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    To help answer that question, keep the following in mind: PlentyofFish also offers a personality test to better match you with others. Browsing is further customizable by utilizing basic search or advanced search which narrows your parameterssearching by username, or by searching for those looking for the same type of relationship as you. Free Chat and Emails. Communication with other users on PlentyofFish is incredibly simple — you can chat for free, as well as send and receive emails.

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    It goes without saying that you want the picture you post to be one of your best. While technically a free site, PlentyofFish offers you the option to purchase a membership upgrade. PlentyofFish has spun off a new dating site called eVowwhich is only for those seriously looking for a long-term relationship. Examples of the questions include: Which is more important to you, sex or true love?

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    How important is religion in your life? You can set your answers to be publicly available, or you can choose to set all or some to private. By continuing to answer questions, you actively update your profile, which leads to more views. OkCupid also features quizzes created by members, which can help you determine if someone is a match for you — just be aware that some can be rather x-rated.

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    Free Chat and Messaging. Communication is possible via live chatting or messaging someone on the site. In fact, you can search for friends, penpals, people to casually date, to date short-term, or to just hook up with. Also like PlentyofFish, you can upgrade to a paid membership, which provides ad-free browsing, preferential placement in search results, storage of up to 5, messages, and anonymous browsing. Paid Subscription Dating Sites If you have no interest in casual dating and are looking for a more meaningful relationship, you may want to subscribe to a paid site.

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    The element beryllium gave a particularly marked effect of this kind, and later observations by Bothe, by Mme. In Webster s experiments the intensity of the radiation was measured both by means of the Geiger Muller tube counter and in a high pressure ionization chamber.

    He found that the beryllium radiation had an absorption coefficient in lead of about 0 22 cm 1 as measured under his experimental conditions. Making the necessary corrections for these conditions, and using the results of Gray and Tarrant to estimate the relative contributions of scattering, photoelectric absorption, and nuclear absorption in the absorption of such penetrating radiation, Webster concluded that the radiation had a quantum energy of about electron volts.

    No unexpected phenomena were observed though, as well be seen later, similar experiments have now revealed some rather striking events. The failure of these early experiments was partly due the weakness of the available source of polonium, and partly to the experimental arrangement, which as it now appears, was not very suitable.

    Curie Joliot and M. Joliot made the very striking observation that these radiation from berillium and from boron were able to eject protons with considerable velocities from matter containing hydrogen. In their experiments the radiation from beryllium was passed through a thin window into an ionisation vessel containing air at room pressure. When paraffin wax, or other matter containing hydrogen, was placed in front of the window, the ionisation in the vessel was increased, in some cases as much as doubled.

    The effect appeared to be due to the ejection of protons, and from further experiment they showed that the protons had ranges in air up to about 26 cm, corresponding to a velocity of nearly cm per second. They suggested that energy was transferred from the beryllium to the proton by a process similar to the Compton effect with electrons, and they estimated that the beryllium radiation had a quantum energy of about electron volts.

    The range of the protons ejected by the boron radiation was estimated to be about 8 cm in air, giving on a Compton process an energy of about electron volts for the effective quantum. Firstly, it is now well established that the frequency of scattering of high energy quanta by electrons is given with fair accuracy by the Klein Nishina formula, and this formula should also apply to the scattering of quanta by a proton.

    The observed frequency of the proton scattering is, however, many thousand times greater than that predicted by this formula. The mass defect of the C 13 nucleus is known both from data supplied by measurements of the artificial disintegration of boron B 10 and from observations of the band spectrum of 1 Many of the arguments of the subsequent discussion apply equally to both radiations, and the term beryllium radiation may often be taken to include the boron radiation.

    On this assumption it follows that the energy of the quantum emitted in such a reaction cannot be greater than about electron volts. So far as the lighter nuclei are concerned, this assumption is supported by the evidence from experiments on artificial disintegration, but is no general proof. Accordingly, I made further experiments to examine the properties of the radiation excited in beryllium.

    It was found that radiation ejects particles not only from hydrogen but from all other light elements which were examined. The experimental results were very difficult to explain on the hypothesis that the beryllium radiation was a quantum radiation, but followed immediately if it were supposed that the radiation consisted of particles of mass nearly equal to that of a proton and with no net charge, or neutron Briefly, it consists of a small ionisation chamber connected to a valve amplifier.

