What I Need to Know This module will help you in understanding the basic concepts of electric charges and fields. The topics covered by this module are electric charges. At the end of this module, you should be able to: 1. Describe using a diagram charging by rubbing and charging by induction STEM_GP12EM-IIIa-1; 2. Explain the role of electron transfer in electrostatic charging by rubbing STEM_GP12EMIIIa-2; 3. Describe experiments to show electrostatic charging by induction STEM_GP12EM-IIIa-3; 4. Calculate the net electric force on a point charge exerted by a system of point charges STEM_GP12EM-IIIa-6; 5. Describe an electric field as a region in which an electric charge experiences a force STEM_GP12EM-IIIa-7; and 6. Calculate the electric field due to a system of point charges using Coulomb’s law and the superposition principle STEM_GP12EM-IIIa-10. What’s In In General Physics 1, your journey explored the various fundamental forces found in nature. Gravity, one of the forces you studied, was examined in a detailed manner and how it influences the movement of physical bodies. This time, we will be exploring the electromagnetic force, one of nature’s fundamental forces, which possesses both electric and magnetic force. However, we need to know how this interaction involves particles with electric charge in understanding this force. This could also be fundamentally represented by mass. When an object with mass is accelerated by an applied force, objects with electric charges are also accelerated by the presence of electric forces. This behavior can be observed when we see lightning strikes the sky, feel the shock from a metallic surface after scrubbing our shoes across a carpet or when lighter objects stick with other objects such as dust clinging on a plastic paper. Activity 1: GETTING RECHARGED! Direction: This is to check what you have learned about electric charges and electric fields. Circle the letter of the best answer. 1. Two unlike charges_________ A. attract each other C. neutralize each other B. repel each other D. have no effect on each other 2. Which of the following is not a process of charging? A. Induction B. Friction C. Conduction D. Convection 3. Material A is positively charged. When brought near to material B, they attract. Which of the following is true? A. Material B is negatively charged C. Material B is uncharged B. Material B is positively charged D. Both are uncharged 1 4. Material B has become positively charged after rubbing it with Material A. Which of the following statements is correct? A. Material B loses protons C. Material A loses proton B. Material B gains electrons D. Material A gains electron 5. What will happen when two unlike charges are brought together? They will _____ A. repel each other C. attract each other B. neutralize each other D. no effect on each other 6. If you comb your hair and the comb becomes positively charged, then your hair becomes _________. A. positively charged C. uncharged B. negatively charged D. discharged For No. 7 & No. 8 study the given Triboelectric series, where moving up means positive and moving down means negative. 7. Which of the following pairs has the strongest electrical force Melgi of attraction? Xatzki A. Welcru and Lokfu C. Xatzki and Melgi Lofku B. Zysmu and Melgi D. Kharmi and Xatzki Khamri Welcru 8. Which of the following would have a negative net charge when Zysmu rubbed with Kharmi? A. Lokfu B. Welcru C. Xatzki D. Melgi 9. A negatively charged rod is brought near a metal can that rests on a wooden box. You touch the opposite side of the can momentarily with your finger. If you remove your finger before removing the rod, what will happen to the can? A. It will be discharged C. It will become negatively charged B. it will become positively charged D. Its charge