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EltronBKP/ElectronC

This website contains an archive of files for the Acorn Electron, BBC Micro, Acorn Archimedes, Commodore 16 and Commodore 64 computers, which Dominic Ford has rescued from his private collection of floppy disks and cassettes.

Some of these files were originally commercial releases in the 1980s and 1990s, but they are now widely available online. I assume that copyright over them is no longer being asserted. If you own the copyright and would like files to be removed, please contact me.

Tape/disk: Home » Personal collection » Acorn ADFS disks » Electron » Pixel_map.ADF
Filename: EltronBKP/ElectronC
Read OK:
File size: 1D6E bytes
Load address: D0D6576
Exec address: 1010100
File contents
�.........*.......*.......*.......*.......*.......*.......*.......*.......*.<
	This still left the difficulty that Hertz had failed to deflect the
cathode rays by applying an electric field. Thomson was suspicious about
this result, for he knew of two previous experiments in which the rays had
apparently been deflected by electric fields. These experiments, by
Crookes and Goldstein in 1879 and 1880 respectively, used slightly
different apparatus, but the principle was the same. Two cathodes were
placed in the vacuum tube, and wired so they could be switched on or off
independently. With only one cathode active, the rays passed in a straight
line as usual, but when the second was swiched on, the two streams of rays
curved away from each other. Crookes said this showed that the rays were
negatively charged particles, which repelled each other and diverged as
they moved away from the cathodes. This explanation was disproved by
Wiedemann and Ebert in 1891, who showed that the deflection is in fact due
to the intense electric field surrounding the other cathode, not the rays
emanating from it. Once again, Crookes had come to the right conclusion
for the wrong reasons! 
	This experiment also explained why cathode rays are always emitted
normally from the surface of the cathode. The electric field next to any
perfect conductor is always perpendicular to its surface, and it is this
field that accelerates the rays away from the cathode. Hence the rays are
initially accelerated at right angles from the cathode, then deflected
according by the shape of the cathode or any other electrodes nearby.
	 Thomson repeated Hertz's experiment to deflect the rays, and
obtained the same result - the electric field between the plates did not
appear to make any difference to the path of the rays, however large he
made the voltage between the plates. The solution to this problem came
from Lenard's old observaion that cathode rays increase the electrical
conductivity of any gas which they pass through. Thomson related this to
his own experiments on gases ionised by X-rays, and concluded that cathode
rays too must generate charged gas molecules. If an electric field is set
up in a gas containing ions, the negative ions will move towards the
positive plate and the positive ions to the negative plate. This will
continue until enough ions have built up near the plates to balance out
the electric field due to the plates themselves. Of course some ions will
be discharged by collisions with the plates, but this will not occur fast
enough to prevent a layer of charged gas building up near the plates.
Hence after a short time the field due to the plates will not be felt at
all by the cathode rays, and they will not show any deflection. 
	To avoid this problem, the obvious solution was to pump away the
gas so there are no ions to build up on the plates. Thomson was lucky in
that the quality of vacuum pumps had greatly improved since Hertz's
experiments, and he was easily able to test his idea. As he predicted, 
the conductivity of the gas dropped rapidly as the air was pumped out, and
the rays were deflected.

(intermediate pressures?)

	Now there there were no known properties of the rays that could not
be explained in terms of particles. All that was left for Thomson to do
was to measure the deflections of the rays and calculate the physical
parameters of the particles, namely their velocity, charge and mass. One
attempt to measure the mass:charge ratio of the particles had already been
made by Schuster in the late 1880s, using the magnetic deflection alone as
follows The acceleration of a particle of mass m and charge e travelling
at speed v perpendicular to a magnetic field of magnitude B is given by
			Bev
		    a =	---
			 m                            
and directed perpendicular to the velocity and magnetic field. This causes
the rays to travel in a circle of radius r, given by
                   2
		   v    Bev                   mv
                 --- = ---    so that    r = --
                  r     m                    Be
	Thus by measuring the field B and radius of curvature r, Schuster
found a value for mv/e. To find the mass:charge ratio m/e from this, he
needed a value for the velocity v, which was not so easily measured and
had to be estimated. He did this by wrongly assuming that the particles in
the rays were in thermal equilibrium with the surrounding air molecules.
As Thomson points out this cannot possibly be the case, since the rays
would not travel in straight lines across the tube if they were all
reflecting from air molecules. From this assumption Schuster unfortunately
arrived at the conclusion that the rays must be streams of ionised air
molecules. When Hertz discovered that the rays could pass through solid
aluminium, the particle theory seemed to be in ridicule, since a stream
gas molecules could not possibly pass through an airtight seal and hardly
be attenuated! Some suggested that the impact of molecules on one side of
the sheet somehow stimulated a new emission of rays on the far side,
though it is not clear how this stimulus could travel through the metal.
