Transition temperatures in the sensitivity of escherichia coli B/r to lysozyme

Lysozyme attacked Escherichia coli B/r in the absence of EDTA or imposed osmotic shocks when the cells were rapidly cooled below specific temperatures. Cells subjected to lysozyme while being cooled to below 20°C began to lose ability to subsequently form colonies. This sensitivity increased with decreasing temperatures and almost all cells cooled to 0°C were affected. Slightly hypertonic solutions did not improve survival. Cells cooled first to as low as 5°C and then subjected to lysozyme while cool did not lose their ability to form colonies subsequent to rewarming. However, 70% of the cells cooled first to 0°C and subjected to lysozyme lost their colony-forming ability. Cell lysis also began when treated near 5°C, but even when treated at 0°C about 50% of the cells maintained their rod shape in the presence of lysozyme. These results are discussed in terms of a possible phase transition in a portion of the cell envelope and/or a transient osmotic swelling as a results of metabolic pumps failing at the low temperatures.     

Visualization of freezing damage. II. Structural alterations during warming

There is a growing amount of indirect evidence which suggests that the loss in viability of rapidly cooled cells is due to recrystallization of intracellular ice. This possibility was tested by an evaluation of the formation of morphological artifacts in rapidly cooled cells to determine whether this process can account for the loss in viability. Samples of the common yeast Saccharomyces cerevisiae were frozen at 1.8 or 1500 °C/min, and the structure of the frozen cells was examined by the use of freeze-fracturing techniques. Other cells cooled at the same rate were warmed to temperatures ranging from ?20 ° to ?50 °C and then rapidly cooled to ?196 °C, a procedure that should cause small ice crystals to coalesce by the process of migratory recrystallization. Cells cooled at 1500 °C/min and then warmed to temperatures above ?40 °C formed large intracellular ice crystals within 30 min, and appreciable recrystallization occurred at temperatures as low as ?45 °C. Cells cooled at 1.8 °C/min and warmed to temperatures as high as ?20 °C underwent little structural alteration. These results demonstrate that intracellular ice can cause morphological artifacts. The correlation between the temperature at which rapid recrystallization begins and the temperature at which the cells are inactivated indicates that recrystallization is responsible for the death of rapidly cooled cells.     

Excitation energy transfer to Photosystem I in filaments and heterocysts of Nostoc punctiforme

Cyanobacteria adapt to varying light conditions by controlling the amount of excitation energy to the photosystems. On the minute time scale this leads to redirection of the excitation energy, usually referred to as state transitions, which involves movement of the phycobilisomes. We have studied short-term light adaptation in isolated heterocysts and intact filaments from the cyanobacterium Nostoc punctiforme ATCC 29133. In N.punctiforme vegetative cells differentiate into heterocysts where nitrogen fixation takes place. Photosystem II is inactivated in the heterocysts, and the abundancy of Photosystem I is increased relative to the vegetative cells. To study light-induced changes in energy transfer to Photosystem I, pre-illumination was made to dark adapted isolated heterocysts. Illumination wavelengths were chosen to excite Photosystem I (708 nm) or phycobilisomes (560 nm) specifically. In heterocysts that were pre-illuminated at 708 nm, fluorescence from the phycobilisome terminal emitter was observed in the 77 K emission spectrum. However, illumination with 560 nm light caused quenching of the emission from the terminal emitter, with a simultaneous increase in the emission at 750 nm, indicating that the 560 nm pre-illumination caused trimerization of Photosystem I. Excitation spectra showed that 560 nm pre-illumination led to an increase in excitation transfer from the phycobilisomes to trimeric Photosystem I. Illumination at 708 nm did not lead to increased energy transfer from the phycobilisome to Photosystem I compared to dark adapted samples. The measurements were repeated using intact filaments containing vegetative cells, and found to give very similar results as the heterocysts. This demonstrates that molecular events leading to increased excitation energy transfer to Photosystem I, including trimerization, are independent of Photosystem II activity.     