will remain as it was 10. Which of the following can be attracted by a positively charged object? A. Another positively charged object C. A neutral object B. Any object D. No other object What’s New Activity 2: WATER BENDING Direction: This activity will help you acquire real-life concepts of static electricity. Materials You Need: 3 Styrofoam cups (you can also use 2 paper cups and an inflated balloon) and a toothpick. Also, this experiment will also require water and someone with dry and clean hair. 1. Prepare the set-up by pushing the toothpick at the bottom side of the cups. Leave the toothpick to produce a gentle drop of water after filling the cup. Hold the cup directly over the second cup. Fill the cup (with a toothpick) with water and check if it is leaking steadily. 2. Observe the flow of water from the top cup to the cup below. What are your observations? ____________________________________________________ 3. Rub the third cup on someone with dry hair several times. (This process will help you in acquiring electrical charges). 4. Hold the cup (rubbed against dry hair) near the water stream without getting the cup wet. What happened to the water flow? _______________________________________ _______________________________________________________________Then, slowly move the cup away from the stream and observe. Did you observe changes? ___________ If yes, describe the change. _________________________________________________________ 2 ____________________________________________________________________________________ 5. Try other objects (such as balloon, paper cup or any material) aside from the Styrofoam cup and rub it on a dry and clear hair. What objects have you tried? _____________________________Which of the objects have changed the flow of water? _______________________________________________________________________________ What Is It Electric Charges The main building block of matter is composed of atoms and molecules. Its properties are primarily influenced by the electrically charged particles – proton, electron, and neutron. The table below shows the properties of the charged particles in terms of mass, charge, and location. Particle Mass (in terms of kg) proton electron 9.1093897 x 10-31 kg 1.6726231 x 10-27 kg neutron 1.6749286 x 10-27 kg Charge (in terms of Coulomb (C)) Location in atom +1.60217733 x 10-19 C -1.60217733 x 10-19 C nucleus outside nucleus none nucleus Materials contain a huge amount of positively charged particles called protons and negatively charged particles called electrons. When there is an equal number of protons and neutrons in a matter, the body is electrically neutral. In making a body negatively charged, electrons are added to a body. On the other hand, a positively charged body removes electrons. Number of Number of protons = electrons negatively charged positively charged The transfer of electrons from one body to another proves the law of conservation of charges. These charges are neither created nor destroyed. According to the principle of conservation of charges, the sum of electric charges of a body within a closed system is always constant. In understanding electrostatic interactions, we have to keep in mind the following conventions: 1. Any charged object can attract a neutral object. 