EXTRA NOTES FOR IGCSE PHYSICS. Calculate the orbital speed of the Earth around the Sun. (Earth orbital radius = 150 million km)

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EXTRA NOTES FOR IGCSE PHYSICS #1.33 use the relationship between orbital speed, orbital radius and time period: orbital speed = 2 π orbital radius time period or v = 2 π r T Example 1: Calculate the orbital speed of the Earth around the Sun. (Earth orbital radius = 150 million km) Using v = (2π x r ) T = (2π x [150 000 000 km] ) but 1 km = 1000 m and 1 year = 365x24x60x60 = 3153600 seconds [1 year] = (2π x [150 000 000 000 m] ) 31 536 000 sec Answer: orbital speed = 29 900 m/s Example 2: Calculate the orbital speed of the Moon around the Earth. (Moon orbital radius = 380 000 km; orbit time = 27.3 days) Using v = (2π x r ) T = (2π x [380 000 km] ) but 1 km = 1000 m and 1 day = 24x60x60 = 86400 seconds [27.3 days] = (2π x [380 000 000 m] ) 2358720 sec Answer: orbital speed = 1 012 m/s Example 3: Calculate the orbital speed of the ISS (International Space Station) around the Earth. (ISS orbital height = 355 km; orbit time = 91 minutes; Earth radius = 6 378 km) The orbit radius of the ISS = (355 + 6 378) km = 6 733 km Using v = (2π x r ) T = (2π x [6 733 km] ) = (2π x [6 733 000 m] ) = Answer: orbital speed = 7748 m/s [91 minutes] (91x60 seconds)

#2.16 understand that electrical current is the rate of flow of charge. From Q = I t current I (A )= Charge Q (C) time t (s) From this equation it can be concluded that: Current is the rate of flow of charge. (rate means time) 1 Amp = 1 Coulomb per second. #2.19 recall that: voltage is the energy transferred per unit charge passed the volt is a joule per coulomb From E = QV Voltage V (V )= Energy E (J). Charge Q (C) From this equation it can be concluded that: Voltage is energy per unit charge 1 Volt = 1 Joule per Coulomb. #3.14 recall that light waves are transverse waves which can be not just reflected and refracted but also diffracted. Light rays can be reflected using a mirror, refracted (bent) when they change medium but just like water waves, they can be diffracted (spread) if they pass through a extremely narrow slit (gap) that is similar to their wavelength. #3.18 recall and use the relationship between refractive index, angle of incidence and angle of refraction: η = sin i sin r Refractive index η = sin i / sin r where: i is the angle of incidence and r is the angle of refraction A beam of light hits a glass block. The angle of incidence angle of incidence is 55. The angle of refraction inside the block is 33. Calculate the refractive index. A ray of light passing from the air into glass, showing the incident ray (in the air) and the refracted ray (in the glass).

Step 1: Work out the sine of angle i sin 55 = 0.819 Step 2: Work out the sine of angle r sin 33 = 0.545 Step 3: Divide sin i by sin r refractive index = sin i sin r refractive index = 0.819 0.545 = 1.5 #3.19 describe an experiment to determine the refractive index of glass, using a glass block. Shine a ray of light through a glass block and using a protractor measure the angle of incidence and the angle of refraction. Using the formula η = sin i / sin r you will calculate the refractive index of glass. #3.22 recall and use the relationship between critical angle and refractive index: η = 1 sin c Given that the critical angle of glass is 42 0, calculate its refractive index. η = 1 = 1 = 1 = 1.5 sin c sin 42 0.669 #3.23 understand the difference between analogue and digital signals Communication signals can be analogue or digital. Analogue signals Music and speech vary continuously in frequency and amplitude. In the same way, analogue signals can vary in frequency, amplitude, or both. Analogue signals include FM radio and AM radio - Frequency Modulated radio and Amplitude Modulated radio. The diagram shows a typical oscilloscope trace of an analogue signal. Oscilloscope trace of an analogue signal Digital signals Digital signals are a series of pulses consisting of just two states: ON (1) or OFF (0). There are no values in between. DAB radio is Digital Audio Broadcast radio - it is transmitted as digital signals. The diagram shows a typical oscilloscope trace of a digital signal. Oscilloscope trace of a digital signal