	In 1894 Thomson had obtained his own estimate for the velocity of
the cathode rays, by measuring the time lag between switching on the rays,
and the appearence of the phosphorescence on the end of the tube. This
approach was also flawed, since the time lag is in fact caused by a
process occurring on the phosphorescent surface, not by time needed for
the rays to arrive there. Hence his value for the velocity was again far
too small and the mass:charge ratio was too large.
	In his paper of October 1897, Thomson admits that these previous
measurements of the velocity were useless, and he describes two better
methods. Both methods use Schuster's experiment to measure mv/e using the
deflection in a magnetic field, as described above. The methods differ in
how they obtain from this the velocity v and mass:charge ratio m/e.
	In the first method, he measures the electric current carried by
the rays. This quantity I is given by
		 I = ne
where n is the number of particles passing along the rays per second. He
then made use of another well-known property of cathode rays, that they
heat up any surface they strike. Assuming that the particles stop dead
when they strike the surface, Thomson reasoned that the kinetic energy
carried by the particles per second would be equal to the heat W given to
to the surface per second. That is,
                   1    2
		W = - nmv
		    2
                     2
	Thus,  2W   mv
	       -- = ---
		I    e
	Dividing this quantity by mv/e, which he already knew, would give
the velocity v and hence the mass:charge ratio. Thomson measured the rate
of heating, W, using a thermocouple, and the current I by collecting the
rays in a cylinder connected to an electrometer as in Perrin's experiment.
The resulting values of m/e and v are tabulated in his paper in the
Philosophical Magazine, October 1897. The values of m/e vary through a
factor of about three between the different readings, though they are all
less than a thousanth of the value for the hydrogen ion (proton). This
seemed a very surprising, and perhaps suspicious result, since no particle
was thought to exist with such a small mass:charge ratio.
00000000  81 2e 2e 2e 2e 2e 2e 2e  2e 2e 2a 2e 2e 2e 2e 2e  |..........*.....|
00000010  2e 2e 2a 2e 2e 2e 2e 2e  2e 2e 2a 2e 2e 2e 2e 2e  |..*.......*.....|
*
00000040  2e 2e 2a 2e 2e 2e 2e 2e  2e 2e 2a 2e 3c 0d 09 54  |..*.......*.<..T|
00000050  68 69 73 20 73 74 69 6c  6c 20 6c 65 66 74 20 74  |his still left t|
00000060  68 65 20 64 69 66 66 69  63 75 6c 74 79 20 74 68  |he difficulty th|
00000070  61 74 20 48 65 72 74 7a  20 68 61 64 20 66 61 69  |at Hertz had fai|
00000080  6c 65 64 20 74 6f 20 64  65 66 6c 65 63 74 20 74  |led to deflect t|
00000090  68 65 0d 63 61 74 68 6f  64 65 20 72 61 79 73 20  |he.cathode rays |
000000a0  62 79 20 61 70 70 6c 79  69 6e 67 20 61 6e 1a 20  |by applying an. |
000000b0  65 6c 65 63 74 72 69 63  1a 20 66 69 65 6c 64 2e  |electric. field.|
000000c0  20 54 68 6f 6d 73 6f 6e  20 77 61 73 20 73 75 73  | Thomson was sus|
