{"id":9851,"date":"2019-12-05T09:57:42","date_gmt":"2019-12-05T04:27:42","guid":{"rendered":"https:\/\/kseebsolutions.guru\/?p=9851"},"modified":"2021-07-02T15:43:58","modified_gmt":"2021-07-02T10:13:58","slug":"2nd-puc-physics-question-bank-chapter-1","status":"publish","type":"post","link":"https:\/\/kseebsolutions.guru\/2nd-puc-physics-question-bank-chapter-1\/","title":{"rendered":"2nd PUC Physics Question Bank Chapter 1 Electric Charges and Fields"},"content":{"rendered":"

You can Download Chapter 1 Electric Charges and Fields Questions and Answers, Notes, 2nd PUC Physics Question Bank with Answers<\/a>, Karnataka State Board Solutions help you to revise complete Syllabus and score more marks in your examinations.<\/p>\n

Karnataka 2nd PUC Physics Question Bank Chapter 1 Electric Charges and Fields<\/h2>\n

2nd PUC Physics Electric Charges and Fields NCERT Text Book Questions and Answers<\/h3>\n

Question 1.
\nWhat is the force between two small charged spheres having charges of
\n2\u00d7 10-7 <\/sup>and 3 x 10-7<\/sup> C placed 30cm apart in air?
\nAnswer:
\n\"2nd<\/p>\n

Question 2.
\nThe electrostatic force on a small sphere of charge 0.4 \u00b5 C due to another small sphere of charge – 0.8 \u00b5 C in air is 0.2 N.
\n(a) What is the distance between the two spheres ?
\n(b) What is the force on the second sphere due to the first?
\nAnswer:
\n\"2nd<\/p>\n

Question 3.
\nCheck that the ratio ke2<\/sup>\/Gme<\/sub> mp<\/sub> is dimensionless. Look up a table of Physical constants and determine the value of this ratio. What does the ratio signify?
\nAnswer:
\n\"2nd
\nThis value represents the ratio of electrostatic force of gravitational force between an electron and a proton.<\/p>\n

Question 4.
\n(a) Explain the meaning of the statement \u2018electric charge of a body is quantised\u2019,
\n(b) Why can one ignore quantisation of electric charges when dealing with macroscopic i.e large scale charges?
\nAnswer:
\n(a) The magnitude of charge on a proton or an electron (e = 1.6 x 1019<\/sup>c) is called elementary charge. Since protons and electrons are only basic charged particles in a matter, the charge on an object must be integral multiple of \u00b1e(1.6\u00d71019<\/sup>c),
\ni.e. the charge possessed by an object cannot be a fraction of + e. Mathematically, the charge on any matter must be equal to q = \u00b1ne, where n is an integer.<\/p>\n

(b) In practice, the charge on any charged body is very large. On the other hand, the charge on an electron is very small. When electrons are added to a body (negatively charged body) or removed from a body (positively charged body), the change taking place in the total charge on the body is so small that the charge seems to be varying in a continuous manner. Therefore quantisation of electric charge can be ignored, when dealing with a large scale charged body.<\/p>\n

\"KSEEB<\/p>\n

Question 5.
\nWhen a glass rod is rubbed with a silk cloth, charges appear on both. A similar phenomenon is observed with many other pairs of bodies. Explain how this observation is consistent with the law of conservation of charge.
\nAnswer:
\nBefore rubbing, both the glass rod and the silk cloth are electrically neutral. In other words, the net charge on the glass rod and the silk cloth is zero. When the glass rod is rubbed with silk cloth, a few electrons from the glass rod get transferred to the silk cloth. As a result, the glass rod becomes positively charged and the silk cloth negatively charged. Since the magnitude of positive charge on the glass rod is the same as that of negative charge on the silk, the net charge on the system is zero. Thus the appearances of charge on the glass rod and the silk cloth is in accordance with the law of conservation of charges.<\/p>\n