The study of the primary photoprocesses in Photosystem I of chloroplasts Recombination luminescence,chlorophyll triplet state and triplet-triplet annihilation

The dependence of the delayed luminescence of Photosystem I on the state of the reaction centers has been studied. Light flash induces a charge separation in the centers: $\text{P-700 · P-430}\textcolor{red}{}\text{P-700}{}^{\mathrm{+}}\text{· P-430}{}^{\mathrm{?}}$. Dark recombination of charges is accompanied by the recombination luminescence with $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 20}\text{ms}$.If the centers are in the P-700 · P-430^? state or if P-430 is inactivated by heat, then flashing of Photosystem I generates the triplet state chlorophyll with $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 0.5}\text{ms}$. The triplet state has been measured by the delayed fluorescence of chlorophyll at 20 °C and 77 °K and by the chlorophyll phosphorescence at 77 °K. The delayed fluorescence at 20 °C arises from the thermal activation of the triplet state up to the excited singlet level of chlorophyll and at 77 °K it is due to triplet-triplet annihilation. The quantum yield of the triplet formation, estimated by a comparison of the light saturation curves of delayed fluorescence at 20 °C and of P-700 photooxidation under the same experimental (optical) conditions, is ≈ 0.9 of the P-700⁺ yield. Only one triplet of chlorophyll can be generated per P-700. Under heat inactivation of P-430 the triplet formation is not observed when P-700 is oxidized.It is assumed that the triplet-triplet annihilation at 77 °K is related with the strong interaction between the chlorophyll molecules in the pigment complex of Photosystem I. The possibility of a triplet participation in the primary processes of photosynthesis is discussed.     

Optimizing conditions for cryopreservation of an insect cell line

A cell line (UM-BGE-2) derived from embryos of the cockroach Blattella germanica was frozen to ?196 °C under a variety of conditions and cell viability was assayed after warming. It was found that cell viability was affected by the cooling rate, the warming rate, the controlled cooling endpoint temperature, and the type and concentration of cryoprotectant. The best survival for cells suspended in Grace's tissue culture medium containing 1 M Me₂SO was obtained when cells were cooled at 1 °C/ min to at least ?90 °C before being placed in liquid nitrogen and warmed at more than 900 °C/min. Cultures initiated from these frozen cells produce typical growth curves and appear normal after several passages.     

Dichlorophenylurea-resistant oxygen evolution in Chlorella after cerulenin treatment

Fluorescence spectra at 77 K, oxygen evolution at 30°C and delayed fluorescence at 25°C were measured in Chlorella pyrenoidosa cultures with and without cerulenin and subsequent 3-(3,4-dichlorophenyl)-1,1-dimethyl urea (DCMU) treatment, respectively. In pure algal cultures the oxygen evolution was inhibited by DCMU and the long-time component of fluorescence was, highly influenced by DCMU, as expected. In contrast, both oxygen evolution and delayed fluorescence became DCMU-resistant in cerulenin-treated cultures. The DCMU-resistance is correlated with a change in the fatty acid distribution of the thylakoid membrane, which also leads to changes in the prompt fluorescence. Cerulenin appears to be a promising new tool of diagnostics for the hitherto unsatisfactorily understood processes of oxygen evolution in photosynthesizing organisms.     

Survival of the parasitic protozoan, Babesia bigemina, in blood cooled at widely different rates to -196 degrees C

Survival of the parasitic protozoan, Babesia bigemina, in blood cooled at widely different rates to ? 196°C. International Journal for Parasitology4: 169–172. The infectivity of Babesia bigemina in blood containing 2 m DMSO was tested in 99 cattle after the blood had been cooled to ? 196°C at eight rates ranging from 0·73–3070°C/min. Blood cooled at each rate was infective; 95 of the recipients became infected, the exceptions being four of the seven cattle inoculated with blood cooled at 3070° C/min. The infectivity of blood cooled at 39, 82 and 212°C/min was higher than that of blood cooled at slower or faster rates. Least depression of infectivity occurred at 82°C/min.     

Reversible inhibition of photochemistry of photosystem II by Ca2+ removal from intact cells of Anacystis nidulans

Depletion of Ca²⁺ from Anacystis nidulans produces an inhibition of O₂ evolution that is accompanied both at 39°C and 77 K by a loss of chlorophyll fluorescence of variable yield. This indicates that Ca²⁺-depletion causes disruption of normal photosystem II function, manifested by the disappearance of photoreduction of Q. Delayed light emission in the ms time range is also eliminated in Ca²⁺-depleted cells, which confirms that Ca²⁺ removal prevents charge separation and recombination in reaction centers of photosystem II. Readdition of Ca²⁺ to depleted cells restores fully the fluorescence of variable yield and delayed light emission, as well as O₂ evolution. Thus, Ca²⁺ may be a required component for photosystem II in A. nidulans.     