000000d0  70 69 63 69 6f 75 73 20  61 62 6f 75 74 0d 74 68  |picious about.th|
000000e0  69 73 20 72 65 73 75 6c  74 2c 20 66 6f 72 20 68  |is result, for h|
000000f0  65 20 6b 6e 65 77 20 6f  66 20 74 77 6f 20 70 72  |e knew of two pr|
00000100  65 76 69 6f 75 73 20 65  78 70 65 72 69 6d 65 6e  |evious experimen|
00000110  74 73 20 69 6e 20 77 68  69 63 68 20 74 68 65 20  |ts in which the |
00000120  72 61 79 73 20 68 61 64  0d 61 70 70 61 72 65 6e  |rays had.apparen|
00000130  74 6c 79 1a 20 62 65 65  6e 1a 20 64 65 66 6c 65  |tly. been. defle|
00000140  63 74 65 64 1a 20 62 79  1a 20 65 6c 65 63 74 72  |cted. by. electr|
00000150  69 63 1a 20 66 69 65 6c  64 73 2e 20 54 68 65 73  |ic. fields. Thes|
00000160  65 1a 20 65 78 70 65 72  69 6d 65 6e 74 73 2c 1a  |e. experiments,.|
00000170  20 62 79 0d 43 72 6f 6f  6b 65 73 1a 20 61 6e 64  | by.Crookes. and|
00000180  1a 20 47 6f 6c 64 73 74  65 69 6e 1a 20 69 6e 1a  |. Goldstein. in.|
00000190  20 31 38 37 39 20 61 6e  64 1a 20 31 38 38 30 1a  | 1879 and. 1880.|
000001a0  20 72 65 73 70 65 63 74  69 76 65 6c 79 2c 1a 20  | respectively,. |
000001b0  75 73 65 64 1a 20 73 6c  69 67 68 74 6c 79 0d 64  |used. slightly.d|
000001c0  69 66 66 65 72 65 6e 74  20 61 70 70 61 72 61 74  |ifferent apparat|
000001d0  75 73 2c 20 62 75 74 20  74 68 65 20 70 72 69 6e  |us, but the prin|
000001e0  63 69 70 6c 65 1a 20 77  61 73 1a 20 74 68 65 1a  |ciple. was. the.|
000001f0  20 73 61 6d 65 2e 1a 20  54 77 6f 20 63 61 74 68  | same.. Two cath|
00000200  6f 64 65 73 20 77 65 72  65 0d 70 6c 61 63 65 64  |odes were.placed|
00000210  20 69 6e 20 74 68 65 20  76 61 63 75 75 6d 20 74  | in the vacuum t|
00000220  75 62 65 2c 20 61 6e 64  20 77 69 72 65 64 20 73  |ube, and wired s|
00000230  6f 20 74 68 65 79 1a 20  63 6f 75 6c 64 1a 20 62  |o they. could. b|
00000240  65 20 73 77 69 74 63 68  65 64 20 6f 6e 20 6f 72  |e switched on or|
00000250  20 6f 66 66 0d 69 6e 64  65 70 65 6e 64 65 6e 74  | off.independent|
00000260  6c 79 2e 20 57 69 74 68  20 6f 6e 6c 79 20 6f 6e  |ly. With only on|
00000270  65 20 63 61 74 68 6f 64  65 20 61 63 74 69 76 65  |e cathode active|
00000280  2c 20 74 68 65 20 72 61  79 73 20 70 61 73 73 65  |, the rays passe|
00000290  64 20 69 6e 20 61 20 73  74 72 61 69 67 68 74 0d  |d in a straight.|
000002a0  6c 69 6e 65 20 61 73 20  75 73 75 61 6c 2c 20 62  |line as usual, b|
000002b0  75 74 20 77 68 65 6e 20  74 68 65 20 73 65 63 6f  |ut when the seco|
000002c0  6e 64 20 77 61 73 20 73  77 69 63 68 65 64 20 6f  |nd was swiched o|
000002d0  6e 2c 20 74 68 65 20 74  77 6f 20 73 74 72 65 61  |n, the two strea|
000002e0  6d 73 20 6f 66 20 72 61  79 73 0d 63 75 72 76 65  |ms of rays.curve|
000002f0  64 20 61 77 61 79 20 66  72 6f 6d 20 65 61 63 68  |d away from each|
00000300  20 6f 74 68 65 72 2e 20  43 72 6f 6f 6b 65 73 20  | other. Crookes |
00000310  73 61 69 64 20 74 68 69  73 20 73 68 6f 77 65 64  |said this showed|
00000320  20 74 68 61 74 20 74 68  65 1a 20 72 61 79 73 1a  | that the. rays.|
00000330  20 77 65 72 65 0d 6e 65  67 61 74 69 76 65 6c 79  | were.negatively|
