120 likes | 303 Views
The Bohr Model of Atoms. The Electrons can only orbit on specific orbits These orbits have specific energies When an electron falls “down” energy is released in the form of a photon If a passing photon has just the right energy, an electron can get bumped “up”.
E N D
The Bohr Model of Atoms • The Electrons can only orbit on specific orbits • These orbits have specific energies • When an electron falls “down” energy is released in the form of a photon • If a passing photon has just the right energy, an electron can get bumped “up” • Because the electrons can only be on certain special energy levels, only certain amounts of energy can be absorbed/emitted • The special energies that can be absorbed or emitted depends on which type of atom you have
The Quantum Mechanics of Atoms • Electrons don’t exist at one place at all – they are in a nebulous probability cloud • The Bohr model is simpler, so we’ll pretend it’s right electron cloud
Atomic Spectra • Suppose you take an atom and bump the electrons up (by heating it, for example). What type of light comes out? • Spectrum consists of emission lines • Exactly which lines tells you the kind of atom, like a fingerprint Q. 19: Analyzing Emission Spectra
Atomic Spectra • Suppose you take an atom and shine a bright white light on it. What does the spectrum of the light look like when it comes out? • Initial spectrum is continuous • Atom absorbs certain very specific frequencies • The same frequencies you saw before
Hot Stuff Heat • Heat is disorganized energy • Kinetic energy is organized motion – like all the air in the room moving the same way • If you make all the atoms in the room move different ways, you heat up the room • Whenever energy gets completely randomized, turned into heat, we say it is in thermal equilibrium • There is a statistical tendency for things to get disorganized
Temperature – the Kelvin Scale • Heat is disorganized energy. Temperature is a measure of how much heat there is. • If you have no disorganized energy,you are at Absolute Zero • Absolute Zero: -273oC • Kelvin - just like Celsius,but the zero is shifted toabsolute zero. T0 = -273o C Temp. F C K Abs. Zero –459 –273 0 Freezing 32 0 273 Room 70 21 294 Boiling 212 100 373 Sun 9900 5500 5800 TK = TC + 273 • 300 K is comfortable
Ideal Gasses • In a gas, all the atoms (or molecules) bounce around randomly. • The hotter it is, the faster they bounce around • As they bounce, they collide with the walls • Collisions cause pressure • The more atoms, and the hotter, thehigher the pressure P Pressure n Number density T Temperature (K) k constant P = knT Q. 19: Ideal Gas Law Temperature must be in Kelvin (K)!
Black Body Radiation Flux is brightnessover area F =T4 2900 K • All Objects give off electromagnetic radiation “light” • Some objects are (nearly) perfect absorbers, and perfect emitters. Such objects are called black bodies • Color and brightness of light depends on temperature 4500 K 5500K 10,000K 20,000K
Black Body Radiation lmaxT = 2900 Km • T in Kelvin Q. 20: Using Wien’s Law
Kirchoff’s Laws • Hot thick solid, liquid, or gas – Continuous spectrum • Thin gas – bright line spectrum • Thin gas with hotter thick gas behind it – dark line spectrum
Kirchoff’s Laws Continuous Spectrum: Hot, thick solid, liquid, or gas Bright Line Spectrum: Hot, thin gas Dark Line Spectrum: Cooler gas in front of hot, thick solid, liquid, or gas