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  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.  This image is part of a series.
    K10BZRXN3572.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.
    K10BZRXN3563.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.  This image is part of a series.
    K10BZRXN3584.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.  This image is part of a series.
    K10BZRXN3581.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.  This image is part of a series.
    K10BZRXN3578.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.  This image is part of a series.
    K10BZRXN3575.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.
    K10BZRXN3566.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.
    K10BZRXN3569.tif
  • Chemical waves in a Belousov-Zhabotinsky (BZ) reagent. This is a well-mixed solution of citric acid, potassium bromate and a cerium sulphate catalyst. If the local relative concentrations in the reagent are altered, for example by the impact of a dust particle on the surface, the equilibrium of the reaction is disturbed. The reaction then oscillates between oxidation and reduction. The oscillation propagates through the solution as a concentration front (yellow lines), caused by the dynamic coupling between the propagation rate of the reaction and the rates of diffusion of the reagents. Such chemical waves may be modeled using chaos mathematics.
    K10BZRXN3560.tif
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glow2A.jpg
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glow2-010A.jpg
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glowmushC8381 copy.jpg
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glow1-043.jpg
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glowmushC8370.jpg
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glowmush1A.jpg
  • A species of glow in the dark mushroom, Panellus stipticus. This naturally occurring bio-luminescent mushroom is common in New England forests in the fall. This species lives on partially decayed oak and uses a unique chemical reaction to digest chemicals in the oak that are toxic to other fungi. Part of a series showing the mushroom in visible and bio-luminescent light.
    K13-glowmush1-combo.jpg
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