Презентация Battery. Direct and Alternating current онлайн

Содержание слайда: Republic of Kazakhstan Republic of Kazakhstan Ministry of Education and Science Kazakh-British Technical University Faculty of Power and Oil and Gas Industry Physical Engineering Department Physics 1 Voronkov Vladimir Vasilyevich

Содержание слайда: Battery The emf of a battery is the maximum possible voltage that the battery can provide between its terminals. Because a real battery is made of matter, there is resistance to the current within the battery. This resistance is called internal resistance r.

Содержание слайда: Direct and Alternating current There exist two types of current: Direct current (dc) is the continuous flow of charge in only one direction. The whole lecture is devoted only to direct current circuits. Alternating current (ac) is a flow of charge continually changing in both magnitude and in direction.

Содержание слайда: Vb-Va: V=  - IR Vb-Va: V=  - IR Circuit current: I= /(R+r) Power output of the battery is *I: *I = I2R + I2r

Содержание слайда: Energy output of a Battery *I = I2R + I2r *I - Power output of the battery. I2R – energy transferred to the external load I2r – energy loss by the internal resistance So the power output of the battery to external resistance is accompanied by the power loss due to internal resistance.

Содержание слайда: Resistor Resistor is a circuit element which is used to control the current level in the various parts of the circuit. It’s main property – it has constant resistivity for a wide range of potential differences.

Содержание слайда: Resistors in Series Iac=I1=I2 Vac=V1 + V2 Rac=R1 + R2

Содержание слайда: Resistors in Parallel I=I1+I2 Vac=V1=V2

Содержание слайда: Any number of resistors In series: I=I1=I2=I3=… V=V1 + V2 + V3 + … Rac=R1 + R2 + R3 + … In parallel: I=I1 + I2 + I3+ … V=V1 = V2 = V3 = …

Содержание слайда: Kirchhoff’s Rules for Direct Current Circuits Junction rule. The sum of the currents entering any junction in a circuit must equal the sum of the currents leaving that junction. Loop rule. The sum of the potential differences across all elements around any closed circuit loop must be zero.

Содержание слайда: Junction Rule I1= I2 + I3 The Kirchhoff’s junction rule is an analogue for fluid current. The junction rule is a consequence of the Charge conservation law.

Содержание слайда: Loop Rule Basis Kirchhoff’s second rule follows from the law of conservation of energy. Let us imagine moving a charge around a closed loop of a circuit. When the charge returns to the starting point, the charge –circuit system must have the same total energy as it had before the charge was moved. The sum of the increases in energy as the charge passes through some circuit elements must equal the sum of the decreases in energy as it passes through other elements. The potential energy decreases whenever the charge moves through a potential drop -IR across a resistor or whenever it moves in the reverse direction through a source of emf. The potential energy increases whenever the charge passes through a battery from the negative terminal to the positive terminal.

Содержание слайда: Loop rule If a resistor is traversed in the direction of the current, the potential difference across the resistor –IR. (Fig. a) If a resistor is traversed in the direction opposite the current, the potential differ- difference the resistor is +IR. (Fig. b) If a source of emf (assumed to have zero internal resistance) is traversed in the direction of the emf (from - to +), the potential difference is + . The emf of the battery increases the electric potential as we move through it in this direction. (Fig. c) If a source of emf (assumed to have zero internal resistance) is traversed in the direction opposite the emf (from + to - ), the potential difference - . In this case the emf of the batter battery reduces the electric potential as we move through it. (Fig. c)

Содержание слайда: Kirchhoff’s rules validity Kirchhoff’s rules are valid only for steady-state conditions - that is, the currents in various branches are constant. Any capacitor acts as an open branch in a circuit; that is, the current in the branch containing the capacitor is zero under steady-state conditions.

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Содержание слайда: Example: a multiloop circuit Given: All currents are steady state, I3=50mA, =6V, R1=100 , R2= 80 , C=2F. Find: I1, I2, R3, VC. VC is the capacitor’s voltage

Содержание слайда: I3=50mA, I3=50mA, =6V, R1=100 , R2= 80 , C=2F. I1, I2, R3, VC= ?

Содержание слайда: Units in Si Capacitance C F=C/V Current I A=C/s Resistance R Ohm=V/A Electro motive force (emf)  V