Question 6.
\nFour point charges qA<\/sub> = 2 \u00b5C, qB<\/sub> = -5 \u00b5C, qc<\/sub> = 2 \u00b5C and qD<\/sub> = -5 \u00b5C are located at the corners of a square ABCD of side 10cm. What is the force of a charge of 1 \u00b5C placed at the centre of the square?
\nAnswer:
\nConsider the square ABCD of each side 10cm and centre O. The charge of 1 \u00b5C is placed at point O. The charge of 1 \u00b5C is placed at point O.
\n\"2nd
\nequal and opposite forces due to the charges qA<\/sub> and qc<\/sub>. Similarly, the charges of 1 \u00b5C experiences equal and opposite forces Ffi<\/sub> and Fd<\/sub> due to the charges qB<\/sub> and qD<\/sub>.<\/p>\n

Hence, the net force on the charge of 1 p C due to the given arrangement of the charges is zero.<\/p>\n

Question 7.
\n(a) An electrostatic field line is a continuous curve. That is a Held line cannot have sudden breaks. Why not?
\n(b) Explain why two field lines never cross each other at any point?
\nAnswer:
\n(a) The tangent at a point on the electric line of force tells the direction of electric field changes from point to point. Therefore the line of force are, generally, curved lines. Further, they are continuous curves and cannot have sudden breaks. For if it is so, it will indicate the absence of electric field at the breakpoints<\/p>\n

(b) The tangents at a point on the line of force gives the direction of electric field at that point. If two lines of forces intersect each other at a point, then electric field at that point will have two directions. As the same cannot be true, two lines of force will never intersect each other.<\/p>\n

Question 8.
\nTwo point charges qA<\/sub> = 3 \u00b5C and qB<\/sub> = -3 \u00b5C are located 20 cm apart in vacuum.
\n(a) What is the electric field at the midpoint O of the line AB joining the two charges?
\n(b) If a negative test charge of magnitude 1.5\u00d710-9<\/sup>C is placed at this point, what is the force experienced by the test charge?
\nAnswer:
\n\"2nd
\n\"2nd
\nThe force on the negative charge acts in a direction opposite to that of the electric field.<\/p>\n

\"KSEEB<\/p>\n

Question 9
\nA system has two charges qA<\/sub> = 2.5\u00d7 10-7<\/sup>C and qB<\/sub> = -2.5 x 10-7<\/sup>C located at points
\nA: (0, 0, -15cm), respectively. What are the total charge and electric dipole moment of the system?
\nAnswer:
\nThe charges qA<\/sub> and qB<\/sub> are located at the points A (0,0, – 15cm) and B (0, 0, +15cm). B The points A and B lie on z-axis as shown.
\nIt follows that,
\nAB = OA + OB = 30ci = 0.3m
\n\"2nd<\/p>\n

\"2nd<\/p>\n

Question 10.
\nAn electric dipole with dipole moment 4\u00d710-9<\/sup>cm is aligned at 30\u00b0 with the direction of a uniform electric field of magnitude 5 \u00d7 104<\/sup> NC1<\/sup>. Calculate the magnitude of the torque acting on the dipole.
\nAnswer:
\n\"2nd<\/p>\n

Question 11.
\nA polythene piece rubbed with wool is found to have a negative charge of 3x 10 7<\/sup>C
\n(a) Estimate the number of electrons transferred (from which to which ?)
\n(b) Is there a transfer of mass from wool to polythene?
\nAnswer:
\n(a) The total charge transferred,
\nq = -3 x 10-7<\/sup>C
\ncharge on an electron, e = -1.6x 1019<\/sup>C From quantization of charge, q = ne Therefore, number of electrons transferred,
\n\"2nd
\n(b) Since electrons are transferred from wool to polythene, there is transfer of mass also. This is because electrons are material particles and possess mass (me<\/sub> = 9.1 x 10-31<\/sup>kg).<\/p>\n

Question 12
\n(a) Two insulated charged copper spheres A and B have their centres separated by a distance of 50 cm. What is the mutual force of electrostatic repulsion if the charge on each is 6.5 x 10-7<\/sup>C ? The radii of A and B are negligible compared to the distance of separation.<\/p>\n