3 2. Unlike charges attract 3. Like charges repel. Charging Objects Materials that allow the movement of electrons from one region to another are called conductors of electricity, while materials that do not allow the flow of electrons are called insulators. The majority of the metals are conductors, while nonmetals are insulators. The electrons can move while protons and neutrons are bound to remain fixed in the positive nuclei. Charging objects could happen through induction and conduction. These charging processes can be demonstrated through an electroscope. The electroscope is composed of a metal knob, metal rod, glass container, and foil (leaf). The small metal foils are hung at the end of the metal rod. This should freely move since they open after being charged. When a charged object is placed near the metal knob, this causes the foil to open up since they are being repelled by the presence of excess charges. The foils drop down when the charged object is placed away from the electroscope. Metal knob Glass Leaves (foil) Charging by Conduction When a negatively charged rod touches the neutrally charged metal knob, the knob attracts the electrons making the leaves negatively charged. When a positively charged rod touches the neutrally charged metal knob, the rod attracts the electrons making the leaves positively charged. 4 Charging by Induction When a negatively charged rod is placed near the knob, the charges undergo polarization. Positive charges are near the knob while negative charges stay away from the knob. This makes the foil open up. Electrons are repelled to the Earth when you touch the knob or when the ground wire is connected. This makes the electroscope positively charged. When you touch the knob with a finger or attach it with ground wire, the electrons from Earth move towards the knob making it negatively charged. When a positively charged rod is placed near the knob, the charges undergo polarization. Negative charges are near the knob while positive charges stay away from the knob. This makes the foil open up. Electric Force Charles Augustin de Coulomb (1736-1806) used a torsion balance in studying gravitational interaction. He studied the attractive and repulsive forces between charges. He found out that the magnitude of force decreases when the distance of separation between the charges increases. This is shown by Coulomb’s law as expressed in the equation below: |πΈπ πΈπ | π=π ππ where k is proportionality constant 9 x 109 ππ2 , πΆ2 Q1 and Q2 and point charges expressed in Coulomb (C), r is the distance of separation of two charges expressed in meter (m), and F is the electrostatic force between the two charges expressed in Newton (N). In SI units, k is not usually written but as 1 4π∈0 πΆ2 where ∈0 = 8.854 π₯ 109 ππ2 . This actually complicates the formula but could somehow help when you encounter other formulas. If test charges are placed at some angle with respect to other charges, this involves computing the x and y components of forces. Recall your previous lessons on vector resolution and trigonometric identities. Refer to the diagram below: F F Fy Ζ 5 Fx Solving for x component ∑ Solving for y component πΉπ₯ = πΉπππ π πΉπ₯ = πΉ1π₯ + πΉ2π₯ + πΉ3π₯ + β― + πΉππ₯ Solving for magnitude of resultant force πΉπππ π’ππ‘πππ‘ = √(∑ 2 πΉπ₯ ) + (∑ πΉπ¦ ) πΉπ¦ = πΉπ πππ ∑ πΉπ¦ = πΉ1π₯ + πΉ2π₯ + πΉ3π₯ + β― + πΉππ¦ Solving for the direction of resultant force ∑ π=( ∑ 2 πΉπ¦ πΉπ₯ ) The next examples will help you understand the application of Coulomb’s Law. Please prepare your scientific calculator and notebook. Example 1: Two charges lie on positive x-axis. Charge A (2.0 x 10-9 C) is 2.0 cm from the origin and Charge B is 4.0 cm from the origin. (-3.0 x 10-9 C). What is the total force exerted by these two charges on Charge C (5.0 x 10-9 C) located at the origin? A What is/are QA = 2.0 x 10-9 C at ππ΄ = 2.0 ππ given? QB = -3.0 x 10-9 C at ππ΅ = 4.0 ππ QC = 5.0 x 10-9 C at ππΆ = (0,0) B What is asked? F = ? at Q3 C Are the units No, distance of separation, r, given should be converted consistent with from cm to m. the formula? Thus, r1 = 0.02 m and r2 = 0.04 m. How will you Q Q Q x D draw the 0.01 m 0.03 m 0.04 m problem? 