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Original Articles

Rapid determination of the dry weight of single, living cyanobacterial cells using the Mach-Zehnder double-beam interference microscope

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Pages 355-364 | Received 08 Oct 2007, Accepted 13 Mar 2008, Published online: 27 Nov 2008

Figures & data

Fig. 1. Phormidium sp. in the monochromatic (λ = 546 nm) stripe field of the Leitz Dualbeam microinterferometer. The optical path difference (OPD) caused by the object leads to a curvature in the interference stripe. The distance between the undisturbed stripes is the direct measure of the OPD and can be read out directly from the image.

Fig. 1. Phormidium sp. in the monochromatic (λ = 546 nm) stripe field of the Leitz Dualbeam microinterferometer. The optical path difference (OPD) caused by the object leads to a curvature in the interference stripe. The distance between the undisturbed stripes is the direct measure of the OPD and can be read out directly from the image.

Fig. 2. (A) Determination of OPD by phase-stepping algorithm. This method is suitable for coloured or complex objects like Gloeocapsa. The bright field image shows that the algae have a green colour due to chlorophyll content, so the specific interference colour of the cell in the homogenous field is a mixture in the chlorophyll specific colour. By shifting the overall phase between reference and object wave in four different positions, which differ by a quarter of a wavelength or π/2 (where 2π is a full wavelength) the OPD distribution in the image plane can be calculated by a phase stepping algorithm (Schwider, Citation1983). (B) The result is a false coloured picture, in which OPD can be determined.

Fig. 2. (A) Determination of OPD by phase-stepping algorithm. This method is suitable for coloured or complex objects like Gloeocapsa. The bright field image shows that the algae have a green colour due to chlorophyll content, so the specific interference colour of the cell in the homogenous field is a mixture in the chlorophyll specific colour. By shifting the overall phase between reference and object wave in four different positions, which differ by a quarter of a wavelength or π/2 (where 2π is a full wavelength) the OPD distribution in the image plane can be calculated by a phase stepping algorithm (Schwider, Citation1983). (B) The result is a false coloured picture, in which OPD can be determined.

Table 1.  Trichome and cell sizes (diameter) of eight cyanobacterial species – comparison of two methods.

Fig. 3. Parameters related to coenobial diameters of Gloecapsa spec. Points represent single coenobia. (a) Cell numbers of single coenobia; (b) dry weight ratio mucous material per cell; (c) the total (cells and mucilage) dry weight of the coenobia.

Fig. 3. Parameters related to coenobial diameters of Gloecapsa spec. Points represent single coenobia. (a) Cell numbers of single coenobia; (b) dry weight ratio mucous material per cell; (c) the total (cells and mucilage) dry weight of the coenobia.

Table 2.  The optical path difference (OPD) of eight cyanobacterial species in relation to the means of trichome and cell diameters.

Table 3.  Mean values of the dry weight per unit biovolume of eight cyanobacterial species, calculated from OPD and size measurements; min–max values are from single cells and trichomes respectively.

Table 4.  Carbon content of 8 cyanobacterial species as a percentage of dry mass.

Table 5.  Dry weight per unit biovolume of six cyanobacterial species calculated by different authors.

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