(b) What is the force of repulsion if each sphere is charged double the above amount and the distance between them is halved?
\nAnswer:
\n(a) Charge on sphere A, q1<\/sub>, = 6.5 x 10-7<\/sup>c
\ncharge on sphere B, q2<\/sub> = 6.5 x 10 7<\/sup>c
\nDistance between the spheres A and B, r = 50 cm= 0.5m
\n\"2nd<\/p>\n

Question 13
\nSuppose the spheres A and B in exercise 1.12 have identical sizes. A third sphere of the same size but uncharged is brought in contact with the first, then brought in contact with the second, and finally removed from both. What is the new force of repulsion between A and B?
\nAnswer:
\nThe charge on A and B, q1<\/sub> = q2<\/sub> = 6.5x 107<\/sup>C.
\nThe distance between the spheres r = 0.5m. Since the spheres are same size, they will possess equal charges on being brought in contact. When uncharged sphere c (q3<\/sub> = 0) is bought in contact with A, charge left on A.
\n\"2nd<\/p>\n

Question 14.
\nFig 1.33 shows tracks of three charged particles in a uniform electrostatic field. Give the signs of the three charges. Which particle has the highest charge to mass ratio?
\n\"2nd
\nAnswer:
\nCharges (1) and (2) are negative as they were attracted by the positive plate and charge (3) is positive as it is deflected towards negative plate.
\nThus charge (3) has highest charge to mass ratio (as it would be a positive figure)<\/p>\n

Question 15.
\nConsider a uniform electric Held \\(\\vec { E } =3\\times { 10 }^{ 3 }\\hat { i } { N }\/{ C }\\)
\n(a) What is the flux of this field through a spheres A and B, charges inside the box. Therefore, if the net outward flux is zero, we cannot conclude that the charge inside the box is zero. One can only say that the net charge inside the box is zero.<\/p>\n

(b) A point charge +10 p C is a distance 5cm directly above the centre of a square of side 10cm, as shown in fig. 1.34. What is the magnitude of the electric flux through the square of 10cm on a side whose plane is parallel to the yz plane?
\n(b) What is the flux through the same square if the normal to its plane makes a 60\u00b0 angle with the x-axis ?
\nAnswer:
\n\"2nd<\/p>\n

Question 16.
\nWhat is the net flux of the uniform electric field of exercise 1.15 through a cube of side 20cm oriented so that its faces are parallel to the coordinate planes?
\nAnswer:
\n\"2nd
\n\"2nd
\nIn each plane, there is a set two faces of the cube. Through one face, electric flux enters and through the other face, an equal flux leaves. Therefore, net flux through the cube,
\n\"2nd<\/p>\n

Question 17.
\nCarefid measurement of the electric field at the surface of a black box indicates that the net outward flux through the surface of the box is 8.0 \u00d7103<\/sup>Nm2<\/sup>\/C.
\n(a) What is the net charge inside the box?
\n(b) If the net outward flux through the surface of the box were zero, could you conclude that there were no charges inside the box? Why or why not?
\nAnswer:
\n\"2nd<\/p>\n

(b) If the net outward flux through the surface of the box is zero, it cannot be concluded that there is no charge inside the box. There may be equal amount of positive and negative charges inside the box. Therefore, if the net outward flux is zero, we cannot conclude that the charge inside the box is zero. One can only say that the net charge inside the box is zero.<\/p>\n

\"KSEEB<\/p>\n

Question 18.
\nA point charge +10 \u00b5 C is a distance 5cm directly above the centre of a square of side 10cm, as shown in fig. 1.34. What is the magnitude of the electric flux through the square?
\n\"2nd
\nAnswer:
\n\"2nd<\/p>\n

consider that the charge q is at a distance of 5 cm from the square ABCD of each side 10cm as shown. The square ABCD can be considered as one of the six faces of a cube of each side 10cm. Then according to Gauss\u2019 theorem, total electric flux through all the six faces of the cube,
\n\"2nd<\/p>\n