0.02 m A C B 0.02 m 0..04 m E What strategy must be employed? In solving the total force experienced by Q C from QA and QB, forces must be computed individually: FAonC and FBonC. The vector sum of these forces will determine the net force exerted by QA and QB on QC. F Solution Solving for FAonC: πΉπ΄πΆ Solving for FBonC: |ππ΄ ππΆ | =π ππ΄ 2 ππ2 |(2 π₯10−9 πΆ)(5 π₯ 10−9 πΆ)| = 9 π₯ 10 ( ) (0.02 π)2 πΆ2 ππ2 |(1 π₯10−17 πΆ 2 )| = 9 π₯ 109 2 ( ) πΆ 4 π₯ 10−4 π2 = 9 π₯ 109 π(2.5π₯ 10−14 ) πΉπ΄πΆ = 2.25 π₯ 10−4 π The direction of this force lies along the negative x-component since like charges repel. Thus, - 2.25 π₯ 10−4 π 9 πΉπ΅πΆ = π |ππ΅ ππΆ | ππ΅ 2 ππ2 |(−3 π₯10−9 πΆ)(5 π₯ 10−9 πΆ)| = 9 π₯ 10 ( ) (0.04 π)2 πΆ2 ππ2 |(1.5 π₯10−17 πΆ 2 )| = 9 π₯ 109 2 ( ) πΆ 1.6 π₯ 10−3 π2 = 9 π₯ 109 π(9.375π₯ 10−15 ) πΉπ΅πΆ = 8.44 π₯ 10−5 π The direction of this force lies along the positive x-component since unlike charges attract. Thus, 8.44 π₯ 10−5 π 9 6 QC ∑ G FBon QB πΉ = πΉπ΄πΆ + πΉπ΅πΆ = (−2.25 π₯ 10−4 π) + (8.44 π₯ 10−5 π) = −1.41 π₯ 10−4 π What is the conclusion? Therefore, the magnitude of total force experienced by QC from QA and QB is 1.406 x 10-4 N directed to the left. Example 2: Two point charges are located in xy coordinate system. A charge 2.00 π₯ 10−9 πΆ is located at (0,4.00 cm) and the other charge −3.00 π₯ 10−9 πΆ is located at (3.00 cm, 4.00 cm). If the third charge 5.00 π₯ 10−9 πΆ is placed at origin, find the resultant force at the third charge. A What is/are Q1 = 2.0 x 10-9 C at π1 = (0,4) given? Q2 = -3.0 x 10-9 C at π2 = (3,4) Q3 = 5.0 x 10-9 C at π3 = (0,0) B What is asked? F = ? at Q3 C Are the units No, the distance of separation, r, given should be consistent with converted from cm to m. the formula? Thus, r1 = (0 m, 0.04 m), r2 = (0.03 m, 0.04 m) and r3 = (0,0 m) D How would you Solving for unknown (c=?) draw the Q1 using Phytagorean Q2 theorem: problem? 0.03 m b = 0.03 m (opposite) 0.04 m a = 0.04 (adjacent) Ζ 36.87° c=? 0.05 m (hypotenuse) Solving for unknown (Ζ = ?) using trigonometric identities: Q3 Locating the individual forces through a diagram Q1 Q2 F2on3 x-component F2on3 36.87° y-component F2on3 F2on3 F1on3 Q3 F1on3 E What strategy must be employed? The forces experienced by Q3 from Q1 and Q2 must be computed individually. However, x and y components must be determined first. For instance, F2on3 has x and y components. The x component will be calculated by multiplying the magnitude of F2on3 by sinΖ. On the other hand, y component will be calculated by multiplying the magnitude of F2on3 by cosΖ. For F1on3, x component is zero since it lies along y component. 7 F Solution (1) Solving for F1on3: πΉ13 (2) Solving for F2on3: |π1 π3 | =π π1 2 πΉ23 = π ππ2 |(2 π₯10−9 πΆ)(5 π₯ 10−9 πΆ)| ( ) (0.04 π)2 πΆ2 ππ2 |(1 π₯10−17 πΆ 2 )| = 9 π₯ 109 2 ( ) πΆ 4 π₯ 10−3 π2 = 9 π₯ 109 π(6.25π₯ 10−15 ) πΉ13 = 5.625 π₯ 10−5 π The direction of this force lies along the negative y-component since like charges repel. Thus, - 5.625 π₯ 10−4 π = 9 π₯ 109 ππ2 |(−3 π₯10−9 πΆ)(5 π₯ 10−9 πΆ)| ( ) (0.05 π)2 πΆ2 ππ2 |(1.5 π₯10−17 πΆ 2 )| = 9 π₯ 109 2 ( ) πΆ 2.5 π₯ 10−3 π2 = 9 π₯ 109 π(6 π₯ 10−15 ) = 5.4 π₯ 10−5 π = 9 π₯ 109 πΉ23 The magnitude of the force from Q2 towards Q3 is 5.4 π₯ 10−5 π (3) Solving for x, y components πΉ23π₯ = (4) Solving for magnitude and direction of the resultant force 5.4 π₯ 10−5 π(π ππ 36.87°) = 3.24 π₯ 10−5 π πΉ23π¦ = 5.4 π₯ 10−5 π(πππ 36.87°) = 4.32 π₯ 10−5 π πΉ13π₯ = 0π (since F13 lies along y-axis) −4 πΉ13π¦ = − 5.625 π₯ 10 π F13 F23 Sum x component y component 0π − 5.625 π₯ 10−4 π 3.24 π₯ 10−5 π 3.24 π₯ 10−5 π |π2 π3 | π1 2 πΉπ = √(∑ 4.32 π₯ 10−5 π −1.31 π₯ 10−5 π π=( 2 πΉπ₯ ) + (∑ πΉπ¦ ) 2 = √(3.24 π₯ 10−5 π)2 + (−1.31 π₯ 10−5 π)2 πΉπ = 3.49 π₯ 10−5 π ∑ ∑ πΉπ¦ πΉπ₯ −1.31 π₯ 10 ) = π‘ππ−1 ( −5 −5 3.24 π₯ 10 π π ) = −21.94° ππ 338° G What is the Therefore, the magnitude and direction of the resultant conclusion? force is 3.49 π₯ 10−5 π , 338°. You can verify the magnitude and direction of the resultant force using the graphical method for vector analysis. Electric Fields You were introduced to the behavior of electric charges and how these charges produce attractive and repulsive forces. Aside from these forces, it also creates an electric field E. The electric field of charge Q is the space surrounding the charge. It also exerts a force F on any test charge q placed within that region. 