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Cambridge International A-Level Physics

A-Level · Cambridge International (CAIE)Physics26個のフォルダーに48件のノート、282 KB

Cambridge International (CAIE) A-Level Physicsの試験勉強用ノート48件。cookieが作成。コースのトピックに沿った26個のセクションに分かれています。

Notes for Cambridge International AS & A Level Physics (9702), in folders for each of the syllabus's topics in its order, with one note for each sub-topic or group of sub-topics. The AS content (the first eleven topics) comes first and the A Level topics follow, and a last folder covers the practical skills of planning, measuring, graphing and estimating uncertainty. Delete the A Level folders if you take AS only.

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内容

  • Physical quantities and units
    • Quantities, units and estimation6 KB
    • Errors and uncertainties6 KB
  • Kinematics
    • Vectors and describing motion6 KB
    • Uniform acceleration, free fall and projectiles5 KB
  • Dynamics
    • Newton's laws, weight and resistive forces6 KB
    • Momentum and collisions6 KB
  • Forces, density and pressure
    • Moments, couples and equilibrium5 KB
    • Density, pressure and upthrust5 KB
  • Work, energy and power
    • Work, energy and power6 KB
  • Deformation of solids
    • Stress, strain and the Young modulus7 KB
  • Waves
    • Progressive waves, intensity and the Doppler effect7 KB
    • Transverse and longitudinal waves, the electromagnetic spectrum and polarisation7 KB
  • Superposition
    • Stationary waves6 KB
    • Diffraction, interference and the diffraction grating8 KB
  • Electricity
    • Current, potential difference and power5 KB
    • Resistance, resistivity and I-V characteristics6 KB
  • D.C. circuits
    • E.m.f., internal resistance and Kirchhoff's laws6 KB
    • Combining resistors and potential dividers6 KB
  • Particle physics
    • The nuclear atom and radiation6 KB
    • Quarks and leptons4 KB
  • Motion in a circle
    • Circular motion5 KB
  • Gravitational fields
    • Gravitational field and Newton's law7 KB
    • Gravitational potential5 KB
  • Temperature
    • Temperature, specific heat capacity and latent heat8 KB
  • Ideal gases
    • The mole and the equation of state5 KB
    • Kinetic theory of gases5 KB
  • Thermodynamics
    • Internal energy and the first law of thermodynamics6 KB
  • Oscillations
    • Simple harmonic motion5 KB
    • Energy, damping and resonance6 KB
  • Electric fields
    • Electric fields and uniform fields5 KB
    • Point charges and electric potential5 KB
  • Capacitance
    • Capacitors and stored energy5 KB
    • Discharging a capacitor4 KB
  • Magnetic fields
    • Magnetic fields and forces on conductors6 KB
    • Moving charges and the Hall effect6 KB
    • Electromagnetic induction5 KB
  • Alternating currents
    • Alternating currents and rectification7 KB
  • Quantum physics
    • Photons and the photoelectric effect6 KB
    • Wave-particle duality and energy levels7 KB
  • Nuclear physics
    • Mass defect and binding energy6 KB
    • Radioactive decay5 KB
  • Medical physics
    • Ultrasound6 KB
    • X-rays and CT scanning6 KB
    • PET scanning4 KB
  • Astronomy and cosmology
    • Standard candles and stellar radii5 KB
    • Hubble's law and the Big Bang4 KB
  • Practical skills
    • Planning an investigation8 KB
    • Tables, graphs and conclusions10 KB

最初のノート

Physical quantities and units / Quantities, units and estimation

Physical quantities

A physical quantity is a property that can be measured, and it always has two parts: a numerical magnitude and a unit. A length of 2.4 m2.4\,\mathrm{m} is not described by the 2.42.4 alone, since the same number of centimetres or miles would be a different length. Every equation in physics relates quantities, so a calculation that loses its units has lost half of its meaning.

Some quantities also have a direction. Those are vectors, and they are treated in the note on vectors and describing motion.

SI base quantities

The SI system is built on a small set of base quantities, from which every other quantity is derived. The five used at this level are these.

Base quantityBase unitSymbol
masskilogramkg
lengthmetrem
timeseconds
electric currentampereA
thermodynamic temperaturekelvinK

A sixth base quantity, amount of substance, has the unit mole (mol) and is used with gases and the Avogadro constant.

Derived units

A derived unit is a product or quotient of base units. Every other unit is one of these, even when it has a name of its own. The work is to reduce a named unit to base units by going back to an equation that defines the quantity.

Velocity is displacement divided by time, so its unit is m s−1\mathrm{m\,s^{-1}}. Acceleration is velocity divided by time, giving m s−2\mathrm{m\,s^{-2}}. Force is mass times acceleration, so the newton is

N=kg m s−2 \mathrm{N} = \mathrm{kg\,m\,s^{-2}}

Energy and work are force times distance, so the joule is

J=N m=kg m2 s−2 \mathrm{J} = \mathrm{N\,m} = \mathrm{kg\,m^2\,s^{-2}}

Power is energy divided by time, so the watt is

W=J s−1=kg m2 s−3 \mathrm{W} = \mathrm{J\,s^{-1}} = \mathrm{kg\,m^2\,s^{-3}}

Pressure is force divided by area, so the pascal is

Pa=N m−2=kg m−1 s−2 \mathrm{Pa} = \mathrm{N\,m^{-2}} = \mathrm{kg\,m^{-1}\,s^{-2}}

Charge is current times time, so the coulomb is C=A s\mathrm{C} = \mathrm{A\,s}. Potential difference is energy per unit charge, so the volt is

V=J C−1=kg m2 s−3 A−1 \mathrm{V} = \mathrm{J\,C^{-1}} = \mathrm{kg\,m^2\,s^{-3}\,A^{-1}}

Resistance is potential difference divided by current, so the ohm is

Ω=V A−1=kg m2 s−3 A−2 \Omega = \mathrm{V\,A^{-1}} = \mathrm{kg\,m^2\,s^{-3}\,A^{-2}}

Frequency has the hertz, Hz=s−1\mathrm{Hz} = \mathrm{s^{-1}}. Density is mass per volume, in kg m−3\mathrm{kg\,m^{-3}}. The same method works for any other quantity met later: write the defining equation and substitute the units of everything in it.