    The sudden production of ions in the chamber by the entry of an ionising particle is detected by means of an oscillograph connected in the output circuit of the amplifier. The deflections of the oscillograph were recorded photographically on a film of bromide paper.

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    The disc had a diameter of 1 cm and was placed close to a disc of pure beryllium of 2 cm diameter, and both were enclosed in a small vessel which could be evacuated [Fig. The first ionisation chamber used had an opening of 13 mm covered with aluminium foil of 4 5 cm air equivalent, and a depth of 15 3 4 Figure 1: This chamber had a very low natural effect, giving on the average only about 7 deflections per hour. When the source vessel was placed in front of the ionisation chamber, the number of deflections immediately increased.

    For a distance of 3 cm between the beryllium and the counter the number of deflections was nearly 4 per minute. Since the number of deflections remained sensibly the same when thick metal sheets, even as much as 2 cm of lead, were interposed between the source vessel and the counter, it was clear that these deflections were due to penetrating radiation emitted from the beryllium.

    When a sheet of paraffin max about 2 mm thick was interposed in the path of the radiation just in front of the counter, the number of deflections recorded by the oscillograph increased markedly. This increase was due to particles ejected from the paraffin wax so as to pass into the counter. By placing absorbing screens of aluminium between the wax and the counter the absorption curve shown in [Fig.

    From this curve it appears that the particles have a maximum range of just over 40 cm of air, assuming that an Al foil of 1 64 mg.

    By comparing the sizes of the deflections proportional to the number of ions produced in the chamber due to these particles with those due to protons of about the same range it was obvious that the particles were protons. From the range velocity curve for protons we deduce therefore that the maximum velocity imparted to a proton by the beryllium radiation is about cm per second, corresponding to an energy of about electron volts.

    The effect of exposing other elements to the beryllium radiation was 4 5 Figure 2: An ionisation chamber was used with an opening covered with a gold foil of 0 5 mm air equivalent. The element to be examined was fixed on a clean brass plate and placed very close to the counter opening.

    In this way, lithium, beryllium, boron, carbon and nitrogen, as paracyanogen, were tested. In each case the number of deflections observed in the counter increased when the element was bombarded by the beryllium radiation. The ranges of the particles ejected from these elements were quite short, of the order of some millimetres in air. The deflections produced by them were of different sizes, but many of them were large compared with the deflection produced even by a slow proton.

    The particles therefore have a large ionising power and are probably in each case recoil atoms of the elements. Gases were investigated by filling the ionisation chamber with the required gas by circulation for several minutes.

    Hydrogen, helium, nitrogen, oxygen, and argon were examined in this way. Again, in each case deflections were observed which were attributed to the production of recoil atoms in the different gases.

    For a given position of the beryllium source relative to the counter, the number of recoil atoms was roughly the same for each gas. This point will be referred to later. It appears then that the beryllium radiation can impart energy to the atoms of matter through which it passes and that the chance of an energy transfer does not vary widely from one element to another.

    It has shown that protons are ejected from paraffin wax with energies up to a maximum of about electron volts. For example, the nitrogen recoil atoms should have energies up to a maximum ofelectron volts. Taking the energy to form a pair of ions in air as 35 electron volts, the recoil atoms of nitrogen should produce not more than about 13, pairs of ions.

    Many of the deflections observed with nitrogen, however, corresponded to far more ions than this; some of the recoil atoms produced from 30, to 40, ion pairs. In the case of the other elements a similar discrepancy was noted between the observed energies and ranges of the recoil atoms and the values calculated on the assumption that the atoms were set in motion by recoil from a quantum of electron volts.

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    The energies of the recoil atoms were estimated from the number of ions produced in the counter, as given by the size of the oscillograph deflections. A sufficiently good measurement of the ranges could be made either by varying the distance between the element and the counter or by interposing thin screens of gold between the element and the counter.

    The nitrogen recoil atoms were also examined, in collaboration with Dr. Feather, by means of the expansion chamber. The source vessel was placed immediately above an expansion chamber of the Shimizu type, so that a large proportion of the beryllium radiation traversed the chamber. A large number of recoil tracks was observed in the course of a few hours. Their range, estimated by eye, was sometimes as much as 5 or 6 mm, in the chamber, or, correcting for the expansion, about 3 mm in standard air.

