Presentation is loading. Please wait.

Presentation is loading. Please wait.

Fall wk 4 – Thus.21.Oct.04 Welcome, roll, questions Exercise on rising CO 2 levels Energy and Work Looking ahead: Winter seminar texts Energy Systems,

Similar presentations


Presentation on theme: "Fall wk 4 – Thus.21.Oct.04 Welcome, roll, questions Exercise on rising CO 2 levels Energy and Work Looking ahead: Winter seminar texts Energy Systems,"— Presentation transcript:

1 Fall wk 4 – Thus.21.Oct.04 Welcome, roll, questions Exercise on rising CO 2 levels Energy and Work Looking ahead: Winter seminar texts Energy Systems, EJZ

2 Measured rising CO 2 levels Intro to Energy, Cassedy & Grossman

3 Predicting future CO 2 levels You found equations for ppm of CO 2 (t in yrs) (a)Linear rise: L(t) = 8/7 t + 315 (b)Exponential rise: z(t) = 315 (1.005) t (c)Oscillations: c(t) = 4 cos 2  t To predict CO 2 level in 2100, use (a) or (b). To predict when CO 2 level will reach 550 ppm, solve (a) or (b) for time.

4 Energy and work Mechanical energy = potential + kinetic Mechanical energy is conserved (E before = E after ) In the absence of dissipative forces If the force is conservative (e.g. gravity, elec) Potential energy depends on the source: Gravitational, chemical, electrostatic, spring, others?

5 Conservation of energy In a conservative system, energy can change from kinetic energy  potential energy K = ½ mv 2  U = mgh Force = slope of potential energy curve. Where is the net force=0? Where is it greatest?

6 Conservative forces No dissipation, e.g. friction Work done = change in kinetic energy Increase in K = decrease in U Work is independent of path Work = force * distance. Which path takes more work? What is the work done in going around a loop?

7 Conservation of energy 1. Which kid will be going fastest at the bottom? A.Paul B. Kathleen C. Same 2. Which kid will reach the bottom first?

8 Energy in oscillations In an oscillating system, energy can slosh back and forth between kinetic and potential

9 Simple harmonic motion Kinetic energy = ½ mv 2 Potential energy = ½ kx 2

10 Candidate Phys7hw1 Ch.7 (p.159) # 2 (meteorite), 3 (proton), 16 (lift), 66 (ski lift) Ch.8 (p.187), Q5 (U), Q9 (K), #2 (drop), 3 (bowl), 9 (bowl), 10 (drop), 37 (U,K), 112 (Mt.Everest), 121 (hydro), 125 (waterfall), (Challenge question: 8.45)

11 Next week Monday: –required Blog workshop in CAL from 1:00-2:30 –5-minute Midquarter conferences in Zita’s office –Energy midterm and Seminar midterm on inQsit – finish by Friday No seminar class (conferences with Sem students) Read Energy Appendix B Tuesday: Required workshops –Research planning #2 –Library workshop #2 –Writing workshop at 3:30 Thus: Present your midquarter Research Proposal

12 Force and Power Energy = Force * distance: E = F x Power = Energy/time: P = E/t P = (F x)/t Velocity = v = x/t P = F (x/t) P = F v Power = Force * velocity

13 Energy derivations (extra) Force = mass * acceleration = m a a = dv/dt and v = dx/dt, so F = m dv/dt = m v (dv/dx) K = Kinetic energy = force * distance =  F dx K =  [m v (dv/dx)]dx =  m v dv = ½ mv 2 Kinetic energy = ½ mv 2 We can define a potential energy U in a conservative force: F = -dU/dx


Download ppt "Fall wk 4 – Thus.21.Oct.04 Welcome, roll, questions Exercise on rising CO 2 levels Energy and Work Looking ahead: Winter seminar texts Energy Systems,"

Similar presentations


Ads by Google