00000340  1a 20 63 68 61 72 67 65  64 1a 20 70 61 72 74 69  |. charged. parti|
00000350  63 6c 65 73 2c 1a 20 77  68 69 63 68 20 72 65 70  |cles,. which rep|
00000360  65 6c 6c 65 64 20 65 61  63 68 20 6f 74 68 65 72  |elled each other|
00000370  20 61 6e 64 20 64 69 76  65 72 67 65 64 20 61 73  | and diverged as|
00000380  0d 74 68 65 79 20 6d 6f  76 65 64 20 61 77 61 79  |.they moved away|
00000390  20 66 72 6f 6d 1a 20 74  68 65 1a 20 63 61 74 68  | from. the. cath|
000003a0  6f 64 65 73 2e 1a 20 54  68 69 73 1a 20 65 78 70  |odes.. This. exp|
000003b0  6c 61 6e 61 74 69 6f 6e  1a 20 77 61 73 1a 20 64  |lanation. was. d|
000003c0  69 73 70 72 6f 76 65 64  20 62 79 0d 57 69 65 64  |isproved by.Wied|
000003d0  65 6d 61 6e 6e 20 61 6e  64 20 45 62 65 72 74 20  |emann and Ebert |
000003e0  69 6e 20 31 38 39 31 2c  20 77 68 6f 20 73 68 6f  |in 1891, who sho|
000003f0  77 65 64 20 74 68 61 74  20 74 68 65 20 64 65 66  |wed that the def|
00000400  6c 65 63 74 69 6f 6e 20  69 73 20 69 6e 20 66 61  |lection is in fa|
00000410  63 74 20 64 75 65 0d 74  6f 20 74 68 65 20 69 6e  |ct due.to the in|
00000420  74 65 6e 73 65 20 65 6c  65 63 74 72 69 63 20 66  |tense electric f|
00000430  69 65 6c 64 1a 20 73 75  72 72 6f 75 6e 64 69 6e  |ield. surroundin|
00000440  67 20 74 68 65 20 6f 74  68 65 72 20 63 61 74 68  |g the other cath|
00000450  6f 64 65 2c 20 6e 6f 74  20 74 68 65 20 72 61 79  |ode, not the ray|
00000460  73 0d 65 6d 61 6e 61 74  69 6e 67 20 66 72 6f 6d  |s.emanating from|
00000470  20 69 74 2e 20 4f 6e 63  65 20 61 67 61 69 6e 2c  | it. Once again,|
00000480  20 43 72 6f 6f 6b 65 73  1a 20 68 61 64 1a 20 63  | Crookes. had. c|
00000490  6f 6d 65 1a 20 74 6f 20  74 68 65 20 72 69 67 68  |ome. to the righ|
000004a0  74 20 63 6f 6e 63 6c 75  73 69 6f 6e 0d 66 6f 72  |t conclusion.for|
000004b0  1a 20 74 68 65 20 77 72  6f 6e 67 20 72 65 61 73  |. the wrong reas|
000004c0  6f 6e 73 21 20 0d 09 54  68 69 73 20 65 78 70 65  |ons! ..This expe|
000004d0  72 69 6d 65 6e 74 20 61  6c 73 6f 20 65 78 70 6c  |riment also expl|
000004e0  61 69 6e 65 64 20 77 68  79 1a 20 63 61 74 68 6f  |ained why. catho|
000004f0  64 65 20 72 61 79 73 20  61 72 65 20 61 6c 77 61  |de rays are alwa|
00000500  79 73 20 65 6d 69 74 74  65 64 0d 6e 6f 72 6d 61  |ys emitted.norma|
00000510  6c 6c 79 20 66 72 6f 6d  20 74 68 65 20 73 75 72  |lly from the sur|
00000520  66 61 63 65 20 6f 66 20  74 68 65 1a 20 63 61 74  |face of the. cat|
00000530  68 6f 64 65 2e 1a 20 54  68 65 20 65 6c 65 63 74  |hode.. The elect|
00000540  72 69 63 20 66 69 65 6c  64 20 6e 65 78 74 20 74  |ric field next t|
00000550  6f 20 61 6e 79 0d 70 65  72 66 65 63 74 20 63 6f  |o any.perfect co|
00000560  6e 64 75 63 74 6f 72 20  69 73 20 61 6c 77 61 79  |nductor is alway|
00000570  73 20 70 65 72 70 65 6e  64 69 63 75 6c 61 72 20  |s perpendicular |
00000580  74 6f 20 69 74 73 20 73  75 72 66 61 63 65 2c 1a  |to its surface,.|
00000590  20 61 6e 64 1a 20 69 74  20 69 73 20 74 68 69 73  | and. it is this|
