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  • A physical reaction where candy mint mentos are dropped into diet soda.  The sugar coatings on the mints acts like a perfect nucleation site for the dissolved carbon dioxide in the soda to turn into bubbles.  The result is the majority of the carbon dioxide changes from liquid to gas form in just a few seconds.  This sudden change of phase causes a plume of soda to be ejected from the bottle at great force causing the soda to make a fountain two meters high.
    K07HSmentos025.jpg
  • A child experimnets with dropping mentos mints into diet soda.  A physical reaction where candy mint mentos are dropped into diet soda.  The sugar coatings on the mints acts like a perfect nucleation site for the dissolved carbon dioxide in the soda to turn into bubbles.  The result is the majority of the carbon dioxide changes from liquid to gas form in just a few seconds.  This sudden change of phase causes a plume of soda to be ejected from the bottle at great force causing the soda to make a fountain two meters high.
    K07HSmentos027.jpg
  • 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.
    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.  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.
    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.
    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.
    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.
    K10BZRXN3560.tif
  • A young girl demonstrates her paper mache volcano reacting with vinegar and baking soda. This is an acid - base neutralization reaction which produces water and a salt as reactants.
    K10volcano002.JPG
  • A golf club moving at 97 miles per hour (43.36 m/s) hits a stationary golf ball.  The action is recorded by a fast strobe with a duration of 1/20,000th of a second.  In all collisions momentum is conserved. .
    K07-golfb0167.jpg
  • A golf club moving at 97 miles per hour (43.36 m/s) hits a stationary golf ball.  The action is recorded by a fast strobe with a duration of 1/1,000,000th of a second.  In all collisions momentum is conserved. .
    K07-golfb0152.jpg
  • A golf club moving at 97 miles per hour (43.36 m/s) hits a stationary golf ball.  The action is recorded by a fast strobe with a duration of 1/1,000,000th of a second.  In all collisions momentum is conserved.   This ball is a soft driving ball - not a regulation play ball..
    K07-golfb0147.jpg
  • A car spark plug firing.  The spark plug is the trigger that causes the gasoline to burn at a specific time in the cars internal combustion engine.  The spark plug fires and give the gas/air mixture the activation energy to start to burn.  This is a critical component in the thermodynamic cycle of an internal combustion engine.  A dirty or poorly adjusted spark plug will cause an engine to mis-fire, or fail to run.
    K10sparkplug_2234.jpg
  • A stroboscopic image of a hammer striking a nail into wood.
    K09hammer4266.jpg
  • Scanning electron microscope image of a Bald-faced hornet stinger(Vespula maculata)   Once the barbs are set into the victim, the poison flows between the two blades of the stinger.  The claibration bar is 20 um and the magnification is 2,880x..
    K08sembaldfacedhornet008b.jpg
  • A mallet is used to smash a green apple.
    K09malletsmash5595.jpg
  • Scanning electron microscope image of a Honey Bee Stinger. (Apis mellifera)  The large sack on the left produces the poison.  Once the barbs are set into the victim, the poison flows between the two blades of the stinger.  This image represents a field of view of 2 mm...
    K08sembeestinger047.jpg
  • A close-up car spark plug firing.  The spark plug is the trigger that causes the gasoline to burn at a specific time in the cars internal combustion engine.  The spark plug fires and give the gas/air mixture the activation energy to start to burn.  This is a critical component in the thermodynamic cycle of an internal combustion engine.  A dirty or poorly adjusted spark plug will cause an engine to mis-fire, or fail to run.
    K10sparkplug2362.jpg
  • A car spark plug firing.  The spark plug is the trigger that causes the gasoline to burn at a specific time in the cars internal combustion engine.  The spark plug fires and give the gas/air mixture the activation energy to start to burn.  This is a critical component in the thermodynamic cycle of an internal combustion engine.  A dirty or poorly adjusted spark plug will cause an engine to mis-fire, or fail to run.
    K10sparkplug2330.jpg
  • A mallet is used to smash an apple.
    K09malletsmash5614.jpg
  • A stroboscopic image of a hammer striking a nail into wood.
    K09hammer4403.jpg
  • A stroboscopic image of a hammer striking a nail into wood.
    K09hammer4388.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-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-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-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-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-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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