#3.24 describe the advantages of using digital signals rather than analogue signals Advantages of digital signals: 1. Digital signals carry more information per second than analogue signals. 2. They are also less prone to interference 3. They can carry more information. _ #3.26 recall that sound waves are longitudinal waves which can be not just reflected ad refracted but also diffracted. When waves meet a gap in a barrier, they carry on through the gap. However, the waves spread out to some extent into the area beyond the gap. This is diffraction. The extent of the spreading depends on the width of the gap compared with the wavelength of the waves. The smaller the width of the gap compared with the wavelength of the wave, the stronger the diffraction. For example, when water waves spread into a harbour, they spread out more if the harbour mouth is narrow. Similarly sound can diffract through a doorway or around buildings. Lower pitched sounds travel better than high-pitched sounds. This is because low-pitched sounds have a long wavelength compared with the width of the gap, so they spread out more. #5.11 understand the significance of Brownian motion What is Brownian Motion? When a smoke particle is observed under a microscope it moved haphazardly as if it is being continuously hit by something. The random motion of particles is called Brownian Motion. The smoke particle (shown as a blue ball) has a jerky motion. As invisible air molecules collide with the smoke particle, they push it about in different directions at random. Brownian motion shows that matter is made up of very small particles that are in constant motion. #5.13 understand that there is an absolute zero of temperature which is 273 0 C The lowest temperature in the Universe is 273 0 C. It is called absolute zero and at this temperture atoms stop vibrating and have no kinetic energy. _

#5.14 describe the Kelvin scale of temperature and be able to convert between the Kelvin and Celsius scales To change from Celsius to Kelvin... add 273 +273 0 C -----------> K E.g. E.g. 2 0 C = 2 + 273 = 275 K 10 0 C = 10 + 273 = 283 K The Kelvin is the SI unit of temperature. #5.16 understand that the Kelvin temperature of the gas is proportional to the average kinetic energy of its molecules When a gas is heated its temperature rises. This is because the kinetic energy of the particles is increasing. The kinetic energy of the particles is proportional to the temperature of the gas if the temperature is measured using the Kelvin scale. If a gas is cooled the particles lose kinetic energy. There must come a point where they can lose no more kinetic energy as they have none left. This is the minimum temperature that the gas can reach. This temperature is the same for all substances and is called 'absolute zero'. This point is zero kelvin or - 273 degrees celsius. Remember: to convert a celsius temperature to a kelvin temperature you add 273 to convert kelvin temperatures to celsius you subtract 273 an increase in temperature of one kelvin is the same as an increase of one celsius #5.17 describe the qualitative relationship between pressure and Kelvin temperature for a gas in a sealed container #5.18 use the relationship between the pressure and Kelvin temperature of a fixed mass of gas at constant volume: p 1 = p 2 T 1 T 2 Imagine a gas is trapped inside a container which has a fixed size (its volume cannot change). If the gas is heated the particles will gain kinetic energy which will make them move faster. This means they will collide with the walls more frequently. This causes the force on the walls of the container to increase and so the pressure increases. If the temperature of the gas is measured on the kelvin scale we find that the pressure is proportional to the temperature.

From this we can derive the equation Where: is the starting pressure is the starting temperature is the finishing pressure is the finishing temperature All the temperatures are measured on the kelvin scale of temperature. This equation is true as long as the volume and mass of the gas are constant. Worked example: Answer: A car tyre contains air at 1.25 10 5 Pa when at a temperature of 27 C. Once the car has been running for a while the temperature of the air in the tyre rises to 42 C. If the volume of the tyre does not change what is the new pressure of the air in the tyre? First convert the temperatures into kelvin. Now calculate the new pressure Therefore, The new pressure is 1.31 10 5 Pa.

#5.19 use the relationship between the pressure and volume of a fixed mass of gas at constant temperature: p 1 V 1 = p 2 V 2 Pressure and volume of a gas (Boyle's Law) Imagine a gas is trapped in a cylinder by a piston. If the piston is pushed in, the gas particles will have less room to move as the volume the gas occupies has been decreased. Because there has been a decrease in volume the particles will collide more frequently with the walls of the container. Each time they collide with the walls, they exert a force on them. More collisions mean more force, so the pressure will increase. When the volume decreases the pressure increases. This shows that the pressure of a gas is inversely proportional to its volume. From this we can derive the equation: Where: is the starting pressure is the starting volume is the finishing pressure is the finishing volume Worked example: Answer: A sealed syringe contains 10 x10-6 m 3 of air at 1 10 5 Pa. The plunger is pushed until the volume of trapped air is 4 x 10-6 m 3. If there is no change in temperature what is the new pressure of the gas?

Therefore, The new pressure in the syringe is 2.5 10 5 Pa _ #7.7 understand how to complete balanced nuclear equations The nucleus of an atom can be represented as: In this symbol: A is the Nucleon number... also known as Mass number (number of protons + neutrons) Z is the Proton number... also known as Atomic number (number of protons) X is chemical symbol (as shown on the Periodic Table) Alpha decay Two protons and two neutrons are lost from a nucleus when it emits an alpha particle. This means that: The nucleon number decreases by 4 The proton number decreases by 2 A new element is formed!! Example 1: A radon decays into polonium when it emits an alpha particle. Here is the equation for that radioactive decay: Example 2: An isotope of polonium decays to an isotope of lead by emitting an alpha particle.

