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Fri. Nov 19 Phy107 Lecture 31 From Last Time… Superconductor = zero-resistance material Meissner effect = exclusion of magnetic field Leads to superconducting levitation Critical temperature, critical current, critical magnetic field - range of usefulness. Most critical temperatures far below room T. High-temperature superconductors discovered with transition temp near liquid nitrogen. HW11 Chap. 15: Concept 2, 4, 14, 24, Prob. 2, 4
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Page 1: Phy107Lect31

Fri. Nov 19 Phy107 Lecture 31

From Last Time…• Superconductor = zero-resistance material• Meissner effect = exclusion of magnetic field

– Leads to superconducting levitation

• Critical temperature, critical current, criticalmagnetic field - range of usefulness.

• Most critical temperatures far below room T.• High-temperature superconductors discovered

with transition temp near liquid nitrogen.

HW11Chap. 15: Concept 2, 4, 14, 24, Prob. 2, 4

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Fri. Nov 19 Phy107 Lecture 31

Physics of the Nucleus

• Nucleus consists of protons and neutrons denselycombined in a small space (~10-14 m)– Protons have a positive electrical charge– Neutrons have zero electrical charge (are neutral)

• Spacing between these nucleons is ~ 10-15 m

• Size of electron orbit is 5x10-11 m

• Nucleus is 5,000 times smallerthan the atom!

Neutron

Proton

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Fri. Nov 19 Phy107 Lecture 31

Neutrons and Protons• The number of protons in a nucleus is the

same as the number of electrons since theatom has a net zero charge.

• The number of electrons determines whichelement it is.– 1 electron → Hydrogen– 2 electrons → Helium– 6 electrons → Carbon

• How many neutrons?

Number of neutrons for a particularelement can vary!

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Fri. Nov 19 Phy107 Lecture 31

Carbon

Another form of Carbon has6 protons, 8 neutrons in the nucleus. This is 14C.

• Example: carbon

• Carbon has 6 electrons (Z=6),this is what makes it carbon.

• Zero net charge so there are6 protons in the nucleus.

• Most common form of carbon has 6 neutronsin the nucleus. Called 12C

C12

6

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Fri. Nov 19 Phy107 Lecture 31

Isotopes• Both 12C and 14C have same chemical properties.

• This is why they are both called carbon. Same # electrons and hence same # protons in nucleus.

• But the nuclei are different. They have differentnumber of neutrons. These are called isotopes.

• Difference is most easily seen in the binding energy.

• Nuclei that are bound more tightly are less likely to ‘fall apart’.

• In fact 14C is radioactive.It is unstable to emission of an electron.

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Fri. Nov 19 Phy107 Lecture 31

QuestionHydrogen is the element with one electron.

Which of the following is NOT the nucleus ofan isotope of hydrogen?

A. One protonB. One proton and one neutronC. Two protons and one neutron

HydrogenDeuterium

Trituium

One proton One protonone neutron

One protontwo neutrons

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Stable and Unstable Isotopes

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Fri. Nov 19 Phy107 Lecture 31

Nuclear Force• So what holds the nucleus together?

• Coulomb force? Gravity?

• Coulomb force only acts oncharged particles– Repulsive between protons,

and doesn’t affect neutrons at all.

• Gravitational force is much too weak.Showed before that gravitational force ismuch weaker than Coulomb force.

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Fri. Nov 19 Phy107 Lecture 31

The Strong Nuclear Force

• New force.• Dramatically stronger than Coulomb force.• But not noticeable at large distances.

– I.e. Atoms do not attract each other.

• Must be qualitatively different than Coulomb force.• How can we characterize this force?

– Range is on the order of the size of nucleus.– Stronger than Coulomb force at short distances.

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Fri. Nov 19 Phy107 Lecture 31

How strong is strong?

• Electron is bound in atom by Coulomb attraction.Strength ~10 eV.

• Protons in nucleus are 50,000 times closer together.Coulomb repulsion ~500,000 eV = 0.5 MeV

• Nuclear force must be much stronger than this.

• Found that nuclear force~ 100 times stronger than Coulomb force

• Nucleons are bound in nucleus by ~ 8 MeV / nucleon(8,000,000 eV / nucleon)

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Fri. Nov 19 Phy107 Lecture 31

Very strong!• To change properties of nucleus, need much

larger energies than to change electronic state.

• Properties of nucleus that might change are– Exciting nucleus to higher internal energy state– Breaking nuclei apart– Fusing nuclei together.

• Required high energiesprovided by impact of high-energy……protons, electrons, photons, other nuclei

• High energies produced in an accelerator facility

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Fri. Nov 19 Phy107 Lecture 31

What is the strong nuclear force?

• Modern view is that all forces arise from anexchange of particles.

• Coulomb force is theexchange of photons that have zero mass

• Strong nuclear force is theexchange of a particle ‘effectively’ with mass.