Question 19.
\nA point charge of 2 p C is at the centre of a cubic Gaussian surface 9cm on edge. What is the net electric flux through the surface?
\nAnswer:
\nHere, q = 2\u00b5C = 2 \u00d7 10-6<\/sup>C
\nside of cube, a = 9cm = 0.09 m
\nAccording to Gauss\u2019 law, the net electric flux through all the six faces of the cube,
\n\"2nd<\/p>\n

Question 20.
\nA point charge causes an electric flux of\u00a0 1 x 103<\/sup>Nm2<\/sup>\/C to pass through a spherical Gaussian surface of a 10cm radius centred on the charge.
\n(a) If the radius of the Gaussian surface were doubted, how much flux would pass through the surface?
\n(b) What is the value of the point charge?
\nAnswer:
\nHere \u03c6 = -1 x 103<\/sup>Nm2<\/sup>C-1
\n<\/sup>radius of Gaussian surface, r = 10cm = 0. 1m.
\n(a) If the radius of the gaussian surface is doubled, the electric flux through the new surface will still remain the same i.e. -1 x 103<\/sup>Nm2<\/sup>C-1
\n<\/sup>This is because the same charge is enclosed by the gaussian surface in the two cases.<\/p>\n

(b) Let q be the charge inside the surface:
\n\"2nd<\/p>\n

Question 21.
\nA conducting sphere of radius 10cm has an unknown charge. If the electric field 20cm from the centre of the sphere is 1.5 x 103<\/sup>N\/C and the points radially inward, what is the net change on the sphere?
\nAnswer:
\nConsider a sphere of radius
\nR = (=10cm = 0.1 m) and centre O.
\nLet the charge on the sphere be \u2018q\u2019. Further, let \u2018P\u2019 be a point at a distance r = 20cm from the centre of the sphere.
\n\"2nd
\nThe electric field E( = 1.5103<\/sup>NC-1<\/sup>) is directed radially inward as shown. So as to enclose the charged sphere, draw a sphere (gaussian surface) with the point O as centre and r as the radius. As the electric field is radial, it is normal to the gaussian surface everywhere. Therefore, electric flux through the gaussian surface,
\n\"2nd<\/p>\n

Question 22.
\nA uniformly charged conducting sphere of 2.4 m diameter has a surface charged density of 80 \u00b5 c\/m2
\n<\/sup>(a) Find the charge on the sphere.
\n(b) What is the total electric flux leaving the surface of the sphere?
\nAnswer:
\n\"2nd
\n\"2nd<\/p>\n

Question 23.
\nAn infinite line charge produces a field of 9 x 104<\/sup>N\/C at a distance of 2cm. Calculate the linear charge density.
\nAnswer:
\n\"2nd<\/p>\n

Question 24.
\nTwo large thin metal plates are parallel and close to each other. On their inner faces, the plates have surface charge densities of opposite signs and of magnitude 17x 10-22<\/sup>C\/m2<\/sup>. What is \\(\\vec { E } \\)\u00a0 :
\n(a) In the outer region of the first plate
\n(b) In the outer region of the second plate, and
\n(c) Between the plates?
\nAnswer:
\nHere, \u03c3= 17 x 10-22<\/sup> Cm-2
\n<\/sup>(a) To the left of plates.
\nThe electric field at this region is zero
\n\"2nd
\n(b) To the right of the plates
\nThe electric field in this region is zero.<\/p>\n

(c) Between the two plates
\nThe electric field at this region is given by
\n\"2nd<\/p>\n

2nd PUC Physics Electric Charges and Fields Additional Exercises<\/h3>\n

Question 25.
\nAn oil drop of 12 excess electrons is hold stationery under a constant electric field of 2.55 x 104<\/sup> NC-1<\/sup> in is 1.26 g em-3<\/sup>. Estimate the radius of the drop, (g = 9.81 ms-2<\/sup>; e = 1.60×10 19<\/sup>c)
\nAnswer:
\n\"2nd<\/p>\n