8 The electric field is represented by the equation below: π¬= π π π where E is the electric field expressed in πΆ , F is the electric force expressed in newton (N), and q is the charge expressed in coulombs (C). If q is positive, the direction of E is the direction of F. On the other hand, the force on a negative charge is opposite to the direction of the E. F E F We can also calculate E given the magnitude and position of all charges |π π | πΉ involved. Since πΉ = π 1 2 2 , we substitute this formula in πΈ = . Thus, π π π π¬=π π π Like dealing with charge situated at some angles, you can similarly perform the same using the trigonometric and vector resolutions concepts. Refer to the diagram below. Suppose we have a negative charge at xy plane. We want to calculate the electric field at point P: E E Ey P Ζ Ex Solving for x component Solving for y component πΈπ₯ = πΈπππ π πΈπ¦ = πΈπ πππ ∑ πΈπ₯ = πΈ1π₯ + πΈ2π₯ + πΈ3π₯ + β― + πΈππ₯ Solving for magnitude resultant force πΉπππ π’ππ‘πππ‘ = √(∑ 2 πΈπ₯ ) + (∑ of ∑ πΈπ¦ = πΈ1π₯ + πΈ2π₯ + πΈ3π₯ + β― + πΈππ¦ the Solving for the direction of resultant force 2 ∑ πΈπ¦ ) π=( ∑ πΈπ¦ ) πΈπ₯ the Example 3: A point charge π1 = +6.00 π₯ 10−9 πΆ is at the point π₯ = 0.800 π, π¦ = 0.600 π and a second point charge π2 = −2.00 π₯ 10−9 πΆ is at the point π₯ = 0.800 π, π¦ = 0 π. Calculate the magnitude and direction of the resultant electric field at the origin due to these charges. 9 A B C D What is/are given? What is asked? Are the units consistent with the formula? How would you draw the problem? q1 = +6.00.0 x 10-9 C at π1 = (0.800 π, 0.600 π) q2 = -2.00.0 x 10-9 C at π2 = (0.800 π, 0 π) E = ? at (0,0) Yes, given values have correct SI units. Solving for unknown (c=?) using Phytagorean theorem: Q1 c=? 1m (hypotenuse) Ζ 53° 0.6 m b = 0.03 m (opposite) Solving for unknown (Ζ = ?) using trigonometric identities: 37° Q2 0.8 m Review field of charges a = 0.04 (adjacent) Locating the individual electric fields at (0,0): E2 E1 53° E1y 53° E1x E What strategy must be employed? The electric fields experienced in origin (0,0) must be computed individually. Furthermore, x and y components must be solved for each E1 and E2. We then calculate the magnitude and direction of the resultant electric field. F Solution (1) Solving for F1on3: (2) Solving for E2: |Q1 | E1 = k 2 r1 2 |(6 x10−9 C)| Nm = 9 x 109 2 ( ) (1 m)2 C Nm2 |(6 x10−9 C)| = 9 x 109 2 ( ) C 1m2 = 9 x 109 N(6x 10−9 ) N E1 = 54 C (outward direction) (3) Solving for x, y components E1x = N 54 C (sin 53°) E1y = 54 = −43.126 N (cos 53°) C N C (along –x-axis) |π2 | π2 2 2 |(−2 π₯10−9 πΆ)| ππ = 9 π₯ 109 2 ( ) (0.8 π)2 πΆ ππ2 |(−2 π₯10−17 πΆ)| = 9 π₯ 109 2 ( ) πΆ 0.64π2 = 9 π₯ 109 π(−3.125 π₯ 10−17 ) π = 28.125 π πΆ πΈ2 = π πΉ23 The electric field is directed towards the positive x-axis since it is a negative charge (inward direction of field). (4) Solving for magnitude and direction of the resultant force πΉπ = √(∑ N = −32.498 (along – y axis) C N E2x = 28.125 C 2 πΉπ₯ ) + (∑ πΉπ¦ ) 2 = √(−15.001 π/πΆ)2 + (−32.498 π/πΆ)2 πΉπ = 35.79 π/πΆ 10 N ∑ π=( ∑ E2y = 0 C since it lies along x-axis x component E1 E2 Sum G N −43.126 C N 28.125 C N −15.001 C What is the conclusion? y component -32.498 0 N C −32.4898 πΉπ¦ πΉπ₯ ) = π‘ππ−1 ( = 65.22° −32.498 π/πΆ ) −15.001 π/πΆ N C Therefore, the magnitude