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Fri. Nov 19 Phy107 Lecture 31

EM force and Strong Force

Electromagnetic force Strong nuclear force(approximate view)

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Fri. Nov 19 Phy107 Lecture 31

Nucleons are not fundamental

• We now know thatprotons and neutronsare not fundamentalparticles.

• They are composedof quarks, whichinteract byexchanging gluons.

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Fri. Nov 19 Phy107 Lecture 31

The ‘new’ nuclear force

• Strong force is actually betweenquarks in the nucleons.

• Quarks exchange gluons.

• Most of the strong force gluesquarks into protons and neutrons.

• But a fraction of this force leaksout, binding protons and neutronsinto atomic nuclei

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Visualizing a nucleus

A nucleon made up ofinteracting quarks. A nucleus of several nucleons,

with their interacting quarks

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Fri. Nov 19 Phy107 Lecture 31

Comparing the ‘old’ and ‘new’

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Fri. Nov 19 Phy107 Lecture 31

Four fundamental forces

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Fri. Nov 19 Phy107 Lecture 31

Particles in the nucleus

• Proton– Charge +e– Mass 1.6726x10-27 kg– Spin 1/2

• Neutron– Charge 0– Mass 1.6749x10-27 kg– Spin 1/2

Both are spin 1/2 particles -> Fermions

One particle per quantum state

Can still, however,get an approximatedescription of nucleuswith protons andneutrons.

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Fri. Nov 19 Phy107 Lecture 31

What makes a nucleus stable?• A nucleus with lower energy is more stable.

• This is a general physical principle,that systems tend to their lowest energyconfigurations– e.g. water flows downhill– Ball drops to the ground– Hydrogen atom will be in its ground state

• Same is true of nucleus

• Observed internal configurationis that with the lowest energy.

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Fri. Nov 19 Phy107 Lecture 31

Quantum states in the nucleus

• Just like any quantum problem, proton andneutron states in the nucleus are quantized.

• Certain discrete energy levels available.

• Neutrons and protons are Fermions– 2 protons cannot be in same quantum state– 2 neutrons cannot be in same quantum state

• But neutron and proton are distinguishable,so proton and neutron can be in samequantum state.

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Fri. Nov 19 Phy107 Lecture 31

Energy of nucleus

• Nucleons attracted by nuclear force,so more nucleons give more attractive force.

– This lowers the energy.

• But more nucleons mean occupying higherquantum states, so higher energy required.

• Tradeoff gives observed nuclearconfigurations

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Fri. Nov 19 Phy107 Lecture 31

Proton and Neutron states• Various quantum states for nucleons in the nucleus• Proton and neutron can be in the same state

protonsneutrons

Nucleon quantum statesin the nucleus

Schematic indicatingneutron & proton canoccupy same state

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Fri. Nov 19 Phy107 Lecture 31

Different nuclear configurations

Nucleus with only protons:high energy statesmust be occupied.

Nucleus with protons and neutrons:don’t need to occupy higherenergy states

Higher energy Lower energy

Tendency towardequal #protons & neutrons

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Fri. Nov 19 Phy107 Lecture 31

Stability of nuclei• Dots are naturally

occurring isotopes.• Blue shaded region is

isotopes created in thelaboratory.

• Observed nucleihave ~ N=Z

• Slightly fewer protonsbecause they costCoulomb repulsionenergy.

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Fri. Nov 19 Phy107 Lecture 31

2 protons &2 neutrons

Nuclear Binding Energy• Mass of nucleus is less than

mass of isolated constituents.• The difference is the binding energy.

Arises from E=mc2

Equivalence of massand energy.

Heliumnucleus

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Fri. Nov 19 Phy107 Lecture 31

Binding energy of different nuclei

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Fri. Nov 19 Phy107 Lecture 31

Differences between nuclei• Schematic view of

previous diagram

• 56Fe is most stable

• Move toward lowerenergies by fission orfusion.

• Energy releasedrelated to differencein binding energy.

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Fri. Nov 19 Phy107 Lecture 31

Nuclear spin• Since nucleus is made of protons and neutrons,

and each has spin, the nucleus also has a spin(magnetic moment).

• Can be very large.

• Turns out to have a biological application.

• Water is ubiquitous in body,and hydrogen is major element of water (H2O)

• Nucleus of hydrogen is a single proton.– Proton has spin 1/2

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Fri. Nov 19 Phy107 Lecture 31

Magnetic resonance imaging• 80% of the body's atoms are hydrogen atoms,• Once excited by the RF signal, the hydrogens will tend to return to their lower state in a

process called "relaxation" and will re-emit RF radiation at their Larmor frequency. Thissignal is detected as a function of time, and then is converted to signal strength as afunction of frequency by means of a Fourier transformation.

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Fri. Nov 19 Phy107 Lecture 31

Magnetic resonance imaging

MRI detects photon resonance emission andabsorption by the proton spins.