Phys 102 – Lecture 4 Electric potential energy & work.

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Presentation transcript:

Phys 102 – Lecture 4 Electric potential energy & work

Today we will... Learn about the electric potential energy Relate it to work Ex: charge in uniform electric field, point charges Apply these concepts Ex: electron microscope, assembly of point charges, dipole energy & hydration shells

Potential energy Potential energy U – stored energy, can convert to kinetic energy K Review Phys. 101 x h Gravitational potential energy (ex: falling object) Elastic potential energy (ex: spring) Total energy K + U is conserved Same ideas apply to electricity r + + Electric potential energy (ex: repelling charges)

Work Review Phys. 101 Work – transfer of energy when a force acts on a moving object Work done by force F Change in potential energy Displacement Angle between force and displacement Units: J (“Joules”) θ It matters who does the work For conservative forces, work is related to potential energy

Electric potential energy & work Gravity Electricity Charge moved xi  xf (in uniform E field to left) Mass raised yi  yf down left yf xi xf d h + yi

Positive and negative work If you moved object against external force (gravitational, electric, etc.), you did positive work, force did negative work + + Wyou > 0 WF < 0 Wyou < 0 WF > 0 If you moved object along external force (gravitational, electric, etc.), you did negative work, force did positive work

Checkpoint 1.2 C – A B When a negative charge is moved from A to C the ELECTRIC force does positive work zero work negative work

ACT: Checkpoint 1.3 C – A B When a negative charge is moved from A to B the ELECTRIC force does positive work zero work negative work

ACT: Work in a uniform E field Let WA-B be the answer to the previous problem – A B The negative charge is now moved from A to C to B. The work done by the electric force is Greater than WA-B Same as WA-B Less than WA-B

Path independence of work B For conservative forces (ex: gravitational, electric), work is independent of path. Work depends only on end points. Potential energy of charge at position A Potential energy of charge at position B

Calculation: Electron microscope (revisited) A uniform E field generated by parallel plates accelerates electrons in an electron microscope. If an electron starts from rest at the top plate what is its final velocity? –Q +Q d = 1 cm E = 106 N/C – Electron microscope

E.P.E of two point charges Electric potential energy of two charges q1 and q2 separated by a distance r Note: NOT r2 q1 + – q2 +1.6 x 10–19 C = = –1.6 x 10–19 C r = 0.53 x 10–10 m Ex: What is the electric potential energy of the proton and the electron in H?

ACT: E.P.E. of 2 charges + – + – In case A, two charges of equal magnitude but opposite sign are separated by a distance d. In case B, they are separated by 2d. + – Case A +q –q d + – Case B +q –q 2d Which configuration has a higher electric potential energy? Case A has a higher E.P.E. Case B has a higher E.P.E. Both have the same E.P.E.

Sign of potential energy What does it mean to have a negative electric potential energy? + – Ex: H atom Electron Proton UE < 0 relative to energy of an electron very far away (r  ), away from E field of proton, i.e. a “free” electron UE Free electron r Energy must be added in order to free electron bound to proton Electron bound to proton in H atom

Calculation: two charges Two +5 C, 1 kg charges are separated by a distance of 2 m. At t = 0 the charge on the right is released from rest (the left charge is fixed). What is the speed of the right charge after a long time (t  )? From EX 1, SPRING ‘10 r = 2 m +5C +5C Fixed Free to move

Work done to assemble charges How much work do you do assembling configuration of charges? q2 q1 + – r Imagine bringing charges from infinitely far away to a separation r Potential energy of charges infinitely far Potential energy of charges in final configuration

Calculation: assembling charges How much work do you do to assemble the charges q1 = +2 μC, q2 = +7 μC, and q3 = –3.5 μC into a triangle? q1 5 m 4 m q2 q3 3 m 3 m

ACT: Checkpoint 2.1 + Charges of equal magnitude are assembled into an equilateral triangle d d d + – The total work required by you to assemble this set of charges is: positive zero negative

Calculation: dipole in E-field An electric dipole with moment p = 6.2 x 10–30 C∙m is placed in a uniform external electric field E = 106 N/C at an angle θ = 60°. Calculate the total electric potential energy of the dipole. θ = 60° +q –q

ACT: dipole energy Which configuration of dipole in a uniform electric field has the lowest electric potential energy? A. B. C. +q –q +q –q +q –q

Hydration shell radius Recall that H2O dipole aligns to electric field of ions. However, at room temperature, H2O also has rotational kinetic energy that tends to randomize dipole orientation Dipoles are randomized (bulk water) Dipoles tend to be aligned (hydration shell) We can estimate distance to interface between bulk and ordered water for a monovalent ion (Ex: Na+) H20 near a charge

Summary of today’s lecture Electric potential energy & work Path independence Conservation of energy Electric potential energy for point charges