000005a0  0d 66 69 65 6c 64 20 74  68 61 74 20 61 63 63 65  |.field that acce|
000005b0  6c 65 72 61 74 65 73 20  74 68 65 20 72 61 79 73  |lerates the rays|
000005c0  20 61 77 61 79 20 66 72  6f 6d 20 74 68 65 20 63  | away from the c|
000005d0  61 74 68 6f 64 65 2e 20  48 65 6e 63 65 1a 20 74  |athode. Hence. t|
000005e0  68 65 20 72 61 79 73 20  61 72 65 0d 69 6e 69 74  |he rays are.init|
000005f0  69 61 6c 6c 79 1a 20 61  63 63 65 6c 65 72 61 74  |ially. accelerat|
00000600  65 64 1a 20 61 74 1a 20  72 69 67 68 74 1a 20 61  |ed. at. right. a|
00000610  6e 67 6c 65 73 20 66 72  6f 6d 20 74 68 65 20 63  |ngles from the c|
00000620  61 74 68 6f 64 65 2c 20  74 68 65 6e 20 64 65 66  |athode, then def|
00000630  6c 65 63 74 65 64 0d 61  63 63 6f 72 64 69 6e 67  |lected.according|
00000640  20 62 79 20 74 68 65 20  73 68 61 70 65 20 6f 66  | by the shape of|
00000650  20 74 68 65 20 63 61 74  68 6f 64 65 20 6f 72 20  | the cathode or |
00000660  61 6e 79 20 6f 74 68 65  72 20 65 6c 65 63 74 72  |any other electr|
00000670  6f 64 65 73 20 6e 65 61  72 62 79 2e 0d 09 20 54  |odes nearby... T|
00000680  68 6f 6d 73 6f 6e 1a 20  72 65 70 65 61 74 65 64  |homson. repeated|
00000690  1a 20 48 65 72 74 7a 27  73 20 65 78 70 65 72 69  |. Hertz's experi|
000006a0  6d 65 6e 74 20 74 6f 1a  20 64 65 66 6c 65 63 74  |ment to. deflect|
000006b0  1a 20 74 68 65 1a 20 72  61 79 73 2c 1a 20 61 6e  |. the. rays,. an|
000006c0  64 0d 6f 62 74 61 69 6e  65 64 20 74 68 65 20 73  |d.obtained the s|
000006d0  61 6d 65 1a 20 72 65 73  75 6c 74 1a 20 2d 20 74  |ame. result. - t|
000006e0  68 65 20 65 6c 65 63 74  72 69 63 20 66 69 65 6c  |he electric fiel|
000006f0  64 20 62 65 74 77 65 65  6e 20 74 68 65 20 70 6c  |d between the pl|
00000700  61 74 65 73 20 64 69 64  20 6e 6f 74 0d 61 70 70  |ates did not.app|
00000710  65 61 72 20 74 6f 20 6d  61 6b 65 20 61 6e 79 20  |ear to make any |
00000720  64 69 66 66 65 72 65 6e  63 65 1a 20 74 6f 1a 20  |difference. to. |
00000730  74 68 65 1a 20 70 61 74  68 20 6f 66 20 74 68 65  |the. path of the|
00000740  20 72 61 79 73 2c 20 68  6f 77 65 76 65 72 20 6c  | rays, however l|
00000750  61 72 67 65 20 68 65 0d  6d 61 64 65 20 74 68 65  |arge he.made the|
00000760  20 76 6f 6c 74 61 67 65  20 62 65 74 77 65 65 6e  | voltage between|
00000770  20 74 68 65 20 70 6c 61  74 65 73 2e 20 54 68 65  | the plates. The|
00000780  20 73 6f 6c 75 74 69 6f  6e 1a 20 74 6f 1a 20 74  | solution. to. t|
00000790  68 69 73 1a 20 70 72 6f  62 6c 65 6d 1a 20 63 61  |his. problem. ca|
000007a0  6d 65 0d 66 72 6f 6d 1a  20 4c 65 6e 61 72 64 27  |me.from. Lenard'|
000007b0  73 1a 20 6f 6c 64 1a 20  6f 62 73 65 72 76 61 69  |s. old. observai|
000007c0  6f 6e 1a 20 74 68 61 74  20 63 61 74 68 6f 64 65  |on. that cathode|
000007d0  20 72 61 79 73 20 69 6e  63 72 65 61 73 65 20 74  | rays increase t|
000007e0  68 65 20 65 6c 65 63 74  72 69 63 61 6c 0d 63 6f  |he electrical.co|
000007f0  6e 64 75 63 74 69 76 69  74 79 20 6f 66 20 61 6e  |nductivity of an|
00000800  79 20 67 61 73 20 77 68  69 63 68 1a 20 74 68 65  |y gas which. the|
