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Page 1 CURRENT ELECTRICITY 1. ELECTRIC CURRENT I av = t q ? ? and instantaneous current i =. dt dq t q Lim 0 t ? ? ? ? ? 2. ELECTRIC CURRENT IN A CONDUCTOR I = nAeV . ? ? ? d v , ? ? ? ? ? ? ? ? ? 2 d m eE 2 1 v = ? m eE 2 1 , I = neA V d 3. CURRENT DENSITY n ds dI J ? ? ? 4. ELECTRICAL RESISTANCE I = neA V d = neA ? ? ? ? ? ? m 2 eE ? = ? ? ? ? ? ? ? ? ? m 2 ne 2 AE AE E = ? V so I = ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? A m 2 ne 2 V = ? ? ? ? ? ? ? ? ? ? A V = V/R ? V = IR ? is called resistivity (it is also called specific resistance) and ? ?= ? 2 ne m 2 = ? 1 , ? is called conductivity. Therefore current in conductors is proportional to potential difference applied across its ends. This is Ohm's Law. Units: ) m ( meter ohm ), ( ohm R ? ? ? ? ? ? ? also called siemens, 1 1 m ? ? ? ? ? . Page 2 CURRENT ELECTRICITY 1. ELECTRIC CURRENT I av = t q ? ? and instantaneous current i =. dt dq t q Lim 0 t ? ? ? ? ? 2. ELECTRIC CURRENT IN A CONDUCTOR I = nAeV . ? ? ? d v , ? ? ? ? ? ? ? ? ? 2 d m eE 2 1 v = ? m eE 2 1 , I = neA V d 3. CURRENT DENSITY n ds dI J ? ? ? 4. ELECTRICAL RESISTANCE I = neA V d = neA ? ? ? ? ? ? m 2 eE ? = ? ? ? ? ? ? ? ? ? m 2 ne 2 AE AE E = ? V so I = ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? A m 2 ne 2 V = ? ? ? ? ? ? ? ? ? ? A V = V/R ? V = IR ? is called resistivity (it is also called specific resistance) and ? ?= ? 2 ne m 2 = ? 1 , ? is called conductivity. Therefore current in conductors is proportional to potential difference applied across its ends. This is Ohm's Law. Units: ) m ( meter ohm ), ( ohm R ? ? ? ? ? ? ? also called siemens, 1 1 m ? ? ? ? ? . Dependence of Resistance on Temperature : R = R o (1 + ? ? ?). Electric current in resistance I = R V V 1 2 ? 5. ELECTRICAL POWER P = V ? ? Energy = ? pdt P = I 2 R = V ? = R V 2 . H = V ?t = ? 2 Rt = t R V 2 H = ? 2 RT Joule = 2 . 4 RT 2 ? Calorie 9. KIRCHHOFF'S LAWS 9.1 Kirchhoff’s Current Law (Junction law) ? ? in = ? ? ? out 9.2 Kirchhoff’s Voltage Law (Loop law) ? ?IR + ? ?EMF =0”. 10. COMBINATION OF RESISTANCES : Resistances in Series: R = R 1 + R 2 + R 3 +................ + R n (this means R eq is greater then any resistor) ) and V = V 1 + V 2 + V 3 +................ + V n . V 1 = V R ......... R R R n 2 1 1 ? ? ? ; V 2 = V R ......... R R R n 2 1 2 ? ? ? ; 2. Resistances in Parallel : Page 3 CURRENT ELECTRICITY 1. ELECTRIC CURRENT I av = t q ? ? and instantaneous current i =. dt dq t q Lim 0 t ? ? ? ? ? 2. ELECTRIC CURRENT IN A CONDUCTOR I = nAeV . ? ? ? d v , ? ? ? ? ? ? ? ? ? 2 d m eE 2 1 v = ? m eE 2 1 , I = neA V d 3. CURRENT DENSITY n ds dI J ? ? ? 4. ELECTRICAL RESISTANCE I = neA V d = neA ? ? ? ? ? ? m 2 eE ? = ? ? ? ? ? ? ? ? ? m 2 ne 2 AE AE E = ? V so I = ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? A m 2 ne 2 V = ? ? ? ? ? ? ? ? ? ? A V = V/R ? V = IR ? is called resistivity (it is also called specific resistance) and ? ?= ? 2 ne m 2 = ? 1 , ? is called conductivity. Therefore current in conductors is proportional to potential difference applied across its ends. This is Ohm's Law. Units: ) m ( meter ohm ), ( ohm R ? ? ? ? ? ? ? also called siemens, 1 1 m ? ? ? ? ? . Dependence of Resistance on Temperature : R = R o (1 + ? ? ?). Electric current in resistance I = R V V 1 2 ? 5. ELECTRICAL POWER P = V ? ? Energy = ? pdt P = I 2 R = V ? = R V 2 . H = V ?t = ? 2 Rt = t R V 2 H = ? 2 RT Joule = 2 . 4 RT 2 ? Calorie 9. KIRCHHOFF'S LAWS 9.1 Kirchhoff’s Current Law (Junction law) ? ? in = ? ? ? out 9.2 Kirchhoff’s Voltage Law (Loop law) ? ?IR + ? ?EMF =0”. 10. COMBINATION OF RESISTANCES : Resistances in Series: R = R 1 + R 2 + R 3 +................ + R n (this means R eq is greater then any resistor) ) and V = V 1 + V 2 + V 3 +................ + V n . V 1 = V R ......... R R R n 2 1 1 ? ? ? ; V 2 = V R ......... R R R n 2 1 2 ? ? ? ; 2. Resistances in Parallel : 11. WHEATSTONE NETWORK : (4 TERMINAL NETWORK) When current through the galvanometer is zero (null point or balance point) Q P = S R , then PS = QR 13. GROUPING OF CELLS 13.1 Cells in Series : ? Equivalent EMFE eq = E E ....... E n 1 2 ? ? ? [write EMF's with polarity] Equivalent internal resistance r eq = n 4 3 2 1 r .... r r r r ? ? ? ? ? 13.2 Cells in Parallel: n 2 1 n n 2 2 1 1 eq r 1 ..... r 1 r 1 r .... r r E ? ? ? ? ? ? ? ? ? ? [Use emf with polarity] n 2 1 eq r 1 .... r 1 r 1 r 1 ? ? ? ? 15. AMMETER A shunt (small resistance) is connected in parallel with galvanometer to convert it into ammeter. An ideal ammeter has zero resistance Page 4 CURRENT ELECTRICITY 1. ELECTRIC CURRENT I av = t q ? ? and instantaneous current i =. dt dq t q Lim 0 t ? ? ? ? ? 2. ELECTRIC CURRENT IN A CONDUCTOR I = nAeV . ? ? ? d v , ? ? ? ? ? ? ? ? ? 2 d m eE 2 1 v = ? m eE 2 1 , I = neA V d 3. CURRENT DENSITY n ds dI J ? ? ? 4. ELECTRICAL RESISTANCE I = neA V d = neA ? ? ? ? ? ? m 2 eE ? = ? ? ? ? ? ? ? ? ? m 2 ne 2 AE AE E = ? V so I = ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? A m 2 ne 2 V = ? ? ? ? ? ? ? ? ? ? A V = V/R ? V = IR ? is called resistivity (it is also called specific resistance) and ? ?= ? 2 ne m 2 = ? 1 , ? is called conductivity. Therefore current in conductors is proportional to potential difference applied across its ends. This is Ohm's Law. Units: ) m ( meter ohm ), ( ohm R ? ? ? ? ? ? ? also called siemens, 1 1 m ? ? ? ? ? . Dependence of Resistance on Temperature : R = R o (1 + ? ? ?). Electric current in resistance I = R V V 1 2 ? 5. ELECTRICAL POWER P = V ? ? Energy = ? pdt P = I 2 R = V ? = R V 2 . H = V ?t = ? 2 Rt = t R V 2 H = ? 2 RT Joule = 2 . 4 RT 2 ? Calorie 9. KIRCHHOFF'S LAWS 9.1 Kirchhoff’s Current Law (Junction law) ? ? in = ? ? ? out 9.2 Kirchhoff’s Voltage Law (Loop law) ? ?IR + ? ?EMF =0”. 10. COMBINATION OF RESISTANCES : Resistances in Series: R = R 1 + R 2 + R 3 +................ + R n (this means R eq is greater then any resistor) ) and V = V 1 + V 2 + V 3 +................ + V n . V 1 = V R ......... R R R n 2 1 1 ? ? ? ; V 2 = V R ......... R R R n 2 1 2 ? ? ? ; 2. Resistances in Parallel : 11. WHEATSTONE NETWORK : (4 TERMINAL NETWORK) When current through the galvanometer is zero (null point or balance point) Q P = S R , then PS = QR 13. GROUPING OF CELLS 13.1 Cells in Series : ? Equivalent EMFE eq = E E ....... E n 1 2 ? ? ? [write EMF's with polarity] Equivalent internal resistance r eq = n 4 3 2 1 r .... r r r r ? ? ? ? ? 13.2 Cells in Parallel: n 2 1 n n 2 2 1 1 eq r 1 ..... r 1 r 1 r .... r r E ? ? ? ? ? ? ? ? ? ? [Use emf with polarity] n 2 1 eq r 1 .... r 1 r 1 r 1 ? ? ? ? 15. AMMETER A shunt (small resistance) is connected in parallel with galvanometer to convert it into ammeter. An ideal ammeter has zero resistance Ammeter is represented as follows - If maximum value of current to be measured by ammeter is ? then I G . R G = (I – I G )S S = G G G R . ? ? ? ? S = ? ? ? G G R when ? >> ? G . where ? = Maximum current that can be measured using the given ammeter. 16. VOLTMETER A high resistance is put in series with galvanometer. It is used to measure potential difference across a resistor in a circuit. For maximum potential difference V = ? G . R S + ? G R G R S = G V ? – R G If R G << R S ? R S ? G V ? 