The lipid integrity of membranes of guinea pig alveolar macrophages studied by nanosecond fluorescence decay of 1,6-diphenyl-1,3,5-hexatriene: The effect of stimulation by concanavalin A and formyl peptides1

Time-resolved fluorescence anisotropy of 1,6-diphenyl-1,3,5-hexatriene was used to monitor physical changes in the membranes of guinea pig alveolar macrophages following stimulation by N-formyl peptides (either N-formylmethionylphenylalanine (FMP) or N-formyl methionyl leucylphenylalanine (FMLP)) and concanavalin A. The anisotropy of diphenylhexatriene in macrophages showed a dependence on stimulation both in the rate of decay and in the value of anisotropy at infinite time. Subtle differences were observed between the effect of concanavalin A and FMLP on the membrane lipid fluidity as detected by fluorescence anisotropy. Concanavalin A stimulation of macrophages decreased the value of the anisotropy at infinite times in the range of 0–20 °C and increased the value at 25–40 °C; and at all temperatures it decreased the rate of decay of anisotropy. At temperatures below 25 °C, the response to FMLP was similar to concanavalin A, but above 25 °C, FMLP only slightly modified the anisotropy decay profile. Another physical parameter, calcium permeability, was examined because Ca⁺² fluxes are dependent upon membrane properties. The temperature-dependent profiles of concanavalin A and FMP-stimulated ⁴⁵Ca⁺² efflux from alveolar macrophages were similar. The rate and extent of ⁴⁵Ca⁺² efflux increased from 4 to 22 °C, with no further increases observed up to 37 °C. This pattern correlated well with observed changes in membrane fluidity.     

Nanosecond fluorescence from isolated photosynthetic reaction centers of Rhodopseudomonas sphaeroides

The time-course of fluorescence from reaction centers isolated from Rhodopseudomonas sphaeroides was measured using single-photon counting techniques. When electron transfer is blocked by the reduction of the electron-accepting quinones, reaction centers exhibit a relatively long-lived (delayed) fluorescence due to back reactions that regenerate the excited state (P*) from the transient radical-pair state, P^F. The delayed fluorescence can be resolved into three components, with lifetimes of 0.7, 3.2 and 11 ns at 295 K. The slowest component decays with the same time-constant as the absorbance changes due to P^F, and it depends on both temperature and magnetic fields in the same way that the absorbance changes do. The time-constants for the two faster components of delayed fluorescence are essentially independent of temperature and magnetic fields. The fluorescence also includes a very fast (prompt) component that is similar in amplitude to that obtained from unreduced reaction centers. The prompt fluorescence presumably is emitted mainly during the period before the initial charge-transfer reaction creates P^F from P*. From the amplitudes of the prompt and delayed fluorescence, we calculate an initial standard free-energy difference between P* and P^F of about 0.16 eV at 295 K, and 0.05 eV at 80 K, depending somewhat on the properties of the solvent. The multiphasic decay of the delayed fluorescence is interpreted in terms of relaxations in the free energy of P^F with time, totalling about 0.05 eV at 295 K, possibly resulting from nuclear movements in the electron-carriers or the protein.     

Thermal adaptation of Tetrahymena membranes with special reference to mitochondria II. Preferential interaction of cardiolipin with specific molecular species of phospholipid