and direction of the resultant force π is 35.79 πΆ , 65.22°. You can verify the magnitude and direction of the resultant force using a graphical method for vector analysis. Electric Flux The relationship between electric charge and electric field was also formulated alternatively in Gauss’s law (Karl Friedrich Gauss 1777-1855). This is logically equivalent to Coulomb’s law, but this was easier to use in finding electric field for symmetrical charge distribution. Gauss’s law general statement is expressed as ππΈ = πΈπ΄cosΖ where is the electric flux ππ2 , πΆ E is the magnitude of electric field expressed in π πΆ , Ζ is the angle between the normal line of the surface and electric field lines. and A is the area of a given surface expressed in m2. Electric flux refers to the amount of electric field lines penetrating a given surface. The electric flux is maximum if the electric field lines are perpendicular to the surface or parallel to the normal line of the surface. The electric flux is zero when the electric field line is parallel to the surface or perpendicular to the normal line of the surface. At a given angle, the electric flux is directly proportional to the component of the electric field lines. Example 4: A point charge π = 8.00 π₯ 10−9 πΆ is at the center of the cube with sides of length 0.200 m. What is the electric flux through one of the six faces of the cube? A B What is/are given? What is asked? q = +8.00 x 10-9 C ; π = 0.200 π π = ? at one of the faces of the cube 11 C D Are the units consistent with the formula? How would you draw the problem? Yes, given values have correct SI units. c = 0.141 c = 0.283 0.200 m 0.200 m 0.200 m E F What strategy must be employed? Solution Hence, the distance from the charge to the surface of the cub is 0.141 m Using Gauss’s law, substitute E with formula for Electric Field π π¬ = π ππ 2 −9 π ππ |(8 π₯10 πΆ)| 9 πΈ = π 2 = 9 π₯ 10 2 ( ) (0.141 π)2 π πΆ 9 = 9 π₯ 10 G What is the conclusion? 0.200 m ππ2 πΆ2 |(8 π₯10−9 πΆ)| ππ2 9 (4.02 π₯ 10−7 ) ( ) = 9 π₯ 10 2 2 0.0199 π πΆ πΈ = 3,621.55 π/πΆ π΄ = π 2 = (0.200 π)2 = 0.04 π2 π ππΈ = πΈπ΄πππ Ζ = 3,621.55 (0.04 π2 ) = 144,862 πΆ ππ2 πΆ Therefore, the electric flux at any surface is 144,862 ππ2 πΆ What’s More Activity 3: QUALITATIVE PROBLEMS Direction: Solve the following problems as directed. You may show your solution on a separate sheet of paper (1) Two spheres of equal mass and equal charge are separated at a distance r. (a) Derive an expression for the quantity of charge that must be on each sphere so that the spheres are in an equilibrium where attractive and repulsive forces are balanced. (b) How would doubling the distance between spheres affect the expression for the value of q from the previous problem. Explain. _____________________________________________________________________________ _____________________________________________________________________________ ____________________________________________________________________ 12 (2) How would you draw the electric field lines given the test charges below: (3) Coulomb’s law and Newton’s law of gravitation are similar in structure. Can Gauss’s law be applied to gravitational fields? _________If so, what changes are needed?____________________________________________________________________________ __________________________________________________________________________ What I Have Learned Activity 4: QUANTITATIVE PROBLEMS Direction: Write your answers on a separate sheet of paper. You may also consult your Physics teacher. Three charged spheres are at the positions shown in the figure. (a) Find the net electrostatic force at sphere B. (b) Find the net electric field at (4,-3) 4 cm 4.5µC A 8.2 µC B 3 cm 6.0µC C Scoring Rubric Criteria 3 Physics The approach is Approach appropriate and