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Electric Charge AP Physics C Montwood High School R. Casao

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Two kinds of electric charge: positive and negative. Two positive charges or two negative charges repel each other. Two unlike charges attract each other.

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Charge cannot be created, but can be transferred from one object to another – charge is conserved. When one object gains a charge, another object loses this charge; total electric charge on both bodies does not change. Electrons have been removed from the objects shown below, leaving them positively charged. Like charges exert equal and opposite repulsive forces on each other.

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Electrons have been added to these objects, making them negatively charged. Like charges exert equal and opposite repulsive forces on each other. Oppositely charged objects exert equal and opposite attractive forces on each other.

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All matter has charge; most often the positive charges equal the negative charges and the object has no net charge. More positive charges than negative charges provides a positive charge on the object. More negative charges than positive charges provides a negative charge on the object. Conductors allow the movement of charge through them; insulators do not allow the movement of charge through them. Most metals are good conductors because one or more outer electrons in each atom become detached and can move through the material.

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The other electrons remain bound to the positive nuclei, which are bound in fixed positions in the material. Insulators have few, if any, free electrons and electrons cannot move freely through the material. Semi-conductors fall between conductors and insulators in the ability of electrons to move freely through the material. An object can become charged by direct contact (friction) 1.Rub a balloon on your hair; electrons from the hair are transferred to the balloon. Balloon becomes negatively charged; hair positively charged. Hair is attracted to balloon when balloon pulled away from hair.

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2.When walking on carpet, movement of shoes on carpet rubs electrons onto shoes or feet. Charge distributes itself over body and when reach out to touch a metal object, charge moves from you to the metal object (static discharge). An object can be charged by induction. –Bring the positively charged rod close to the spheres, but dont touch the spheres.

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–Negative charges are attracted to the positively charged rod; positive charges are repelled by the positively charged rod. –Separating the spheres ensures that the charges remain on the respective sphere. –Removing the rod with the spheres separated causes the charges on the sphere to repel and seek an equilibrium position.

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Bring the positively charged rod close to the sphere, but dont touch. Positively charged rod attracts negative charges on sphere and repels the positive charges on the sphere. The sphere becomes polarized – one side positive and the other side negative. Not all charges move, just enough so that the forces of attraction equals the forces of repulsion.

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If the positively charged rod is removed, the sphere goes back to being neutral. To keep a charge on the sphere, you can attach a ground to the sphere. A ground is a conducting path between an object and the earth to prevent an electric shock due to excess charge. Earth is a conductor and can act as a source for extra electrons or as a sink for unwanted electrons.

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Electrons from the Earth pass through the ground into the sphere leaving a negative charge on the sphere. Take the positively charged rod away and the sphere stays negative.

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For a positively charged sphere, use a negatively charged rod. When the ground is connected, electrons pass from the sphere to the Earth. In either case, the sphere has been charged by induction. We cant say what charge is, we an only describe its properties and behavior. Proton and electron carry the same charge q; q = x C. Unit of charge: Coulomb, C. 1 C = total charge of 6.24 x electrons. All charge is a whole number multiple of q because there are no fractional portions of protons or electrons.

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Conductors and Insulators When charge is placed on an insulator, the charge stays where it is placed and does not move at all. When charge is placed on a conductor, it will move because of the force of repulsion between like charges. –If an object is hollow, the charge will spread uniformly over the surface. –If the object is solid, the charge will spread uniformly over the surface of the object.

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CHARGING METAL SPHERE BY INDUCTION Charges are free to move in a conductor but are tightly bound in an insulator. The earth (ground) is a large conductor having many free charges.

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In an insulator the charges can move slightly (called polarization of the insulator). A piece of paper is attracted to a charged comb because the positive charges are closer to the negatively charged comb (in the upper figure). CHARGED COMB ATTRACTS PAPER

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Charge Neutralization When two charged conductors touch, charge neutralization occurs. Sphere A contains a charge of +16 C; sphere B contains a charge of –4 C. –Allow A to touch B and 4 C of negative charge combines with 4 C of positive charge (neutralization). Net charge = 16 C + -4 C = 12 C. –12 C of positive charge remains. –Positive charges repel, so one half of the positive charge moves onto A and the other half of the positive charge moves onto B, so both A and B will have 6 C of charge when separated.

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Coulombs Law Coulombs law describes the force between any two charges q 1 and q 2. –r is the distance between the charges. –k is a constant that considers the effect of the medium on the charges. Air or vacuum: – Unit of force: Newton.

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–This expression for k will be important later in some of the problems; o is a constant used in capacitance. The smallest unit of charge known in nature is the charge on an electron or a proton. ParticleCharge (C)Mass (kg) Electron x x Proton1.602 x x Neutron01.67 x

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Coulombs law deals with forces between point charges or charged particles. –These forces are equal and opposite. –The sign of the force indicates the type of force (positive – repulsion; negative – attractive); but let the direction of the force vector determine if the force is considered positive or negative in sign.

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Small-Angle Approximation A small-angle approximation is a useful in situations involving small angles. For such angles, when the angle x is measured in radians, the trigonometric functions can be approximated by: sin x x cos x 1 tan x x Small angle approximations are useful in the calculation of the period of a pendulum, the calculation of the intensity minima in single slit diffraction, and in geometric optics.

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Small angle approximation. The value of the small angle X in radians is approximately equal to its tangent. When one angle of a right triangle is small, its hypotenuse is approximately equal in length to the leg adjacent to the small angle, so the cosine is approximately 1. The short leg is approximately equal to the arc from the long leg to the hypotenuse, so the sine and tangent are both approximated by the value of the angle in radians.

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