00000810  79 1a 20 70 61 73 73 20  74 68 72 6f 75 67 68 2e  |y. pass through.|
00000820  20 54 68 6f 6d 73 6f 6e  20 72 65 6c 61 74 65 64  | Thomson related|
00000830  20 74 68 69 73 20 74 6f  0d 68 69 73 20 6f 77 6e  | this to.his own|
00000840  20 65 78 70 65 72 69 6d  65 6e 74 73 20 6f 6e 20  | experiments on |
00000850  67 61 73 65 73 20 69 6f  6e 69 73 65 64 20 62 79  |gases ionised by|
00000860  20 58 2d 72 61 79 73 2c  20 61 6e 64 20 63 6f 6e  | X-rays, and con|
00000870  63 6c 75 64 65 64 20 74  68 61 74 20 63 61 74 68  |cluded that cath|
00000880  6f 64 65 0d 72 61 79 73  20 74 6f 6f 20 6d 75 73  |ode.rays too mus|
00000890  74 20 67 65 6e 65 72 61  74 65 20 63 68 61 72 67  |t generate charg|
000008a0  65 64 20 67 61 73 20 6d  6f 6c 65 63 75 6c 65 73  |ed gas molecules|
000008b0  2e 1a 20 49 66 20 61 6e  20 65 6c 65 63 74 72 69  |.. If an electri|
000008c0  63 20 66 69 65 6c 64 20  69 73 20 73 65 74 0d 75  |c field is set.u|
000008d0  70 20 69 6e 20 61 20 67  61 73 20 63 6f 6e 74 61  |p in a gas conta|
000008e0  69 6e 69 6e 67 1a 20 69  6f 6e 73 2c 1a 20 74 68  |ining. ions,. th|
000008f0  65 1a 20 6e 65 67 61 74  69 76 65 1a 20 69 6f 6e  |e. negative. ion|
00000900  73 1a 20 77 69 6c 6c 1a  20 6d 6f 76 65 20 74 6f  |s. will. move to|
00000910  77 61 72 64 73 20 74 68  65 0d 70 6f 73 69 74 69  |wards the.positi|
00000920  76 65 1a 20 70 6c 61 74  65 1a 20 61 6e 64 1a 20  |ve. plate. and. |
00000930  74 68 65 1a 20 70 6f 73  69 74 69 76 65 1a 20 69  |the. positive. i|
00000940  6f 6e 73 20 74 6f 20 74  68 65 20 6e 65 67 61 74  |ons to the negat|
00000950  69 76 65 20 70 6c 61 74  65 2e 20 54 68 69 73 20  |ive plate. This |
00000960  77 69 6c 6c 0d 63 6f 6e  74 69 6e 75 65 20 75 6e  |will.continue un|
00000970  74 69 6c 20 65 6e 6f 75  67 68 20 69 6f 6e 73 20  |til enough ions |
00000980  68 61 76 65 20 62 75 69  6c 74 1a 20 75 70 1a 20  |have built. up. |
00000990  6e 65 61 72 1a 20 74 68  65 20 70 6c 61 74 65 73  |near. the plates|
000009a0  20 74 6f 20 62 61 6c 61  6e 63 65 20 6f 75 74 0d  | to balance out.|
000009b0  74 68 65 20 65 6c 65 63  74 72 69 63 20 66 69 65  |the electric fie|
000009c0  6c 64 20 64 75 65 20 74  6f 20 74 68 65 20 70 6c  |ld due to the pl|
000009d0  61 74 65 73 20 74 68 65  6d 73 65 6c 76 65 73 2e  |ates themselves.|
000009e0  20 4f 66 1a 20 63 6f 75  72 73 65 20 73 6f 6d 65  | Of. course some|
000009f0  20 69 6f 6e 73 20 77 69  6c 6c 0d 62 65 20 64 69  | ions will.be di|
00000a00  73 63 68 61 72 67 65 64  20 62 79 20 63 6f 6c 6c  |scharged by coll|
00000a10  69 73 69 6f 6e 73 20 77  69 74 68 20 74 68 65 20  |isions with the |
00000a20  70 6c 61 74 65 73 2c 20  62 75 74 20 74 68 69 73  |plates, but this|
00000a30  20 77 69 6c 6c 1a 20 6e  6f 74 20 6f 63 63 75 72  | will. not occur|
00000a40  20 66 61 73 74 0d 65 6e  6f 75 67 68 1a 20 74 6f  | fast.enough. to|
00000a50  1a 20 70 72 65 76 65 6e  74 1a 20 61 20 6c 61 79  |. prevent. a lay|
00000a60  65 72 20 6f 66 20 63 68  61 72 67 65 64 20 67 61  |er of charged ga|
00000a70  73 20 62 75 69 6c 64 69  6e 67 20 75 70 20 6e 65  |s building up ne|