complete Procedure Description Mathematical and logical procedures are clear, complete, and connected Diagrams and symbols used are appropriate and complete 2 The approach contains minor errors Mathematical and logical procedures are missing/contain errors Parts of the diagrams and symbols contain errors 13 1 Some of the concepts and principles are missing or inappropriate Most of the mathematical and logical procedures 0 The solution doesn’t indicate an approach Most of the parts of the diagrams and symbols are not useful The entire visualization is wrong or did not include visualization. All procedures are incomplete and contain errors What I Can Do Activity 5. BUILDING CONCEPT MAP Direction: Create a concept map out from the things you have learned from this module. You can use words, terms, phrases, or formulas in connecting these concepts. Refer to the scoring guide below: Mueller’s Classroom Concept Rubric Legible (easy to read) Accurate (concepts were used accurately) Complete (sufficient number of relevant concepts and relationships) Sophisticated (finding meaningful connections between relevant concepts) No (0-1) Yes (2) Many inaccuracies (0-2) A few inaccuracies (3-4) No inaacuracies (5) Limited use of concepts (0-2) Some use of concepts (3-4) Sufficient number of concepts (5) Little or none (0-1) Few meaningful connections made (2-4) Some meaningful connections made (5-7) Meaningful and original insights demonstrated (8) Assessment Direction: Write the letter of your choice in the space provided. ______1.The diagram below shows the behavior of the electroscope before and after a positively charged rod is placed near the electroscope knob. This tells us that the movement of electrons is from ______. a.rod to leaves b.leaves to knob c.knob to leaves, then back to knob d.leaves to knob, then back to leaves _____2.A glass rod was positively charged when rubbed with a silk cloth. The net positive charge is accumulated because the glass rod a.loses protons c.gains electrons b.loses electrons d.loses electrons _____3.Gravitational forces and electric forces are both a.forces with attractive and repulsive behaviors b.indirectly proportional to the square root of separation between bodies c.directly proportional to the product of the masses and charges d.decreasing when the distance between two bodies is decreasing 14 _____4.At which point is the electric field strength strongest? A D C B _____5.Three spheres were brought together. When Spheres A and B are brought together, they attract. When spheres B and C are brought together, they also repel. Which of the following is true? a.Spheres A & C have same signs c.Spheres A & C have opposite signs b.Spheres B & C have same signs d.Spheres A & B have similar signs _____6.The first object has a charge of +3nC, and the second object has a charge of 6 nC. Which is true about the electric forces between these objects? a.F1on2= 2F2on1 b.3F1on2= 6F2on1 c.-6F1on2=2F2on1 d.F1on2=F2on1 For Nos. 7 to 9, refer to the diagram below: _____7. A positively charged rod was brought near to a metallic plate; what is the type of charge induced along the side facing the rod? a.positive b.negative c.netural d.depends on number of charges _____8.If the positively charged rod was touched on the neutral metallic plate, what is the charge of the plate? a.same b.negative c.positive d.depends on number of charges _____9.After the positively charged rod is placed near the plate, a grounded wire was attached. What is the charge of the plate after the wire is removed? a.negative c.neutral b.positive d.depends on number of charges _____10.The electric flux through the surface at the right is ____ η a.zero c.positive b.negative d.unknown _____11.A test charge produced an electric field, E, at point 3 m away from the