Question 26.
\nWhich among the curves shown in Fig 1.35 cannot possibly represent electrostatic field lines?
\n\"2nd
\nAnswer:
\n(a) It is not. Because field lines are not normal to the surfaces of the conductors.
\n(b) It is not, because, field lines cannot start from negative charge.
\n(c) It is correct representation of electric field lines.
\n(d) It is not because, field lines cannot intersect each other.
\n(q) It is not, because field lines cannot form closed loops without having touching the source or any charge.<\/p>\n

\"KSEEB<\/p>\n

Question 27.
\nIn a certain region of space, electric field is along the z-direction throughout. The magnitude of the electric field is, however, not constant but increases uniformly along the positive z-direction, at the rate of 105<\/sup>Nc1 <\/sup>per meter. What are the force and torque experienced by a system having a total dipole moment equal to 10-7<\/sup>cm in the negative z-direction?
\nAnswer:
\nSuppose that a dipole consisting of charges – q at A and +q at B is placed along z-axis, such that it has dipole moment along the negative z-direction. The dipole moment of the dipole along z axis, PZ<\/sub>= -10-7<\/sup>Cm
\n\"2nd
\nThe negative sign has been taken for they reason that dipole moment is along the x negative z-axis.<\/p>\n

The electric field is applied along the positive direction of z-axis, such that (along z-axis) In a non – uniform electric field, the force on dipole is given by,
\n\"2nd<\/p>\n

The negative sign shows that force on the dipole is along negative z-axis.
\nSince the elctric dipole moment is along negative z-axis and the electric field is along positive z-axis, 0 = 180\u00b0.
\nHence, torque on the dipole, \u03c4 = pE sin 180\u00b0 = 0.<\/p>\n

Question 28.
\n(a) A conductor A with a cavity as shown in Fig. 1.36 (a) is given a charge Q. Show that the entire charge must appear on the outer surface of the conductor.
\nAnswer:
\n\"2nd
\n(b) Another conductor B with charge q is inserted into the cavity keeping B insulated from A. Show that the total charge on the outside surface of A is Q + q [Fig. 1.36(b)].
\n(c) A sensitive instrument is to be shielded from the strong electrostatic fields in its environment. Suggest a possible way.
\nAnswer:
\n\"2nd
\nConsider the gaussian surface (dotted) so as to enclose the cavity by lying wholly inside the conductor A. Since the electric field inside a conductor is zero, the part of the conductor within the cavity does not contain any net charge. By extending the same argument, no charge can be present inside the gaussian surface, which lies just within the conductor. Hence the entire charge A must appear on the outer surface of the conductor A.<\/p>\n

consider the gaussian surface (dotted), it encloses the cavity and the conductor B with ^ charge q inserted in the cavity.
\n\"2nd
\nAs such, the electric flux will cross the gaussion surface and it would imply that the electric field exists inside the conductor A. But the electric field inside the conductor A must be zero. It will be true, only if the charge q on conductor B induces charge-q on the inner surface and +q on the outer surface of the<\/p>\n

Conductor A. As there is already a charge +Q on the outer surface of the conductor A, the total charge on its outer surface becomes Q+q.<\/p>\n

(c) The electric field inside a metallic conductor is zero. Therefore, instrument can be shielded from the strong electrostatic fields by enclosing n it with a hollow metallic structure.<\/p>\n

Question 29.
\nA hollow charged conductor has a tiny hole cut into its surfaces. Show that the electric field in the hole is \\(\\left( { \\sigma }\/{ { 2\\epsilon }_{ 0 } } \\right) \\hat { i } \\), where q is the unit vector in the outward normal direction and a is the surface charge density near the hole.
\nAnswer:
\nLet \\(\\vec { E } \\)be the electric field in the hole due to rest of the charged conductor. In order to find \\(\\vec { E } \\) consider that the hole in the conductor is plugged. Let \\(\\vec { E } \\) be the electric field due to the charged conductor at a point’ outside it then,
\n\"2nd<\/p>\n

