Waves and Radiation: Nuclear radiation Sample pages Waves and Radiation Nuclear radiation The key concepts discussed in this spread are the nature of alpha radiation (α), beta radiation (β), gamma radiation (γ) and the relative effects of ionisation, absorption and shielding. Types of nuclear radiation Alpha (α) radiation alpha particle Beta (β) radiation + – + 2 neutrons Gamma (γ) radiation beta particle = 1 electron 2 protons gamma ray = energy wave The atoms of radioactive substances emit radiation, and nuclear radiation is emitted from the nucleus (centre) of an atom. Any radiation can be harmful, but it is also very useful when used carefully, so it is important to know exactly how each type of radiation behaves. VIDEO LINK www.youtube.com/watch?fe ature=endscreen&NR=1&v=I jS0bTGCcJQ Absorption and shielding of radiation It is vital to know how far radiation can travel or penetrate before it is absorbed. Then materials can be selected and used to shield humans from the radiation. 3 cm of aluminium Sample pages 20 cm of air Alpha (α) radiation several cm of lead Beta (β) radiation Gamma (γ) radiation A thin sheet of paper can absorb alpha radiation, but gamma radiation can even penetrate several cm of lead. Ionisation ion atom α particle dislodges electron Don’t Forget Although gamma radiation travels the furthest and is the most penetrating radiation, alpha radiation does the most damage over a very short distance because of its strong ionising capability. Ionisation is when nuclear radiation changes atoms into ions. Alpha radiation causes the most ionisation, and happens when an alpha particle collides with an atom and removes an electron from the atom which then becomes an ion (a charged particle). Beta particles cause less ionisation than alpha, they are smaller particles. Gamma radiation causes even less radiation, but because it is a ‘wave’ of energy, it can travel through atoms without being absorbed. Ionisation can be used deliberately for useful reasons: • • • to help diagnose or treat certain illnesses to protect people – for example by its use in smoke detectors in industry – for example to monitor the thickness of newspaper in a paper mill. However, unexpected ionisation can be dangerous, and should be prevented. cont 2 Sample pages α particle Sample pages The three types of nuclear radiation are: Background radiation VIDEO LINK When the atoms of radioactive materials decay, they can give out alpha or beta or gamma radiation. www.youtube.com/ watch?v=Utpi5rFSVe0 Radioactive materials exist everywhere, and so there is always radiation around us, called background radiation. When background radiation is measured, it measures the Activity of a variety of sources in the particular area. The Activity is measured in Becquerels (Bq). Background radiation can be due to natural or artificial radiation. Artificial Source Annual equivalent dose μSv mSv Medical uses (X-rays) 250 0⋅250 Weapons testing 10 0⋅010 Nuclear industry (waste) 2 0⋅002 Other (job, TV, flights) 18 0⋅018 Total man-made sources 280 0⋅280 Natural Source Annual cosmic equivalent dose rays medical mSv radioactive μSv foodgases in airgases Radioactive and 800 0⋅80 buildings (radon and thoron) rocks Rocks of the earth 400 0⋅40 medical other Total natural sources 1870 Absorbed Dose D rocks 1⋅87 Online test E Absorbed Dose D = ––– m http://cloud4test.com/ hello/tests Absorbed Dose is how much energy per kilogram from radiation has been received. It depends on the mass of biological material exposed to the radiation, and the absorbed dose is measured in Grays (Gy). Calculate the absorbed dose. radioactive gases food In food and our bodies 370 0⋅37 weapons other Cosmic rays from spaceindustry 300 0⋅30 nuclear weapons nuclear industry Example: A 2⋅5 kg sample of tissue receives 2mJ of energy. cosmic rays E D= ––– m 2 x 10–3 = –––––––– 2⋅5 =8 x 10–4 Gy (80 mGy) Online test http://cloud4test.com/ hello/tests Equivalent Dose H Equivalent Dose H = DwR The effect of radiation on humans depends on the Absorbed Dose and the type of radiation. Equivalent Dose measures this in Sieverts (Sv). Different types of radiation are given a ‘radiation weighting factor’ (wR) depending on how harmful the effect is on biological material like bone or tissue. Example: A sample of tissue which received an Absorbed Dose of 80 mGy was exposed to alpha radiation. Alpha radiation has a radiation weighting factor of 20. Calculate the Equivalent Dose. H= DwR =8 x 10–4 x 20 =0⋅016 Sv (16 mSv) Don’t Forget THINGS TO DO AND THINK ABOUT There are a variety