Particles Quantum Phenomena and Electricity 4 Fundamental Forces

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Particles, Quantum Phenomena and Electricity

Particles, Quantum Phenomena and Electricity

4 Fundamental Forces n n Gravity Electromagnetic Weak nuclear Strong nuclear Ø Ø gravitons

4 Fundamental Forces n n Gravity Electromagnetic Weak nuclear Strong nuclear Ø Ø gravitons photons W bosons (and Z boson) Pi mesons (pions) Any particle with mass Any charged particle All leptons, baryons and mesons Hadrons

Alpha Particle Scattering • Nucleus is tiny • Nucleus is massive • Nucleus is

Alpha Particle Scattering • Nucleus is tiny • Nucleus is massive • Nucleus is very dense • Atom is mostly free space

Quantum Phenomena Annihilation - The conversion of mass to energy - 2 gamma ray

Quantum Phenomena Annihilation - The conversion of mass to energy - 2 gamma ray photons released

Quantum Phenomena Pair Production - The conversion of energy to mass - A gamma

Quantum Phenomena Pair Production - The conversion of energy to mass - A gamma ray photon of sufficient energy may decay into an electron and a positron

Particle Families Leptons – Fundamental particles Leptons = Lepton No. of +1 Anti-leptons =

Particle Families Leptons – Fundamental particles Leptons = Lepton No. of +1 Anti-leptons = Lepton No. of -1 Not a Lepton = Lepton No. of 0

Particle Families Hadrons – Composed of quarks Baryons = Baryon No. of +1 Anti-baryon

Particle Families Hadrons – Composed of quarks Baryons = Baryon No. of +1 Anti-baryon = Baryon No. of -1 Not a Baryon = Baryon No. of 0 (Including mesons)

Particle Families

Particle Families

Some particles:

Some particles:

Feynmann Diagrams EM Interaction

Feynmann Diagrams EM Interaction

Feynmann Diagrams Weak Interaction (Beta minus)

Feynmann Diagrams Weak Interaction (Beta minus)

Feynmann Diagrams Weak Interaction (Beta plus)

Feynmann Diagrams Weak Interaction (Beta plus)

Feynmann Diagrams Weak Interaction (Electron capture)

Feynmann Diagrams Weak Interaction (Electron capture)

Feynmann Diagrams Weak Interaction (Electron-proton collision)

Feynmann Diagrams Weak Interaction (Electron-proton collision)

β- (neutron) Decay The quark structure of the neutron is udd In β- decay

β- (neutron) Decay The quark structure of the neutron is udd In β- decay a down quark changes to an up quark. uud = +2/3 -1/3 = 1 The neutron (Q = 0) has changed into a proton (Q = 1). neutron (udd) → proton (uud)

β+ (proton) Decay In β+ decay an up quark in a proton changes to

β+ (proton) Decay In β+ decay an up quark in a proton changes to a down quark. This only happens in proton-rich nuclei. proton (uud) → neutron (udd)

Particle Interactions The 4 quantities (Q, B, S and L) have to be the

Particle Interactions The 4 quantities (Q, B, S and L) have to be the same after a reaction as they were before it occurred. Important: Strangeness is only conserved in the strong and electromagnetic interactions.

The electronvolt is an amount of energy equal to the above value. It is

The electronvolt is an amount of energy equal to the above value. It is arrived at by applying the equation E= QV to an electron accelerated by a p. d. of 1 Volt.

Photoelectric Effect hf = φ + Ek (SI Units)

Photoelectric Effect hf = φ + Ek (SI Units)

Energy Levels and electron excitation E = hf

Energy Levels and electron excitation E = hf

Fluorescent Tube

Fluorescent Tube

Wave-particle Duality The Photoelectric Effect suggests the particle nature of light. Electron diffraction suggests

Wave-particle Duality The Photoelectric Effect suggests the particle nature of light. Electron diffraction suggests the wave nature of particles. de. Broglie Wavelength,

Series circuits: n n Current same at all points – it is a continuous

Series circuits: n n Current same at all points – it is a continuous flow. Voltage shared between components. 24

Parallel Circuits n n Voltage same across branches as that of power source. Current

Parallel Circuits n n Voltage same across branches as that of power source. Current splits between branches (splits and rejoins at junctions). 25

Cells in Series and Parallel

Cells in Series and Parallel

Using Ammeters n n n Ammeters measure the current flowing through themselves. Ammeters are

Using Ammeters n n n Ammeters measure the current flowing through themselves. Ammeters are placed in series. The ideal ammeter ought to have zero resistance.

Using Voltmeters n n n Voltmeters measure the voltage between two places. This is

Using Voltmeters n n n Voltmeters measure the voltage between two places. This is also called potential difference. (The difference in the “push” between two places) Voltmeters are placed in parallel.

I-V Characteristics Thermistors – Resistance decreases as temperature increases LDR – Resistance decreases as

I-V Characteristics Thermistors – Resistance decreases as temperature increases LDR – Resistance decreases as light intensity increases

Resistors in Series Easy!

Resistors in Series Easy!

Resistors in Parallel

Resistors in Parallel

Resistor Combinations

Resistor Combinations

Potential Dividers What is the p. d. across each of the two resistors? 12

Potential Dividers What is the p. d. across each of the two resistors? 12 V across each as they are equal resistance

Potential Dividers What is the p. d. across each branch? 3. 0 V

Potential Dividers What is the p. d. across each branch? 3. 0 V

Potential Dividers What is the p. d. across the whole of the upper branch?

Potential Dividers What is the p. d. across the whole of the upper branch? 6. 0 V What is the p. d. across the lower branch? 6. 0 V What is the p. d. across each of the resistors in the upper branch? 3. 0 V

Potential Dividers What is the potential at X when thermistor has a resistance of

Potential Dividers What is the potential at X when thermistor has a resistance of 1000Ω? This is the p. d. across thermistor, the potential at X is 12 -11. 7=0. 3 V

Potential Dividers What is the potential at X when the LDR has a resistance

Potential Dividers What is the potential at X when the LDR has a resistance of 5000Ω? This is the p. d. across the LDR, in this case it is also the potential at X due to where the LDR is in the circuit.

Superconductivity Certain materials have zero resistivity at and below a critical temperature which depends

Superconductivity Certain materials have zero resistivity at and below a critical temperature which depends on the material. There is a persistent current in the superconductor that causes a magnetic field to be set up that repels the magnetic field of the permanent magnet.

EMF and internal resistance • The quantity of energy transferred to unit charge as

EMF and internal resistance • The quantity of energy transferred to unit charge as it passes through the cell • The p. d. across the cell when no current flows • Energy is transferred in the cell due to the internal resistance

RMS Values

RMS Values

Oscilloscope n n x-axis is called the timebase y-axis is the y-gain or input

Oscilloscope n n x-axis is called the timebase y-axis is the y-gain or input sensitivity (which represents p. d. ) Calculate the frequency and the amplitude of the signal shown if the timebase is set to 10 ms / division and the y-gain is set at 100 m. V / division T=40 x 10 -3 s f=1/T=25 Hz Peak Voltage = 1. 5 x 100 m. V = 150 m. V