After plugging the hole, the conductor becomes a closed one, the electric field inside it must be zero. It implies that inside the conductor, electric field due to the rest of the conductor must be equal and opposite to that due to the small portion of the conductor, that plugs the hole. However, outside the conductor, the two fields are in the same direction i.e. along the outward normal to the surface of the conductor. It therefore, follows that the electric field in the hole due to the rest of the conductor,
\n\"2nd<\/p>\n

Question 30.
\nObtain the formula for the electric field due to a long thin wire of uniform linear charge density X, without using Gauss\u2019 law
\nAnswer:
\nConsider a long thin wire of uniform linear charge density \u03bb \u00a0Let us find electric field due to the wire at the point P at a normal distance. PN = r from the wire Let AB = dx be a small elementary portion of the wire at a distance x from point N.
\n\"2nd
\nThen charge on the elementary portion AB, dq= \u03bb dn<\/p>\n

Therefore, electric field due to the small portion AB at the point P,
\n\"2nd
\nThe component dE sin \u03b8due to the different small portions, such as AB, will cancel each other. Therefore, effective electric field due to the small portion AB,
\n\"2nd<\/p>\n

Question 31.
\nIt is now believed that protons and neutrons are themselves built out of more elementary of charge \\(+\\frac { 2e }{ 3 } \\) and then\u2019 down quarks\u2019 denoted by \u2018d\u2019 of charge \\(-\\frac { e }{ 3 } \\) together with electrons build up ordinary matter. Suggest a possible quark composition of a proton and neutron.
\nAnswer:
\nThe charge on up quark (u) = \\(+\\frac { 2e }{ 3 } \\)
\nThe charge on down quark = \\(-\\frac { e }{ 3 } \\)
\nThe charge on proton is +e and it is made of three quarks. Therefore the possible quark composition of a proton is \u2018uud<\/p>\n

On the other hand, neutron is a neutral particle but it is also made of three quarks. For this, the possible composition of the neutron is \u2018udd\u2019.<\/p>\n

Question 32.
\n(a) Consider an arbitrary electrostatic field configuration. A small test charge is placed at a null point of the configuration. Show that the equilibrium of the test charge is necessarily unstable.<\/p>\n

(b) Verify the result for the simple configuration of two charges of the same magnitude and sign placed a certain distance apart.
\nAns:
\n(a) To prove the result, let us assume that the test charge placed at the null point is in stable equilibrium. If it is so, then on being displaced slightly away from the null point, the test charge should return to its position., It implies that if a closed surface is drawn around the test charge, there will be a net inward flux of the electric field through its surface. According to Gauss law, there cannot be any electric flux through its surface as it does not enclose any charge. Hence our assumption is wrong and the test<\/p>\n

(b) For the configuration of the two charges of the same magnitude and sign, the null point is the mid point of the line joining the two charges. If the test charge is displaced slightly from the null point along the line, it will return back due to the restoring force that comes into the day. But if the charge is displaced slightly from the null – point along normal to the line it will not return. This is because the resultant force due to the configuration of two charges will take it away from the null point. For the test charge to be in stable equilibrium restoring force must come into play, when it is displaced in any direction. Hence the test charge cannot be in stable equilibrium.<\/p>\n

\"KSEEB<\/p>\n

Question 33.
\nA particle of mass m and change -q enters the region between the two plates initially moving along X-axis with speed \\({ V }_{ \\lambda }\\). The length The length of plate is L and a uniform electric field \u00a3 is maintained between the plates. Show that the vertical deflection of the particle at the far edge of the plate is \\(-\\frac { qE{ L }^{ 2 } }{ 2m{ v }_{ \\lambda }^{ 2 } } \\)
\nAnswer:
\nLet y be the vertical deflection of the charged particle since the particle is initially moving along x-axis, its initial speed along the vertical.
\nThe electric field E is directed along vertical. Therefore, acceleration of the particle along the vertical, \\({ U }_{ y }=0\\)
\nThe time for which the force due to the electric field acts on the particle,
\n\\({ a }_{ y }=\\frac { qE }{ m } \\)
\n\"2nd<\/p>\n

