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| Alphabetical [« »] part 30 parted 1 particle 7 particles 89 particular 4 particularly 2 particulars 1 | Frequency [« »] 94 two 92 then 90 very 89 particles 86 heat 85 glass 84 together | Michael Faraday Lectures on the Forces of Matter IntraText - Concordances particles |
Lecture
1 II | suppose I take a few iron particles [dropping some small fragments 2 II | where bodies fall it is the particles that are attracted. You 3 II | these, then, as separate particles magnified, so as to be evident 4 II | present, and when these particles are placed upon it, see 5 II | Now just as these iron particles hold together in the form 6 II | bridge, so do the different particles of iron which constitute 7 II | the attraction between the particles that it is held together 8 II | nothing more than separate the particles which compose these two 9 II | does still exist in those particles; for here is a piece of 10 II | attraction between its separate particles; for if I take these portions 11 II | to the attraction of the particles, forming, as it were, the 12 II | great pains to bring the particles together, you see perhaps 13 II | power of attraction in its particles - giving to it such strength - 14 II | before the little set of particles in the small space equal 15 II | the attraction of their particles, and I am going to make 16 II | is this attraction of the particles. [The lectured here placed 17 II | supported by these little particles of the wire, just as in 18 II | make this attraction of the particles a little more simple? There 19 II | the attraction of their particles, and it I press these two 20 II | together, so as to bring their particles within the sphere of attraction, 21 II | of the attraction of the particles.~This, however, is not the 22 II | best way of bringing those particles together; we have many better 23 II | attraction exerted between the particles of bodies to hold them together. 24 II | dissolve the alum; all the particles will be separated by the 25 II | to-morrow, find that these particles of alum which I have put 26 II | To-morrow you will see the particles of alum drawn together; 27 II | simply a collection of small particles of no definite shape or 28 II | circumstances has had its particles so brought together that 29 II | to the attraction of the particles one for the other being 30 II | different manner in which its particles are arranged by the force 31 II | internal arrangement of the particles of this calcareous spar 32 III| it will show you that the particles of alum have done something 33 III| strong attraction which the particles of alum have for each other.~ 34 III| the manner in which the particles of bodies - of solid bodies - 35 III| the attraction between the particles is so weakened that it is 36 III| lessening the adhesion of the particles, although he is not exactly 37 III| because the attraction of the particles to each other is sufficient 38 III| attraction of some of the particles is so much diminished that 39 III| which existed between the particles of the ice, for below a 40 III| certain temperature the particles of water increase in their 41 III| of attraction between the particles of ice, we made use of another 42 III| the attraction between the particles of ice. Here you see the 43 III| the mere circumstance that particles attract each other. But 44 III| rod of fluid mercury, the particles of which have attraction 45 III| strong attraction of the particles of the water. Let me show 46 III| that the soap makes the particles of the water more adhesive 47 III| manner the attraction of the particles (and let me advise you, 48 III| power of cohesion of the particles of liquids. For instance, 49 III| Now if it were not for the particles of liquid cohering together, 50 III| attractive force between its particles, and yet you see that there 51 III| increase the attraction of the particles by cold or otherwise. So 52 III| the bulk occupied by the particles increased by giving them 53 III| gases produced by colorless particles themselves mixing together, 54 III| of the attraction of the particles for each other. You see 55 III| the condition in which its particles are arranged. If I were 56 III| is capable of drawing off particles from the water and sending 57 III| you see that one set of particles (H) is coming off twice 58 III| consists of two kinds of particles attracting each other in 59 III| the attraction between particles of a different nature one 60 III| upon the energy with which particles of different kinds attract 61 III| Oxygen and hydrogen are particles of different kinds, and 62 III| eight times as heavy as the particles of hydrogen in the water; 63 III| means of a sieve, the fine particles of iron filings through 64 IV | which there is between its particles to make it hold together 65 IV | jars (oxygen being those particles derived from the water which 66 IV | gives us certain gaseous particles. Here, then, is the hydrogen. 67 IV | understand that we can have particles of very different k_nds, 68 IV | how exceedingly different particles are one from the other; 69 IV | water so produced and the particles of which it consists chemically. 70 IV | combine these different particles together without producing 71 IV | these two different sets of particles together and I want to show 72 IV | place when we make different particles act together. Now I can 73 IV | attraction of cohesion of the particles. Again, here is a little 74 IV | instance: here are some oxygen particles, and here is a lump of carbon 75 IV | here is a lump of carbon particles. I am going to put the carbon 76 IV | going to put the carbon particles into the oxygen; they can 77 IV | oxygen, and if I put these particles of metal into it the two 78 IV | attraction between different particles exists also most curiously 79 IV | by reason of some of its particles gaining access to the air. 80 IV | the very finely divided particles of cotton being diffused 81 IV | has caught these raised particles, and it has run from one 82 IV | it contains supplies the particles with that without which 83 IV | attraction of the different particles one to the other that we 84 V | spoke of the attraction of particles of the same kind to each 85 V | into water, that there were particles of two different kinds attracted 86 V | not attract any of its own particles, so that there we obtained 87 V | affinity, or of aggregation of particles, or of cohesion, or of electricity ( 88 VI | it, so that both sets of particles will have an equal chance 89 VI | identical chemical force of the particles of zinc acting, and yet,