Quantitative high resolution light and EM autoradiography of fluorophosphate-esterase in developing mouse liver

1978 ◽  
Vol 36 (2) ◽  
pp. 66-67
Author(s):  
C. Budd
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Mouse Liver ◽  
Unit Area ◽  
Irreversible Inhibitor ◽  
Adult Mice ◽  
Quantitative Measurements ◽  
Em Autoradiography ◽  
Old Mice ◽  
Silver Grains

The distribution and concentration of fluorophosphate reactive (FPR) esterases in the liver of developing and adult mice was determined quantitatively from light and electron microscope autoradiograms of liver reacted with 3H - diisopropylfluorophosphate (3H-DFP) an irreversible inhibitor of carboxylesterases.The majority of labeled cells in the liver of 2, 8, 14 and 28- day-old mice and in adult mice (60-180 days old) were hepatocytes, but in the liver from 2-day-old mice and to a lesser extent 8-day-old mice, the autoradiographic silver grains were also concentrated over granulocytes of the intrahepatic hemopoietic population.Quantitative measurements of grain density (developed silver grains/unit area) in light microscope autoradiograms revealed an increase in the predominantly cytoplasmic concentration of FPR esterase sites in hepatocytes from 137o of the adult concentration in 2-day-old mice, to 497, and 78% of the adult concentration in 8- and 14-day-old animals, respectively.

scholarly journals DISTRIBUTION OF LEUCINE-3H DURING AXOPLASMIC TRANSPORT WITHIN REGENERATING NEURONS AS DETERMINED BY ELECTRON-MICROSCOPE RADIOAUTOGRAPHY

1972 ◽  
Vol 52 (3) ◽  
pp. 719-732 ◽  
Author(s):  
Thomas L. Lentz
Keyword(s):  
Electron Microscope ◽  
Short Distance ◽  
Unit Area ◽  
Trophic Factors ◽  
Nerve Terminals ◽  
Sensory Ganglia ◽  
Successive Addition ◽  
Myelinated Nerves ◽  
Almost All ◽  
Silver Grains

The distribution of leucine-3H in neurons was determined by electron-microscope radioautography after infusion of label into the spinal cord or sensory ganglia of regenerating newts. In the nerve cell bodies 3 days after infusion, the highest concentration of label per unit area occurred over the rough-surfaced endoplasmic reticulum. In the large brachial nerves, the silver grains were not distributed uniformly in the axoplasm, indicating that the labeled materials are restricted in their movement to certain regions of the axon. Almost all of the radioautographic grains observed in myelinated nerves could be accounted for by the presence of a uniformly labeled band occupying the area 1500–9000 A inside the axolemma. This region of the axon was rich in microtubules and organelles while the unlabeled central core of the axon contained mainly neurofilaments. This observation supports the hypothesis that microtubules are related to axonal transport. In small, vesicle-filled nerve terminals in the blastema, labeled material was restricted to a thin zone a short distance beneath the plasma membrane while the central region of the terminal was largely unlabeled. The peripheral pattern of labeling in the nerve endings is consistent with successive addition of newly synthesized proteins at the periphery of the growth cone and release of substances such as trophic factors at the nerve terminal.

TIMING AND LOCALIZATION OF THE STIMULATORY EFFECT OF FOLLICLE-STIMULATING HORMONE ON URIDINE INCORPORATION IN THE MOUSE TESTIS IN VIVO

1981 ◽  
Vol 88 (3) ◽  
pp. 443-449 ◽  
Author(s):  
A. G. DAVIES ◽  
N. R. LAWRENCE
Keyword(s):  
Sertoli Cells ◽  
Rna Synthesis ◽  
Germinal Cell ◽  
Human Pituitary ◽  
Stimulatory Action ◽  
Subcutaneous Injections ◽  
Adult Mice ◽  
Old Mice ◽  
Silver Grains

Human pituitary FSH increased the incorporation of [5-3H]uridine into RNA in vivo in the testes of intact 9-day-old mice and of hypophysectomized adults. In both groups the effect was greatest 8 h after administration of 5–7·5 i.u. FSH. Autoradiographs were prepared from the testes of hypophysectomized adult mice given subcutaneous injections of FSH or of 0·9% saline 6 h, and [5-3H]uridine 1·5 h, before death. Treatment with FSH caused statistically significant increases in the density of silver grains over the nuclei of Sertoli cells, type A and intermediate spermatogonia, and preleptotene and mid-pachytene primary spermatocytes. It was concluded that FSH has a generalized stimulatory action on RNA synthesis in the nuclei of Sertoli cells and those types of germinal cell which synthesize RNA most actively.