charge. The point where the field is half its original values is located at a.1.5 m from the charge c.4.5 m from the charge b.6 m from the charge d.at the point of charge _____12.The electric field of a body is directly related to its a.momentum b.kinetic energy c.potential energy d.charge it carries _____13.Charge q1 (26.0 µC) and q2 (-47.0 µC) experienced an electrostatic force of 5.70 N between them at a distance of ____ a.1.39 m b.1.93 m c.2.14 x 10-19 d.1.464 x 10-8 _____14.How many electrons have been removed from a positively charged particle if it has a net charge of 5 x 10-9 C? a.5 x 10-9 electrons c.1 x 10-8 electrons -9 b.2.5 x 10 electrons d.incomplete information 15 _____15.A sphere of radius 0.05 m has a charge of 2.0 nC. The charge is said to be located at the center of the sphere. The magnitude of electric field inside the surface is a.zero c.thrice the original value b.twice the original value d.half the original value Additional Activities Activity 6. SOCIAL CONTEXT Direction: The community is a rich source for learning opportunities in electrostatics. Choose one from the following suggested activities in understanding the importance and utilization of electrostatics in our daily lives: 1. Ask a local weather forecaster/Science teacher/physicist/electrician/engineer through phone calls or interview through Zoom, Google Meet, or Messenger and inquire (with supervision from your parents/guardian/learning facilitator) about lightning, lightning safety, and lightning rods. 2. Conduct simulations on electrostatics, electric fields, Gauss’s law using online sources. From this, write a short reflection. Refer to any sites below: - https://phet.colorado.edu/en/simulation/charges-and-fields - https://www.falstad.com/emstatic/ - http://web.mit.edu/viz/soft/visualizations/DLIC/doc/simulations/ex periments/electrostatics/package-summary.html - https://javalab.org/en/category/electricity_en/static_electricity_en/ 3. Suppose you are to demonstrate a trick to kids using electrostatic charging. How will you demonstrate the trick? List down the materials (preferably available at home), step-step procedures, and brief explanation of how this trick works. 16 Answer Key General Physics 2 Module 1 Activity 1: Getting Recharged 1. A 2. D 3. A 4. A 5. A 6. B 7. D 8. C 9. B 10. C Activity 2: Water Bending 2. vertical, thin, unbroken stream of water 4. the stream of water was bent towards the cup; yes (there should be changes); the stream went back to its original flow 5. answers may vary; the influence of charged objects to water bending may vary depending on their ability to gain or lose charges Activity 3. Qualitative Problems Activity 4. Quantitative Problems 17 References Printed Resources Sears, F., Zemansky, M. and Young, H. (1992). College Physics 7th Edition. Addison-Wesley Publishing Company Zitzewits, Haase and Harper (2013). PHYSICS Principles and Problems. The MAcGraw-Hill Companies, Inc. Online References Harmon, K. (2011). Bend water with static electricity. Scientific American. https://www.scientificamerican.com/article/static-electricity-bring-science-home/ Java Lab (n.d.). Static Electricity Simulation. Retrieved last February 18, 2021 from https://javalab.org/en/category/electricity_en/static_electricity_en/ Massachusetts Institute of Technology. (n.d.) Package simulations experiments electrostatics. Retrieved last February 20, 2021 from http://web.mit.edu/viz/soft/visualizations/DLIC/doc/simulations/experiments/electros tatics/package-summary.html Mueller, J. (n.d.) Concept map rubric. Retrieved last February 22, 2021 from https://teach.its.uiowa.edu/sites/teach.its.uiowa.edu/files/docs/docs/Concept_Map_Ru brics_ed.pdf PHET (2021). Charges and Fields. University of Colorado. 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