A specific effect of cardiolipin on fluidity of mitochondrial membranes was demonstrated in Tetrahymena cells acclimated to a lower temperature in the previous report (Yamauchi, T., Ohki, K., Maruyama, H. and Nozawa, Y. (1981) Biochim. Biophys. Acta 649, 385–392). This study was further confirmed by the experiment using fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH). Anisotropy of DPH for microsomal and pellicular total lipids from Tetrahymena cells showed that membrane fluidity of these lipids increased gradually as the cells were incubated at 15°C after the shift down of growth temperature from 39°C. However, membrane fluidity of mitochondrial total lipids was kept constant up to 10 h. This finding is compatible with the result obtained using spin probe in the previous report. Additionally, the break-point temperature of DPH anisotropy was not changed in mitochondrial lipids whereas those temperatures in pellicular and microsomal lipids lowered during the incubation at 15°C. Interaction between cardiolipins and various phospholipids, which were isolated from Tetrahymena cells grown at 39°C or 15°C and synthesized chemically, was investigated extensively using a spin labeling technique. The addition of cardiolipins from Tetrahymena cells grown at either 39°C or 15°C did not change the membrane fluidity (measured at 15°C) of phosphatidylcholine from whole cells grown at 39°C. On the other hand, both cardiolipins of 39°C-grown and 15°C-grown cells decreased the membrane fluidity of phosphatidylcholine from Tetrahymena cells grown at 15°C. The same results were obtained for phosphatidylcholines of mitochondria and microsomes. Membrane fluidity of phosphatidylethanolamine, isolated from cells grown at 15°C, was reduced to a small extent by Tetrahymena cardiolipin whereas that of 39°C-grown cells was not changed. Representative molecular species of phosphatidylcholines of cells grown at 39°C and 15°C were synthesized chemically; 1-palmitoyl-2-oleoylphosphatidylcholine for 39°C-grown cells and dipalmitoleoylphosphatidylcholine for 15°C-grown ones. By the addition of Tetrahymena cardiolipin, the membrane fluidity of 1-palmitoyl-2-oleoylphosphatidylcholine was not changed but that of dipalmitoleoylphosphatidylcholine was decreased markedly. These phenomena were caused by Tetrahymena cardiolipin. However, bovine heart cardiolipin, which has a different composition of fatty acyl chains from the Tetrahymena one, exerted only a small effect.     

Light- and temperature-induced changes in the distribution of excitation energy between Photosystem I and Photosystem II in spinach leaves

The influence of light quality and temperature on the distribution of the absorbed quanta between Photosystem I (PS I) and Photosystem II (PS II) in spinach leaves has been studied from the characteristics of chlorophyll fluorescence at 77 K. Leaves were preilluminated at different temperatures with either PS I light (to establish State 1) or with PS II light (to establish State 2), then cooled to 77 K and measured for fluorescence. In State 1, energy distribution appeared to be unaffected by temperature. A transition to State 2 resulted in an increase in PS I fluorescence and a decrease in the PS II fluorescence, indicating that a larger fraction of energy becomes redistributed to PS I. However, the extent of this redistribution varied: it was only small at 5°C to 20°C, but it largely increased at temperatures exceeding 20°C. This variation in the extent was related to a change in the mechanism of the state transition: at 15°C only the ‘initial’ distribution of energy was affected, while at 35°C an additional increase in the spill-over constant, k_{T (II → I)}, was included. It is assumed that under physiological conditions k_{T (II → I)} is under the control of temperature rather than of light quality, whereby in leaves adapted to high physiological temperatures, the probability of energy spill-over from closed PS II centres to PS I is enhanced. In darkened leaves, the spill-over constant has been manipulated by preincubation at different temperatures. Then, the light-induced ‘energization’ of thylakoid membranes has been tested by measuring the light-induced electrochromic absorbance change at 515 nm (and light-induced light-scattering changes) in these leaves. The flash-induced 515 nm signal as well as the initial peak during a 1 s illumination were not affected by energy distribution. However, the amplitude of the pseudo-steady-state signal (as established during 1 s illumination) was considerably enhanced in leaves in which a larger fraction of the absorbed energy is distributed to PS I at the expense of PS II excitation. The results have been interpreted in such a way that an increase in energy spill-over from PS II to PS I favours a cyclic electron transport around PS I. It is discussed that changes in energy distribution (via spill-over) may serve to maintain a suitable balance between non-cyclic and cyclic electron transport in vivo.     