Radiation Damage, Contrast and Statistics in High Resolution Biological Electron Microscopy

1970 ◽  
Vol 28 ◽  
pp. 260-261
Author(s):  
Robert M. Glaeser
Keyword(s):  
High Resolution ◽  
Particle Flux ◽  
Unit Area ◽  
Signal To Noise ◽  
Resolution Image ◽  
High Resolution Image ◽  
Pass Through ◽  
Counting Statistics ◽  
The Relationship ◽  
Picture Element

It is well known that a large flux of electrons must pass through a specimen in order to obtain a high resolution image while a smaller particle flux is satisfactory for a low resolution image. The minimum particle flux that is required depends upon the contrast in the image and the signal-to-noise (S/N) ratio at which the data are considered acceptable. For a given S/N associated with statistical fluxtuations, the relationship between contrast and “counting statistics” is s131_eqn1, where C = contrast; r2 is the area of a picture element corresponding to the resolution, r; N is the number of electrons incident per unit area of the specimen; f is the fraction of electrons that contribute to formation of the image, relative to the total number of electrons incident upon the object.

The High Resolution Scanning Transmission Electron Microscope

1974 ◽  
Vol 32 ◽  
pp. 316-317
Author(s):  
A. V. Crewe
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
High Vacuum ◽  
Scanning Transmission Electron Microscope ◽  
Ultra High Vacuum ◽  
Resolving Power ◽  
Imaging Characteristics ◽  
Transmission Electron ◽  
Scanning Transmission ◽  
The Moment

The high resolution STEM is now a fact of life. I think that we have, in the last few years, demonstrated that this instrument is capable of the same resolving power as a CEM but is sufficiently different in its imaging characteristics to offer some real advantages.It seems possible to prove in a quite general way that only a field emission source can give adequate intensity for the highest resolution^ and at the moment this means operating at ultra high vacuum levels. Our experience, however, is that neither the source nor the vacuum are difficult to manage and indeed are simpler than many other systems and substantially trouble-free.

A Liquid Nitrogen Cooled Stage for STEM

1974 ◽  
Vol 32 ◽  
pp. 444-445
Author(s):  
Louis T. Germinario
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Liquid Nitrogen ◽  
Room Temperature ◽  
Objective Lens ◽  
Thermal Drift ◽  
Specimen Holder ◽  
Resolution Capability ◽  
Focal Position

A liquid nitrogen stage has been developed for the JEOL JEM-100B electron microscope equipped with a scanning attachment. The design is a modification of the standard JEM-100B SEM specimen holder with specimen cooling to any temperatures In the range ~ 55°K to room temperature. Since the specimen plane is maintained at the ‘high resolution’ focal position of the objective lens and ‘bumping’ and thermal drift la minimized by supercooling the liquid nitrogen, the high resolution capability of the microscope is maintained (Fig.4).

An Analysis of Dissociation of Molecules in a High Resolution Electron Microscope

1973 ◽  
Vol 31 ◽  
pp. 486-487
Author(s):  
Mihir Parikh
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Cross Sections ◽  
Resolving Power ◽  
Peak Intensity ◽  
Molecular Film ◽  
Resolution Electron ◽  
Dissociation Cross Section ◽  
High Resolution Electron Microscope ◽  
The Stability

It is well known that the resolution of bio-molecules in a high resolution electron microscope depends not just on the physical resolving power of the instrument, but also on the stability of these molecules under the electron beam. Experimentally, the damage to the bio-molecules is commo ly monitored by the decrease in the intensity of the diffraction pattern, or more quantitatively by the decrease in the peaks of an energy loss spectrum. In the latter case the exposure, EC, to decrease the peak intensity from IO to I’O can be related to the molecular dissociation cross-section, σD, by EC = ℓn(IO /I’O) /ℓD. Qu ntitative data on damage cross-sections are just being reported, However, the microscopist needs to know the explicit dependence of damage on: (1) the molecular properties, (2) the density and characteristics of the molecular film and that of the support film, if any, (3) the temperature of the molecular film and (4) certain characteristics of the electron microscope used