00000a80  61 72 1a 20 74 68 65 1a  20 70 6c 61 74 65 73 2e  |ar. the. plates.|
00000a90  0d 48 65 6e 63 65 20 61  66 74 65 72 20 61 20 73  |.Hence after a s|
00000aa0  68 6f 72 74 1a 20 74 69  6d 65 1a 20 74 68 65 20  |hort. time. the |
00000ab0  66 69 65 6c 64 20 64 75  65 20 74 6f 20 74 68 65  |field due to the|
00000ac0  20 70 6c 61 74 65 73 20  77 69 6c 6c 20 6e 6f 74  | plates will not|
00000ad0  20 62 65 20 66 65 6c 74  20 61 74 0d 61 6c 6c 20  | be felt at.all |
00000ae0  62 79 20 74 68 65 20 63  61 74 68 6f 64 65 20 72  |by the cathode r|
00000af0  61 79 73 2c 20 61 6e 64  20 74 68 65 79 20 77 69  |ays, and they wi|
00000b00  6c 6c 20 6e 6f 74 20 73  68 6f 77 20 61 6e 79 20  |ll not show any |
00000b10  64 65 66 6c 65 63 74 69  6f 6e 2e 20 0d 09 54 6f  |deflection. ..To|
00000b20  20 61 76 6f 69 64 20 74  68 69 73 20 70 72 6f 62  | avoid this prob|
00000b30  6c 65 6d 2c 20 74 68 65  1a 20 6f 62 76 69 6f 75  |lem, the. obviou|
00000b40  73 1a 20 73 6f 6c 75 74  69 6f 6e 1a 20 77 61 73  |s. solution. was|
00000b50  20 74 6f 20 70 75 6d 70  20 61 77 61 79 20 74 68  | to pump away th|
00000b60  65 0d 67 61 73 20 73 6f  20 74 68 65 72 65 20 61  |e.gas so there a|
00000b70  72 65 20 6e 6f 20 69 6f  6e 73 20 74 6f 20 62 75  |re no ions to bu|
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00001980  74 68 65 1a 20 73 75 72  66 61 63 65 2c 1a 20 54  |the. surface,. T|
00001990  68 6f 6d 73 6f 6e 1a 20  72 65 61 73 6f 6e 65 64  |homson. reasoned|
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000019f0  74 68 65 20 68 65 61 74  20 57 20 67 69 76 65 6e  |the heat W given|
00001a00  20 74 6f 0d 74 6f 20 74  68 65 20 73 75 72 66 61  | to.to the surfa|
00001a10  63 65 20 70 65 72 20 73  65 63 6f 6e 64 2e 20 54  |ce per second. T|
00001a20  68 61 74 20 69 73 2c 0d  20 20 20 20 20 20 20 20  |hat is,.        |
00001a30  20 20 20 20 20 20 20 20  20 20 20 31 20 20 20 20  |           1    |
00001a40  32 0d 09 09 57 20 3d 20  2d 20 6e 6d 76 0d 09 09  |2...W = - nmv...|
00001a50  20 20 20 20 32 0d 20 20  20 20 20 20 20 20 20 20  |    2.          |
00001a60  20 20 20 20 20 20 20 20  20 20 20 32 0d 09 54 68  |           2..Th|
00001a70  75 73 2c 20 20 32 57 20  20 20 6d 76 0d 09 20 20  |us,  2W   mv..  |
00001a80  20 20 20 20 20 2d 2d 20  3d 20 2d 2d 2d 0d 09 09  |     -- = ---...|
00001a90  49 20 20 20 20 65 0d 09  44 69 76 69 64 69 6e 67  |I    e..Dividing|
00001aa0  20 74 68 69 73 20 71 75  61 6e 74 69 74 79 20 62  | this quantity b|
00001ab0  79 20 6d 76 2f 65 2c 1a  20 77 68 69 63 68 1a 20  |y mv/e,. which. |
00001ac0  68 65 20 61 6c 72 65 61  64 79 20 6b 6e 65 77 2c  |he already knew,|
00001ad0  20 77 6f 75 6c 64 20 67  69 76 65 0d 74 68 65 20  | would give.the |
00001ae0  76 65 6c 6f 63 69 74 79  20 76 20 61 6e 64 20 68  |velocity v and h|
00001af0  65 6e 63 65 20 74 68 65  20 6d 61 73 73 3a 63 68  |ence the mass:ch|
00001b00  61 72 67 65 1a 20 72 61  74 69 6f 2e 20 54 68 6f  |arge. ratio. Tho|
00001b10  6d 73 6f 6e 20 6d 65 61  73 75 72 65 64 20 74 68  |mson measured th|
