Physics 1161 Lecture 4 Potential & Potential Energy

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Presentation transcript:

Physics 1161 Lecture 4 Potential & Potential Energy

Recall Work from Phy 1151 Work done by the force given by: W = F d cos(θ) Positive: Force is in direction moved Negative: Force is opposite direction moved Zero: Force is perpendicular to direction moved Careful! Ask WHAT is doing work! Opposite sign for work done by you! Conservative Forces Δ Potential Energy = -Wconservative Use book or brick for prop. Ask students if I am doing positive or negative work, what about gravity.

Preflight 4.1 F In what direction does the force on a negative charge at point A point? left right up 58% Electric field points in the direction a POSITIVE charge would feel force. 39% 3%

Preflight 4.2 motion - F C - F - F The work is zero because the path is perpendicular to the field - F - F A B Uniform E When a negative charge is moved from A to C the ELECTRIC force does positive work. zero work. negative work. 37% 45% 18%

Preflight 4.3 C The work is negative the electric force opposes the direction of motion A B - F - F - F - F - F - Uniform E motion When a negative charge is moved from A to B the ELECTRIC force does positive work. zero work. negative work. 32% 24% 43%

Preflight 4.5 C A B - - - - - Uniform E When a negative charge is moved from A to B, the electric potential energy of the charge Increases is constant decreases 33% UE = -WE field Like “climbing up hill” – increases potential energy 33% 33%

When a negative charge is moved from A to B, the electric potential energy of the charge + C increases is constant decreases

When a negative charge is moved from A to B, the electric potential energy of the charge + C increases is constant decreases

Electric Potential Energy AC: W=0 E + C CB: W<0 B A - - - - - When a negative charge is moved from A to B, the electric potential energy of the charge (1) increases (2) is constant (3) decreases 1) The electric force is directed to bring the electron closer to the proton. 2) Since the electron ends up further from the proton the electric field did negative work. 3) So the electric potential energy increased

Work and D Potential Energy W = F d cos(q) Gravity Electric Brick raised yi yf Charge moved ∞  rf FE = kq1q2/r2 (left) WE = -kq1q2/rf DUE= +kq1q2/rf FG = mg (down) WG = -mgh DUG= +mgh yf rf h yi

Preflight 4.11 1 + 5 m 5 m + - 2 5 m 3 The electric potential energy of this set of charges is: (1) positive (2) zero (3) negative Bring in (1): zero Bring in (2): positive Bring in (3): negative x 2 55% 26% 18%

Electric Potential (like height)* Units Joules/Coulomb Volts Batteries Outlets EKG Really Potential differences Equipotential lines at same height Field lines point down hill V = k q/r (distance r from charge q) V(∞) = 0 Comment on lab w/ equipotential lines

Preflight 4.7 To go from B to A, a positive charge must climb “up hill” – increases potential energy. Hence A is at higher potential than B The electric potential at point A is _______ at point B greater than equal to less than 38% 32% 30%

Preflight 4.9 The electric potential at point A is _______ at point B conductor The electric potential at point A is _______ at point B greater than equal to less than 8% 81% 11% The electric field is zero at any point within a conducting material

The electric potential at A is _______ the electric potential at B. greater than equal to less than A B C + +

The electric potential at A is _______ the electric potential at B. greater than equal to less than A B C + E + 1) Electric field lines point “down hill” 2) AC is equipotential path (perpendicular to E) 3) CB is down hill, so B is at a lower potential than (“down hill from”) A

Electric Potential due to Proton What is the electric potential a distance r = 0.5310-10 m from a proton? (Let V() = 0) What is the electric potential energy of an electron a distance r = 0.5310-10 m from a proton? rf = 0.510-10 m + -

Comparison: Electric Potential Energy vs. Electric Potential Electric Potential Energy (U) - the energy of a charge at some location. Electric Potential (V) - found for a location only – tells what the EPE would be if a charge were located there (usually talk about potential differences between two locations): U = qV Neither has direction, just location. Sign matters!

Example Two Charges Calculate electric potential at point A due to charges Calculate V from +7mC charge Calculate V from –3.5mC charge Add (EASY!) V = kq/r V7 = 1.26 x 104 V V3 = -0.63 x 104 V Vtotal = 0.63 x 104 V A 4 m 6 m Q=+7.0μC Q=-3.5 μ C W=ΔU= ΔVq = 1.26 x 104 V How much work do you have to do to bring a 2 μ C charge from far away to point A?

In the region II (between the two charges) the electric potential is always positive Positive at some points, negative at others Always negative Q=-3.5 mC Q=+7.0mC I II III

In the region II (between the two charges) the electric potential is always positive Positive at some points, negative at others Always negative Q=-3.5 mC Q=+7.0mC I II III Very close to positive charge potential is positive Very close to negative charge potential is negative