Heat shock response of Dictyostelium

In response to a shift from 22 to 30°C the relative rate of synthesis of a small number of proteins is dramatically increased in Dictyostelium discoideum. The cells neither grow nor develop at this temperature but die slowly with a half-life of 18 hr. The major protein synthesized in response to a heat shock to 30°C in either growing cells or developing cells has an apparent molecular weight of 70,000 (70K). An increase in the relative rate of synthesis of 70K can be seen as early as 20 min following heat shock. Synthesis of 70K remains high for 4 hr at 30°C and then decreases. Similar kinetics of 70K synthesis occur during recovery at 22°C following a 1-hr heat shock. RNA synthesis during the first half-hour of heat shock is essential for the high rate of 70K measured 2 hr later. By isoelectric focusing the 70K protein can be separated into two spots, one of which overlaps one of the major heat shock proteins of Drosophila melanogaster. The relative rate of synthesis of several other proteins (82K, 60K, 43K) increases less dramatically in Dictyostelium during heat shock at 30°C. A heat shock to 34°C results in rapid synthesis of these proteins but not of 70K. The relative rates of synthesis of most other proteins made at 22°C decreases, most notably that of actin. Synthesis of heat shock proteins at 30°C does not significantly affect viability at 30°C but dramatically prolongs the period of time the cells can survive at 34°C. Thus, 30°C appears to be a stasis condition for Dictyostelium which elicits a response essential for protection from lethal temperatures. The similarity of the heat shock response in Dictyostelium to that in Drosophila and vertebrate cells suggests that certain aspects of the response may be universal in eukaryotes.     

Cooling of embryonic cells,isolated blastoderms,and intact embryos of the zebra fish Brachydanio rerio to −196 °c

Single cells from the developing embryo of the zebra fish survive freezing when protected with 1 M DMSO and cooled to ?196 °C in two steps. Cell survival drops from 85 to 26% when clumps of 5–10 cells are similarly frozen, and to 2% when isolated blastoderms are treated in the same way. This drastic decrease in survival is interpreted as an example of the “scale-up problem,” in which diffusional barriers prevent cryoprotectant equilibration and osmotic dehydration in large cell assemblanges.Isolated blastoderms develop considerably in culture, and retain some of this ability following cooling to ?25 °C after protection with DMSO or glycerol.Intact embryos protected with high concentrations of glycerol (2.8 M) tolerate slow cooling to ?196 °C surprisingly well, with most of the embryonic cells morphologically intact and actively extruding lobopodia. Glycerol could, however, only be removed from cells by disrupting the embryo so that diffusional barriers were removed. DMSO (2.8 M) was ineffective in preserving embryos or cells cooled to ?196 °C.     

Viability and Morphology of rat heart cells after freezing and thawing of the whole heart

Intact adult rat hearts were cooled in the presence of 10% DMSO according to an external cooling program which approximated the optimal external three-step cooling program for the isolated adult heart cells: 20 min at ?20 °C, 0.2 °C/min from ?20 to ?25, ?30, or ?50 °C, and rapid cooling to ?196 °C. Following rapid thawing, cells were isolated after perfusion with a 0.1% collagenase solution. Only cells which originated from the free wall of the right ventricle could be isolated, even after cooling to ?20 °C. Most cells from hearts cooled to ?196 °C did not survive. When the third cooling step was omitted and the end temperature of the second cooling step was ?30 °C, 38% of the cells excluded trypan blue, 29% were morphologically intact, and 30% showed spontaneous contractions after thawing, expressed as percentages of the control, A much lower survival was found after cooling to ?50 °C.Histological and electron microscopical study of the heart immediately after thawing revealed no differences between hearts cooled to ?20, ?30, or ?196 °C. Also no marked differences were observed between the morphological integrity after freezing and thawing of the atrium, the left and right ventricle walls, and the ventricular septum. The survival data suggest the presence of nonmorphologically detectable alterations in cells frozen to ?196 °C, compared to cells frozen to ?30 °C. The morphological investigations indicate no essential differences in resistance of atrial and ventricular cells to the freezing process.Experiments involving neonatal rat hearts cooled to ?196 °C, according to the method which gave optimal preservation of the isolated cells, revealed that after thawing cells are present from which growing and contracting cultures can be derived. It appears that cells in the neonatal rat heart are more resistant to freezing to ?196 °C than cells in the adult rat heart.     

Microscopic observation of intracellular ice formation in unfertilized mouse ova as a function of cooling rate

A physical-chemical analysis of water loss from cells at subzero temperatures had shown that the likelihood of intracellular ice formation increased with increasing cooling rate (22). We have now used a modified version of a unique conductioncooled cryomicroscope stage (8) to observe the freezing of unfertilized mouse ova suspended in dimethyl sulfoxide. Survival measurements showed that the respective survivals of ova were about 65, 56, and 0% when they were cooled at rates of 0.2 to 1.5, 2.5, and 5.4 °C/min. Direct microscopic observation of mouse ova during freezing showed that the respective fractions of cells that froze intracellularly were 13, 72, and 100% when they were cooled at rates of 1.3, 2.9, and 4.8 °C/min or faster. These values agree with those predicted from the physical-chemical analysis for cells the size of mouse ova. The microscopic observations have also shown that intracellular freezing generally occurred at about ?40 to ?45 °C. We had previously observed that mouse embryos must be cooled slowly to ?50 °C or below if they are to survive subsequent rapid cooling to ?196 °C. The observation of intracellular ice formation at ?45 °C supports the interpretation that at temperatures above ?50 °C the embryos still contain water capable of freezing intracellularly.     