of tasks that can be carried out either on your own or in a group to explore this topic further. Why not have a go at: • Researching the extraction of naturally occurring radioactive materials and maybe determine levels of background radiation in places near you? • Discuss or debate the risks and benefits of radioactivity in society or the biological effects of radiation in a class environment with one group arguing for and another against. Activity in Bq. Absorbed dose in Gy. Equivalent dose in Sv. 3 Energy and Electricity – Conservation of Energy CONSERVATION OF ENERGY The key concepts to learn in this topic are the principles of ‘conservation’ and ‘loss’ of energy, applied to examples where energy is transferred between stores, the principle of heat energy (Eh) and how to perform calculations with gravitational and elastic potential energy (Ep) and kinetic energy (Ek) in situations involving conservation of energy. VIDEO LINK Energy is never destroyed but is always transformed (changed) into other stores (types) of energy. For example, gravitational potential energy is often transformed into kinetic energy: http://www.youtube. com/watch?v=BSWl_ Zj-CZs&feature=related Potential energy Kinetic energy A bouncing ball dropped on to the ground illustrates how energy is transformed: What happens when the ball is dropped? What happens when the ball stops going up? As the ball falls, if air resistance is ignored then all of the gravitational Ep is transformed into Ek When all of the Ek is transformed back into gravitational Ep the ball will be at the top of its bounce – but not at the height it was dropped from because of the Eh ‘lost’ when it changed shape. Ep ≡ Ek What happens when the ball rebounds? As the ball hits the ground, it changes shape, and the Ek transforms into elastic Ep and some Eh As the ball rebounds, the elastic Ep transforms back into Ek and some Eh and regains its shape. Then this Ek is transformed into gravitational Ep as the ball gets higher. Each time the ball bounces, the lost energy means that the ball will rebound to a lower height until eventually it loses all of its energy. 4 Sample pages What happens when the ball hits the ground? Sample pages Heat energy is usually always produced whenever potential energy is transformed into other stores of energy – whether heat energy is wanted or not. For example, in a car, energy from fuel is transformed by the engine into useful kinetic energy but also into wasted or ‘lost’ heat energy. Sample pages Energy conservation and loss Sample pages Energy and Electricity Energy calculations Online test To calculate gravitational potential energy use Ep = mgh To calculate kinetic energy use Ek = ½mv2 http://cloud4test.com/hello/ tests This example illustrates how to calculate speeds, height and ‘lost’ energy: A 600 g ball is dropped to the ground from a vertical height of 4 metres. (a) Calculate the speed of the ball just as it collides with the ground. Ignore air resistance. Energy is transformed from potential energy into kinetic energy as the ball falls. Ep ≡ Ek mgh= ½mv2 so v= ƒ 2gh = E 2 × 9⋅8 × 4 Don’t Forget Because Ep ≡ Ek ,to calculate the final speed where Ep is transformed into Ek then the equation v = ƒ 2gh can be used to calculate the answer. = 8⋅9 m s–1 (b)When the ball rebounds, it leaves the ground with a speed of 7∙4 m s–1. Calculate the height the ball will return to. v= ƒ 2gh Don’t Forget This rearranges to h= v2 To calculate the final rebound height then the 2g 7⋅42 = 2 × 9⋅8 equation h = v2 can be 2g used to calculate the answer = 2⋅8 m (c) Calculate the energy lost when the ball collides with the ground. Before the collision After the collision Energy lost during the collision Ek = ½mv2 = ½ × 0⋅6 × 8⋅92 = 23⋅76 J Ek = ½mv2 = ½ × 0⋅6 × 7⋅42 = 16⋅4 J = Ek before – Ek after collision = 23⋅76 – 16⋅4 = 7⋅4 J Don’t Forget Good advice: This lost energy is usually transformed into sound and heat. Sometimes this heat energy can cause the ball to become warm in sports where there are lots of ‘rebounds’ e.g. squash and tennis. THINGS TO DO AND THINK ABOUT There are several other examples of everyday energy transformations, e.g. A clock pendulum Water stored in a reservoir which flows downwards through pipes to a generator in a hydro electric power station Think of examples of energy transformations going on around you and consider the energy loss which may occur in these transfers. Discuss and explain why processes are not 100% efficient in terms of useful energy. 5
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