Charges, Qualitative: Electroscope l The Phenomena Charge electroscope with rubber rod which has been rubbed with fur. Leaves separate. »Bring same.

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Presentation transcript:

Charges, Qualitative: Electroscope l The Phenomena Charge electroscope with rubber rod which has been rubbed with fur. Leaves separate. »Bring same rubber rod close to top of electroscope. observe leaves separate further. »Bring glass rod (rubbed with silk) close to top of electroscope. observe leaves approach each other. Now repeat experiment, but charge with glass rod. Leaves still separate. »Now rubber rod causes leaves to approach each other. »Glass rod causes leaves to separate. l Explanation? There exist two kinds of charge Unlike charges attract; like charges repel.

More about conductors and charging electroscopes Add some negative charge –add electrons Inside a conductor charges (electrons) are free to move The electroscope is made out of conductors –conducting main electrode –2 conducting gold leaves Add some positive charge –subtract electrons

More about conductors and charging electroscopes (continued) Add some positive charge to negatively charged leaves –subtract electrons - -

Conductors & Insulators çInsulators: In these materials, once they are charged, the charges ARE NOT FREE TO MOVE. Plastics, glass, and other “bad conductors of electricity” are good examples of insulators. çConductors: In these materials, the charges ARE FREE TO MOVE. Metals are good examples of conductors.

Law of Electrical Force Charles-Augustin Coulomb ( ) " The repulsive force between two small spheres charged with the same sort of electricity is in the inverse ratio of the squares of the distances between the centers of the spheres" q2q2 q1q1 r

Coulomb's Law MKS Units: r in meters q in Coulombs l in Newtons l is a unit vector pointing from 1 to 2 q2q2 q1q1 The force from 1 acting on 2 We call this group of constants “ k ” as in:  1 4  = 9 · 10 9 N-m 2 /C 2 0  o is permittivity of free space  o = 8.85 x C 2 /N m 2

Summary l Charges come in two varieties çnegative and positive çin a conductor, negative charge means extra mobile electrons, and positive charge means a deficit of mobile electrons Coulomb Force Law of Superposition F  =F 1  +F 2 

Two charges q = + 1 μC and Q = +10 μC are placed near each other as shown in the figure. Which of the following diagrams best describes the forces acting on the charges: +10 μC +1 μC a) b) c)

The Electric Field - The net Coulomb force on a given charge is always proportional to the strength of that charge. q q1q1 q2q2 F1F1 F F2F2 F2F2 F1F1 F = + test charge - We can now define a quantity, the electric field, which is independent of the test charge, q, and depends only on position in space: q F E    The q i are the sources of the electric field Electric Field AppletApplet

The Electric Field q F E    With this concept, we can “map” the electric field anywhere in space produced by any arbitrary: “Net” E at origin + F These charges or this charge distribution “source” the electric field throughout space Bunch of Charges

Example Two charges, Q 1 and Q 2, fixed along the x-axis as shown produce an electric field, E, at a point (x,y)=(0,d) which is directed along the negative y-axis. Q2Q2 Q1Q1 x y E d - Which of the following is true? (a) Both charges Q 1 and Q 2 are positive (b) Both charges Q 1 and Q 2 are negative (c) The charges Q 1 and Q 2 have opposite signs

Example Two charges, Q 1 and Q 2, fixed along the x-axis as shown produce an electric field, E, at a point (x,y)=(0,d) which is directed along the negative y-axis. - Which of the following is true? E Q2Q2 Q1Q1 (a) Q2Q2 Q1Q1 (c) E Q2Q2 Q1Q1 (b) E Q2Q2 Q1Q1 x y E d (a) Both charges Q 1 and Q 2 are positive (b) Both charges Q 1 and Q 2 are negative (c) The charges Q 1 and Q 2 have opposite signs

Ways to Visualize the E Field Consider the E-field of a positive point charge at the origin + + chg field lines + chg vector map +

Rules for Vector Maps Direction of arrow indicates direction of field Length of arrows  local magnitude of E + chg +

Lines leave (+) charges and return to (-) charges Number of lines leaving/entering charge  amount of charge Tangent of line = direction of E Local density of field lines  local magnitude of E Field at two white dots differs by a factor of 4 since r differs by a factor of 2 Local density of field lines also differs by a factor of 4 (in 3D) Rules for Field Lines + -

A negative charge is placed in a region of electric field as shown in the picture. Which way does it move ? a) up c) left e) it doesn't move b) down d) right

Compare the field strengths at points A and B. a) E A > E B b) E A = E B c) E A < E B

Two equal, but opposite charges are placed on the x axis. The positive charge is placed at x = -5 m and the negative charge is placed at x = +5m as shown in the figure above. 3) What is the direction of the electric field at point A? a) up b) down c) left d) right e) zero 4) What is the direction of the electric field at point B? a) up b) down c) left d) right e) zero

Field Lines From Two Like Charges There is a zero halfway between the two charges r >> a : looks like the field of point charge ( +2q ) at origin