Set the duration time between 1 and 600 seconds. Be careful not to set the time too long because the measurement time is too long and may cause sedimentation.
Normally 3 times. Set 10 times if you want an accurate measurement (depending on sample or situation). However, in this case, it is necessary to be able to distinguish abnormal results because there are many repeated analysis times.
Make sure that the there is no excessive ambient vibration during the measurement.
After the measurement, select the measured data in the Records View and check the Quality Report. The Attenuator index of good measurements is lower than 11 and greater than 0. In addition, PdI (Polydispersity) index must be less than 1.000.
Column 1 is time and column 2 is hydrodynamic diameter; they are fixed. Column 2 in figure 2 is transformed to Row 1 in figure 3. Column 3 in figure 2 is transformed to Row 2 in figure 3.
Column 4 in figure 2 is transformed to Row 3 in figure 3. Column 5 in figure 2 is transformed to Row 4 in figure iv. Column 6 in figure iii is transformed to Row 5 in figure iv.