    These visual estimates were confirmed by a preliminary series of experiments by Dr. Feather with a large automatic expansion chamber, in which photographs of the recoil tracks in nitrogen were obtained. Now the ranges of recoil atoms of nitrogen of different velocities have been measured by Blackett and Lees.

    Using their results we find that the nitrogen recoil atoms produced by the beryllium radiation may have a velocity of at least cm per second, corresponding to an energy of about electron volts. In order that the nitrogen nucleus should acquire such an energy in a collision with a quantum of radiation, it is necessary to assume that the energy of the quantum should be about electron volts, if energy and momentum are conserved in the collision.

    It has been shown that a quantum of electron volts is sufficient to explain the hydrogen collisions. In general, the experimental results show that if the recoil atoms are to be 6 7 explained by collision with a quantum, we must assume a larger and larger energy for the quantum as the mass of the struck atom increases.

    If we suppose that the radiation is not a quantum radiation, but consists of particles of mass very nearly equal to that of the proton, all the difficulties connected with the collisions disappear, both with regard to their frequency and to the energy transfer to different masses. In order to explain the great penetrating power of the radiation we must further assume that the particle has no get charge. We may suppose it to consist of a proton and an electron in close combination, the neutron discussed by Rutherford in his Bakerian Lecture of When such neutrons pass through matter they suffer occasionally close collisions with the atomic nuclei and so give rise to the recoil atoms which are observed.

    The experiments showed that the maximum velocity of the protons ejected from paraffin wax was about cm per second. From this we can now calculate the maximum energy which can be given by a colliding neutron to other atoms, and we find that the results are in fair agreement with the energies observed in the experiments. Both these values are in good according with experiment.

    It is possible to prove that the mass of the neutron is roughly equal to that of the proton, by combining the evidence from the hydrogen collisions with that the nitrogen collisions. In the succeeding paper, Feather records experiments in which about tracks of nitrogen recoil atoms have been photographed 7 8 in the expansion chamber.

    The measurement of the tracks shown that the maximum range of the recoil atoms is 3 5 mm in air 15 C and mm pressure, corresponding to a velocity of cm per second according to Blackett and Lees. The process is analogous to the well known artificial disintegrations. The energy relations of this process cannot be exactly deduced, for the masses of the Be 9 nucleus and the neutron are not known accurately.

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    It is, however, easy to show that such a process fits the experimental facts. The energy equation becomes n 1 K. The velocity of the neutron must therefore be less than cm per second. We have seen that the actual maximum velocity of the neutron is about cm per second, so that the proposed disintegration process is compatible with observation. The source vessel [Fig. The maximum range of the protons ejected from the wax was determined as before, by counting the numbers of protons observed through different thickness of aluminium interposed between the wax and the counter.

    The absorption curve obtained is shown in curve B, [Fig. The maximum of the protons was about 22 cm in air, corresponding to a velocity of about cm per second.

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    The velocity found in the above experiment should be less than this, for the angle of emission is slightly greater than 90 degrees. The agreement with calculation is as good as can be expected from such measurements.

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    The simplest hypothesis one can make about the nature of the particle is to suppose that it consists of 9 10 a proton and an electron in close combination, giving a net charge 0 and a mass which should be slightly less than the mass of the hydrogen atom.

    This hypothesis is supposed by an examination of the evidence which can be obtained about the mass of the neutron. As we have seen, a rough estimate of the mass of the neutron was obtained from measurements of its collisions with hydrogen and nitrogen atoms, but such measurements cannot be made with sufficient accuracy for the present purpose. We must turn to a consideration of the energy relations in a process in which a neutron is liberated from an atomic nucleus; if the masses of the atomic nuclei concerned in the process are accurately known, a good estimate of the mass of the neutron can be deduced.

    The mass of the beryllium nucleus has, however, not yet been measured, and, as was shown [earlier], only general conclusions can be drawn from this reaction. Fortunately, there remains the case of boron. Further examination showed that this radiation behaves in all respects like that from beryllium, and it must therefore be assumed to consist of neutrons.

    It is probable that the neutrons are emitted from the isotope B 11, for we know that the isotope B 10 disintegrates with the emission of a proton. The masses of B 11 and N 14 are known from Aston s measurements, and the further data required for the deduction of the mass of the neutron can be obtained by experiment.

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