Beta decay In beta decay, a neutron changes into a proton plus an electron. The proton stays in the nucleus. The electron leaves the atom with high energy as a beta particle. The nucleus has one more proton and one less neutron when it emits a beta particle. This means that: The nucleon number stays the same The proton number increases by 1 Example 1: A carbon-14 is a radioactive isotope of carbon. Here is the equation for the beta decay of carbon-14 into nitrogen: Example 2: An isotope of lead (Pb) decays to an isotope of bismuth (Bi) by emitting a beta particle. #7.10 understand that the activity of a radioactive source decreases over a period of time and is measured in becquerels To get a proper indication of how radioactive something is, the count rate or activity is measured. The activity of a substance is the number of counts or ionisations per second. Activity is measured in units called Becquerels (Bq) named after Henri Becquerel, a French scientist who shared the 1903 Nobel Prize for Physics with his students - Marie and Pierre Curie. Activity = Number of counts / Time taken to measure counts A=N/t where time is in seconds (s) and activity is measured in Becquerels (Bq). Number of counts has no units. Worked example: A pupil measures the background activity in the classroom. The pupil records 45 counts in 60 seconds. What is the background activity in the room? Answer: Number of counts = 45 Time = 60 s A = N/t A = 45/60 A = 0.75 Bq

#7.15 describe the results of Geiger and Marsden s experiments with gold foil and alpha particles #7.16 describe Rutherford s nuclear model of the atom and how it accounts for the results of Geiger and Marsden s experiment and understand the factors (charge and speed) which affect the deflection of alpha particles by a nucleus Rutherford's nuclear atom In 1911 Ernest Rutherford used experimental evidence to show that an atom must contain a central nucleus. In an early model, the atom was imagined as a sphere of positive charge with negatively charged electrons dotted around inside, rather like plums in a pudding. An experiment was carried out in 1905 to support this 'plum pudding' model of the atom but the results were unexpected. Geiger and Marsden's experiment Rutherford designed an experiment to test the plum pudding model. It was carried out by his assistants Geiger and Marsden. A beam of alpha particles was aimed at very thin gold foil and their passage through the foil detected. The scientists expected the alpha particles to pass straight through the foil but something else also happened. Some of the alpha particles emerged from the foil at different angles and some even came straight back. The scientists realised that the positively charged alpha particles were being repelled and deflected by a tiny concentration of positive charge in the atom. As a result of this experiment, the plum pudding model was replaced by the nuclear model of the atom. Because of the results of this experiment, Rutherford showed that: the nucleus of an atom has a relatively small diameter compared with that of the atom most of the mass of the atom is concentrated in the nucleus the nucleus is positively charged The amount of deflection observed during this experiment depended on: the speed of the alpha particles. the charge of the alpha particles. #7.17 understand that a nucleus of U-235 can be split (the process of fission) by collision with a neutron, and that this process releases energy in the form of kinetic energy of the fission products #7.18 recall that the fission of U-235 produces two daughter nuclei and a small number of neutrons #7.19 understand that a chain reaction can be set up if the neutrons produced by one fission strike other U-235 nuclei Nuclear reactors use the heat from nuclear reactions in the nuclear fuel to boil water. Just as in conventional power stations, the steam from the boiling water makes a turbine spin, which in turn makes the generator turn. Unlike conventional power stations, however, nuclear power stations do not release carbon dioxide, so they do not contribute to global warming while in use. Nuclear reactors use a type of nuclear reaction called nuclear fission. Two isotopes in common use as nuclear fuels are uranium-235 and plutonium-239.

Fission: Splitting atoms Fission is another word for splitting. The process of splitting a nucleus is called nuclear fission. Uranium or plutonium isotopes are normally used as the fuel in nuclear reactors, because their atoms have relatively large nuclei that are easy to split, especially when hit by neutrons. When a uranium-235 or plutonium-239 nucleus is hit by a neutron, the following happens: 1. the nucleus splits into two smaller nuclei, which are radioactive 2. two or three more neutrons are released 3. some energy is released The additional neutrons released may also hit other uranium or plutonium nuclei and cause them to split. Even more neutrons are then released, which in turn can split more nuclei. This is called a chain reaction. The chain reaction in nuclear reactors is controlled to stop it going too fast. #7.20 understand the role played by the control rods and moderator when the fission process is used as an energy source to generate electricity. The nuclear reactor is designed to allow a controlled chain reaction to take place. Each time a uranium nucleus splits up it releases energy and three neutrons. If all the neutrons are allowed to be absorbed by other uranium nuclei the chain reaction will spiral out of control causing an explosion. To control the energy released in the reactor moveable control rods are placed between the fuel rods. These control rods are made of boron which absorbs some of the neutrons so fewer neutrons are available to split uranium nuclei. The control rods are raised to increase and lowered to decrease the number of free neutrons.