Quantitative Measurements on the Ion Etching of TMV

1973 ◽  
Vol 31 ◽  
pp. 336-337
Author(s):  
Irwin Bendet ◽  
Nabil Rizk
Keyword(s):  
Electron Microscope ◽  
Tobacco Mosaic Virus ◽  
Mosaic Virus ◽  
Ion Current ◽  
Beam Diameter ◽  
Ion Etching ◽  
Preliminary Results ◽  
Quantitative Measurements ◽  
Monitoring Devices

Preliminary results reported last year on the ion etching of tobacco mosaic virus indicated that the diameter of the virus decreased more rapidly at 10KV than at 5KV, perhaps reaching a constant value before disappearing completely.In order to follow the effects of ion etching on TMV more quantitatively we have designed and built a second apparatus (Fig. 1), which incorporates monitoring devices for measuring ion current and vacuum as well as accelerating voltage. In addition, the beam diameter has been increased to approximately 1 cm., so that ten electron microscope grids can be exposed to the beam simultaneously.

A New High Resolution Transmission Electron Microscope with Second-Zone Objective Lens

1969 ◽  
Vol 27 ◽  
pp. 176-177 ◽  
Author(s):  
H. Tochigi ◽  
H. Uchida ◽  
S. Shirai ◽  
K. Akashi ◽  
D. J. Evins ◽  
...  
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Transmission Electron Microscope ◽  
Objective Lens ◽  
High Excitation ◽  
Transmission Electron ◽  
New Instrument

A New High Excitation Objective Lens (Second-Zone Objective Lens) was discussed at Twenty-Sixth Annual EMSA Meeting. A new commercially available Transmission Electron Microscope incorporating this new lens has been completed.Major advantages of the new instrument allow an extremely small beam to be produced on the specimen plane which minimizes specimen beam damages, reduces contamination and drift.

Field Emission SEM Equipped With Noise Compensator

1973 ◽  
Vol 31 ◽  
pp. 302-303
Author(s):  
S. Saito ◽  
H. Todokoro ◽  
S. Nomura ◽  
T. Komoda
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Scanning Electron Microscope ◽  
Field Emission ◽  
Low Contrast ◽  
Probe Current ◽  
High Resolution Images ◽  
Scanning Electron

Field emission scanning electron microscope (FESEM) features extremely high resolution images, and offers many valuable information. But, for a specimen which gives low contrast images, lateral stripes appear in images. These stripes are resulted from signal fluctuations caused by probe current noises. In order to obtain good images without stripes, the fluctuations should be less than 1%, especially for low contrast images. For this purpose, the authors realized a noise compensator, and applied this to the FESEM.Fig. 1 shows an outline of FESEM equipped with a noise compensator. Two apertures are provided gust under the field emission gun.

To What Extent are Inelastically Scattered Electrons Useful in the Stem?

1973 ◽  
Vol 31 ◽  
pp. 286-287 ◽  
Author(s):  
H. Rose
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Electron Correlation ◽  
Quantum Noise ◽  
Collection Efficiency ◽  
Scanning Transmission Electron Microscope ◽  
Electron Cloud ◽  
Scanning Time ◽  
Transmission Electron ◽  
Scanning Transmission

The scanning transmission electron microscope offers the possibility of utilizing inelastically scattered electrons. Use of these electrons in addition to the elastically scattered electrons should reduce the scanning time (dose) Which is necessary to keep the quantum noise below a certain level. Hence it should lower the radiation damage. For high resolution, Where the collection efficiency of elastically scattered electrons is small, the use of Inelastically scattered electrons should become more and more favorable because they can all be detected by means of a spectrometer. Unfortunately, the Inelastic scattering Is a non-localized interaction due to the electron-electron correlation, occurring predominantly at the circumference of the atomic electron cloud.

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