00001b20  65 20 72 61 74 65 0d 6f  66 20 68 65 61 74 69 6e  |e rate.of heatin|
00001b30  67 2c 20 57 2c 20 75 73  69 6e 67 20 61 20 74 68  |g, W, using a th|
00001b40  65 72 6d 6f 63 6f 75 70  6c 65 2c 20 61 6e 64 20  |ermocouple, and |
00001b50  74 68 65 1a 20 63 75 72  72 65 6e 74 1a 20 49 20  |the. current. I |
00001b60  62 79 20 63 6f 6c 6c 65  63 74 69 6e 67 20 74 68  |by collecting th|
00001b70  65 0d 72 61 79 73 20 69  6e 20 61 20 63 79 6c 69  |e.rays in a cyli|
00001b80  6e 64 65 72 20 63 6f 6e  6e 65 63 74 65 64 20 74  |nder connected t|
00001b90  6f 20 61 6e 20 65 6c 65  63 74 72 6f 6d 65 74 65  |o an electromete|
00001ba0  72 20 61 73 20 69 6e 20  50 65 72 72 69 6e 27 73  |r as in Perrin's|
00001bb0  20 65 78 70 65 72 69 6d  65 6e 74 2e 0d 54 68 65  | experiment..The|
00001bc0  1a 20 72 65 73 75 6c 74  69 6e 67 1a 20 76 61 6c  |. resulting. val|
00001bd0  75 65 73 1a 20 6f 66 20  6d 2f 65 20 61 6e 64 20  |ues. of m/e and |
00001be0  76 20 61 72 65 20 74 61  62 75 6c 61 74 65 64 20  |v are tabulated |
00001bf0  69 6e 1a 20 68 69 73 1a  20 70 61 70 65 72 1a 20  |in. his. paper. |
00001c00  69 6e 1a 20 74 68 65 0d  50 68 69 6c 6f 73 6f 70  |in. the.Philosop|
00001c10  68 69 63 61 6c 20 4d 61  67 61 7a 69 6e 65 2c 20  |hical Magazine, |
00001c20  4f 63 74 6f 62 65 72 20  31 38 39 37 2e 1a 20 54  |October 1897.. T|
00001c30  68 65 1a 20 76 61 6c 75  65 73 1a 20 6f 66 1a 20  |he. values. of. |
00001c40  6d 2f 65 20 76 61 72 79  20 74 68 72 6f 75 67 68  |m/e vary through|
00001c50  20 61 0d 66 61 63 74 6f  72 20 6f 66 20 61 62 6f  | a.factor of abo|
00001c60  75 74 20 74 68 72 65 65  20 62 65 74 77 65 65 6e  |ut three between|
00001c70  1a 20 74 68 65 20 64 69  66 66 65 72 65 6e 74 20  |. the different |
00001c80  72 65 61 64 69 6e 67 73  2c 20 74 68 6f 75 67 68  |readings, though|
00001c90  20 74 68 65 79 20 61 72  65 20 61 6c 6c 0d 6c 65  | they are all.le|
00001ca0  73 73 20 74 68 61 6e 20  61 20 74 68 6f 75 73 61  |ss than a thousa|
00001cb0  6e 74 68 20 6f 66 20 74  68 65 1a 20 76 61 6c 75  |nth of the. valu|
00001cc0  65 1a 20 66 6f 72 1a 20  74 68 65 1a 20 68 79 64  |e. for. the. hyd|
00001cd0  72 6f 67 65 6e 20 69 6f  6e 20 28 70 72 6f 74 6f  |rogen ion (proto|
00001ce0  6e 29 2e 20 54 68 69 73  0d 73 65 65 6d 65 64 20  |n). This.seemed |
00001cf0  61 20 76 65 72 79 20 73  75 72 70 72 69 73 69 6e  |a very surprisin|
00001d00  67 2c 20 61 6e 64 20 70  65 72 68 61 70 73 20 73  |g, and perhaps s|
00001d10  75 73 70 69 63 69 6f 75  73 20 72 65 73 75 6c 74  |uspicious result|
00001d20  2c 20 73 69 6e 63 65 20  6e 6f 20 70 61 72 74 69  |, since no parti|
00001d30  63 6c 65 0d 77 61 73 20  74 68 6f 75 67 68 74 20  |cle.was thought |
00001d40  74 6f 20 65 78 69 73 74  20 77 69 74 68 20 73 75  |to exist with su|
00001d50  63 68 20 61 20 73 6d 61  6c 6c 20 6d 61 73 73 3a  |ch a small mass:|
00001d60  63 68 61 72 67 65 20 72  61 74 69 6f 2e 0d        |charge ratio..|
00001d6e
EltronBKP/ElectronC.m0
EltronBKP/ElectronC.m1
EltronBKP/ElectronC.m2
EltronBKP/ElectronC.m4
EltronBKP/ElectronC.m5