Question 34.
\nSuppose that the particle in exercise 1.33 is an electron projected with velocity Vx<\/sub> = 2x 106<\/sup>ms1<\/sup>. If E between the plates separated by 0.5 cm is 9.1 x 102<\/sup>Nc_1<\/sup>, where will the electron strike the upper plate? Given, e = 1.6 x 1019<\/sup>C; and Me<\/sub> = 1 x 1031 <\/sup>kg.
\nAnswer:
\nSuppose that the electron strikes the upper plate at a distance x from the end, where it enters the electric field. Therefore the expression for vertical deflection becomes
\n\"2nd<\/p>\n

2nd PUC Physics Electric Charges and Fields Additional Entrance Examination Questions and Answers<\/h3>\n

Question 1.
\nA charge Q is placed at each of the opposite corners of a square. A charge q is placed at each
\nof the other two corners. If the net electrical force on the Q is zero, then ~ equals
\n(A) -1
\n(B) 1
\n(C) \\(-2\\sqrt { 2 } \\)
\n(D) \\({ -1 }\/{ \\sqrt { 2 } }\\)
\nAnswer:
\n(C) \\(-2\\sqrt { 2 } \\)<\/p>\n

Question 2.
\nFour charge equals to -Q are placed at the four corners of a square and a charge q is at its centre. If the system is in equilibrium, the value of q is
\n\"2nd
\nAnswer:
\n(A)<\/p>\n

Question 3.
\nIf the amounts of electric flux entering and leaving an enclosed surface respectively are \\({ \\phi }_{ 1 }\\) and <\\({ \\phi }_{ 1 }\\) the electric charge inside the surface will be
\n\"2nd
\nAnswer:
\n(A)<\/p>\n

Question 4.
\nA charged particle q is placed at the centre O of the cube (ABCDEFGH) of length L. Another same charge q is placed at a distance L from 0. Then, the electric flux through ABCD is.
\n\"2nd
\nAnswer:
\n(C)<\/p>\n

Question 5.
\nA thin spherical shell of radius R has charge Q spread uniformly over its surface. Which of the following graphs most closely represents the electric field E (r) produced by the shell in the range o\u2264 r < \u221e where r is the distance from the centre of the shell ?
\n\"2nd
\n\"2nd
\nAnswer:
\n(B)<\/p>\n

Question 6.
\nTwo-point charge +8q and -2q are located at x = 0 and x = L respectively. The location of a point on z-axis at which the net electric field due to these two point charges is zero is (CET 2009)
\n(A) 2L
\n(B) L\/4
\n(C) 8L
\n(D) 4L
\nAnswer:
\n(D) 4L<\/p>\n

Question 7.
\nIf a charge q is placed at the centre of the line joining two equal charges Q such that the system is in equilibrium then the value of q is (CET 2010)
\n(A) Q\/2
\n(B) -Q\/2
\n(C) Q\/4
\n(D) -Q\/4.
\nAnswer:
\n(D) -Q\/4.<\/p>\n","protected":false},"excerpt":{"rendered":"

You can Download Chapter 1 Electric Charges and Fields Questions and Answers, Notes, 2nd PUC Physics Question Bank with Answers, Karnataka State Board Solutions help you to revise complete Syllabus and score more marks in your examinations. Karnataka 2nd PUC Physics Question Bank Chapter 1 Electric Charges and Fields 2nd PUC Physics Electric Charges and …<\/p>\n","protected":false},"author":5,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[82],"tags":[],"jetpack_sharing_enabled":true,"jetpack_featured_media_url":"","_links":{"self":[{"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/posts\/9851"}],"collection":[{"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/users\/5"}],"replies":[{"embeddable":true,"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/comments?post=9851"}],"version-history":[{"count":0,"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/posts\/9851\/revisions"}],"wp:attachment":[{"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/media?parent=9851"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/categories?post=9851"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/kseebsolutions.guru\/wp-json\/wp\/v2\/tags?post=9851"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}