Properties of the low-temperature Photosystem I primary reaction in the P-700-chlorophyll a-protein

The Photosystem I primary reaction, as measured by electron paramagnetic resonance changes of P-700 and a bound iron-sulfur center, has been studied at 15°K in P-700-chlorophyll a-protein complexes isolated from a blue-green alga. One complex, prepared with sodium dodecyl sulfate shows P-700 photooxidation only at 300°K, whereas a second complex, prepared with Triton X-100, is photochemically active at 15°K as well as at 300°K. Analysis of these two preparations shows that the absence of low-temperature photoactivity in the sodium dodecyl sulfate complex reflects a lack of bound iron-sulfur centers in this preparation and supports the assignment of an iron-sulfur center as the primary electron acceptor of Photosystem I.     

Effect of cooling rate on human and murine hemopoietic precursor cell recovery

The effect of cooling rate on recovery of human and murine hemopoietic precursor cells was studied. In the presence of 10% Me₂SO, a cooling rate of 7 °C/min from ?4 to ?30 °C was optimal for recovery of both human and murine precursor cells which give rise to colonies in diffusion chambers implanted in mice (CFU-DG). Cooling of human marrow at a rate between 3 and 7 °C/min resulted in the best CFU-C recovery, although no good correlation between the cooling rate and murine CFU-C recovery was demonstrated. These data suggest that recovery of the primitive hemopoietic precursor cells can be improved by changing the standard cryopreservation programs used presently. However, improved recovery of CFU-DG does not necessarily translate into faster reconstitution of hemopoiesis. No significant difference was observed in overall recovery of bone marrow cellularity in lethally irradiated mice following injection of untreated marrow and marrow cooled at a rate of 1 and 7 °C/min.     

Freezing cytorrhysis and critical temperature thresholds for photosystem II in the peat moss Sphagnum capillifolium

Leaflets of Sphagnum capillifolium were exposed to temperatures from ?5°C to +60°C under controlled conditions while mounted on a microscope stage. The resultant cytological response to these temperature treatments was successfully monitored using a light and fluorescence microscope. In addition to the observable cytological changes during freezing cytorrhysis and heat exposure on the leaflets, the concomitant critical temperature thresholds for inactivation of photosystem II (PS II) were studied using a micro fibre optic and a chlorophyll fluorometer mounted to the microscope stage. Chlorophyllous cells of S. capillifolium showed extended freezing cytorrhysis immediately after ice nucleation at ?1.1°C in the water in which the leaflets were submersed during the measurement. The occurrence of freezing cytorrhysis, which was visually manifested by cell shrinkage, was highly dynamic and was completed within 2 s. A total reduction of the mean projected diameter of the chloroplast containing area during freezing cytorrhysis from 8.9 to 3.8 μm indicates a cell volume reduction of approximately ?82%. Simultaneous measurement of chlorophyll fluorescence of PS II was possible even through the frozen water in which the leaf samples were submersed. Freezing cytorrhysis was accompanied by a sudden rise of basic chlorophyll fluorescence. The critical freezing temperature threshold of PS II was identical to the ice nucleation temperature (?1.1°C). This is significantly above the temperature threshold at which frost damage to S. capillifolium leaflets occurs (?16.1°C; LT₅₀) which is higher than observed in most higher plants from the European Alps during summer. High temperature thresholds of PS II were 44.5°C which is significantly below the heat tolerance of chlorophyllous cells (49.9°C; LT₅₀). It is demonstrated that light and fluorescence microscopic techniques combined with simultaneous chlorophyll fluorescence measurements may act as a useful tool to study heat, low temperature, and ice-encasement effects on the cellular structure and primary photosynthetic processes of intact leaf tissues.