Homogeneity of equations

An equation is homogeneous when every term has the same base units. Terms that are added or subtracted must have the same units, and the two sides of an equals sign must match. This gives a quick test for whether an equation could be right. It cannot show that an equation is right, because numerical factors and dimensionless quantities such as π\pi have no units and so are invisible to the test.

To test s=ut+12at2s = ut + \tfrac12 at^2, take each term in base units. The left side is in m\mathrm{m}. The term utut is m s−1×s=m\mathrm{m\,s^{-1}} \times \mathrm{s} = \mathrm{m}. The term 12at2\tfrac12 at^2 is m s−2×s2=m\mathrm{m\,s^{-2}} \times \mathrm{s^2} = \mathrm{m}. All three agree, so the equation is homogeneous.

The same test finds the units of a constant. The period of a pendulum is thought to follow T=kl/gT = k\sqrt{l/g}. The units of l/g\sqrt{l/g} are m/m s−2=s\sqrt{\mathrm{m}/\mathrm{m\,s^{-2}}} = \mathrm{s}, which matches TT, so kk has no unit. If an equation were proposed as T=klgT = k\sqrt{lg}, the right side would have units m2 s−2=m s−1\sqrt{\mathrm{m^2\,s^{-2}}} = \mathrm{m\,s^{-1}} for lg\sqrt{lg}, which cannot equal a time unless kk carried units of s2 m−1\mathrm{s^2\,m^{-1}}, so the form is rejected.

A calculation that ends in the wrong units has gone wrong somewhere, which makes checking the units of a final answer worthwhile.

Prefixes

Prefixes scale a unit by a power of ten so that very large and very small quantities can be written compactly.

PrefixSymbolFactor
teraT101210^{12}
gigaG10910^{9}
megaM10610^{6}
kilok10310^{3}
decid10−110^{-1}
centic10−210^{-2}
millim10−310^{-3}
microμ\mu10−610^{-6}
nanon10−910^{-9}
picop10−1210^{-12}

The prefix belongs to the unit and is raised to the power with it. So 1 cm21\,\mathrm{cm^2} is (10−2 m)2=10−4 m2(10^{-2}\,\mathrm{m})^2 = 10^{-4}\,\mathrm{m^2}, not 10−2 m210^{-2}\,\mathrm{m^2}, and 1 mm3=10−9 m31\,\mathrm{mm^3} = 10^{-9}\,\mathrm{m^3}. Conversions done in the wrong direction are a common source of errors of a factor of a thousand or a million.

Worked example

A wire has a diameter of 0.36 mm0.36\,\mathrm{mm}. Its cross-sectional area in square metres is

d=0.36×10−3 mA=π(d2)2=π×(1.8×10−4)2=1.02×10−7 m2 \begin{aligned} d &= 0.36\times10^{-3}\,\mathrm{m} \\ A &= \pi\left(\frac{d}{2}\right)^2 = \pi\times(1.8\times10^{-4})^2 \\ &= 1.02\times10^{-7}\,\mathrm{m^2} \end{aligned}

A frequency of 2.4 GHz2.4\,\mathrm{GHz} is 2.4×109 Hz2.4\times10^{9}\,\mathrm{Hz}, and a wavelength of 650 nm650\,\mathrm{nm} is 6.5×10−7 m6.5\times10^{-7}\,\mathrm{m}.

Estimating physical quantities

An estimate is a value that is right to within about a factor of ten, reached by reasoning from sizes and quantities known well enough. Estimates are used to check that a calculated answer is sensible and to judge which effects matter. A few values are worth knowing at this level:

QuantityTypical value
mass of an adult70 kg70\,\mathrm{kg}
height of a door2 m2\,\mathrm{m}
walking speed1.5 m s−11.5\,\mathrm{m\,s^{-1}}
speed of a car on a motorway30 m s−130\,\mathrm{m\,s^{-1}}
speed of sound in air340 m s−1340\,\mathrm{m\,s^{-1}}
mass of a 1 litre bottle of water1 kg1\,\mathrm{kg}
density of water1000 kg m−31000\,\mathrm{kg\,m^{-3}}
atmospheric pressure1.0×105 Pa1.0\times10^{5}\,\mathrm{Pa}
wavelength of visible light400400 to 700 nm700\,\mathrm{nm}
mains voltage (UK)230 V230\,\mathrm{V}
power of a kettle2 kW2\,\mathrm{kW}

To estimate the kinetic energy of a cyclist, take a mass of 80 kg80\,\mathrm{kg} for rider and bicycle and a speed of 6 m s−16\,\mathrm{m\,s^{-1}}. Then EK=12mv2=12×80×36≈1.4×103 JE_\mathrm{K} = \tfrac12 mv^2 = \tfrac12 \times 80 \times 36 \approx 1.4\times10^{3}\,\mathrm{J}, and it is stated as roughly a kilojoule, not to three figures. The precision of an estimate should match the precision of the inputs.

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