17. POTENTIOMETER ? = R r ? ? V A – V B = r R ? ? .R Potential gradient (x) ? Potential difference per unit length of wire x = L V V B A ? = r R ? ? . L R Page 5 CURRENT ELECTRICITY 1. ELECTRIC CURRENT I av = t q ? ? and instantaneous current i =. dt dq t q Lim 0 t ? ? ? ? ? 2. ELECTRIC CURRENT IN A CONDUCTOR I = nAeV . ? ? ? d v , ? ? ? ? ? ? ? ? ? 2 d m eE 2 1 v = ? m eE 2 1 , I = neA V d 3. CURRENT DENSITY n ds dI J ? ? ? 4. ELECTRICAL RESISTANCE I = neA V d = neA ? ? ? ? ? ? m 2 eE ? = ? ? ? ? ? ? ? ? ? m 2 ne 2 AE AE E = ? V so I = ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? A m 2 ne 2 V = ? ? ? ? ? ? ? ? ? ? A V = V/R ? V = IR ? is called resistivity (it is also called specific resistance) and ? ?= ? 2 ne m 2 = ? 1 , ? is called conductivity. Therefore current in conductors is proportional to potential difference applied across its ends. This is Ohm's Law. Units: ) m ( meter ohm ), ( ohm R ? ? ? ? ? ? ? also called siemens, 1 1 m ? ? ? ? ? . Dependence of Resistance on Temperature : R = R o (1 + ? ? ?). Electric current in resistance I = R V V 1 2 ? 5. ELECTRICAL POWER P = V ? ? Energy = ? pdt P = I 2 R = V ? = R V 2 . H = V ?t = ? 2 Rt = t R V 2 H = ? 2 RT Joule = 2 . 4 RT 2 ? Calorie 9. KIRCHHOFF'S LAWS 9.1 Kirchhoff’s Current Law (Junction law) ? ? in = ? ? ? out 9.2 Kirchhoff’s Voltage Law (Loop law) ? ?IR + ? ?EMF =0”. 10. COMBINATION OF RESISTANCES : Resistances in Series: R = R 1 + R 2 + R 3 +................ + R n (this means R eq is greater then any resistor) ) and V = V 1 + V 2 + V 3 +................ + V n . V 1 = V R ......... R R R n 2 1 1 ? ? ? ; V 2 = V R ......... R R R n 2 1 2 ? ? ? ; 2. Resistances in Parallel : 11. WHEATSTONE NETWORK : (4 TERMINAL NETWORK) When current through the galvanometer is zero (null point or balance point) Q P = S R , then PS = QR 13. GROUPING OF CELLS 13.1 Cells in Series : ? Equivalent EMFE eq = E E ....... E n 1 2 ? ? ? [write EMF's with polarity] Equivalent internal resistance r eq = n 4 3 2 1 r .... r r r r ? ? ? ? ? 13.2 Cells in Parallel: n 2 1 n n 2 2 1 1 eq r 1 ..... r 1 r 1 r .... r r E ? ? ? ? ? ? ? ? ? ? [Use emf with polarity] n 2 1 eq r 1 .... r 1 r 1 r 1 ? ? ? ? 15. AMMETER A shunt (small resistance) is connected in parallel with galvanometer to convert it into ammeter. An ideal ammeter has zero resistance Ammeter is represented as follows - If maximum value of current to be measured by ammeter is ? then I G . R G = (I – I G )S S = G G G R . ? ? ? ? S = ? ? ? G G R when ? >> ? G . where ? = Maximum current that can be measured using the given ammeter. 16. VOLTMETER A high resistance is put in series with galvanometer. It is used to measure potential difference across a resistor in a circuit. For maximum potential difference V = ? G . R S + ? G R G R S = G V ? – R G If R G << R S ? R S ? G V ? 17. POTENTIOMETER ? = R r ? ? V A – V B = r R ? ? .R Potential gradient (x) ? Potential difference per unit length of wire x = L V V B A ? = r R ? ? . L R Application of potentiometer (a) To find emf of unknown cell and compare emf of two cells. In case ?, In figure (1) is joint to (2) then balance length = ? 1 ? 1 = x ? 1 ....(1) in case ? ?, In figure (3) is joint to (2) then balance length = ? 2 ? 2 = x ? 2 ....(2) 2 1 2 1 ? ? ? ? ? If any one of ? 1 or ? 2 is known the other can be found. If x is known then both ? 1 and ? 2 can be found (b) To find current if resistance is known V A – V C = x ? 1 IR 1 = x ? 1 ? = 1 1 R x ? Similarly, we can find the value of R 2 also. Potentiometer is ideal voltmeter because it does not draw any current from circuit, at the balance point. (c) To find the internal resistance of cell. I st arrangement 2 nd arrangementRead More
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