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Internal Resistance, EMF and Oscilloscopes
What we are going to achieve today ,[object Object],[object Object],[object Object],[object Object]
Using lemons, limes and potatoes to power an LED zinc copper
Making Batteries There is nothing special about batteries – but these have a high internal resistance. R l What do you think the best way to minimise the internal resistance of your battery? Think about resistivity (lemon is a poor conductor)
Batteries What is the main energy transfer in a battery?  Electrical energy This is powered by two 1.5 V AA cells in series - what is the supply voltage? What is the emf of the supply? After a while the battery needs to be replaced; why? What determines how quickly it runs down? What determines how much current is drawn from the supply?
EMF Electromotive Force ,[object Object],[object Object],[object Object]
Batteries have internal resistance The circuit now has two resistors in The internal resistance of the battery, r is very small. R is much larger The total resistance of this circuit is  R total  = R +r I = E / (R+r)
Batteries have internal resistance As charge goes around the circuit the sum of emfs must equal the sum of voltage drops leading to EMF = I R + I r The terminal voltage is equal to I R so this can be rearranged to give: V = E – I r and interpreted as terminal voltage = emf – ‘lost volts’
R -small R total  = r + R  -small The current will now be larger as the total resistance of the circuit is much lower The voltage lost across r  V = I (large) r The voltage lost will now be a problem This case is of a small load resistance connected to a battery is seen in a starter motor on a car http://www.youtube.com/watch?v=al6Yz3Nv7dY http://www.youtube.com/watch?v=Ut7yBdIehYY&NR=1
Starter motor on a conventional car The headlamps are connected in parallel across a twelve-volt battery.  The starter motor is also in parallel controlled by the ignition switch. Since the starter motor has a very low resistance it demands a very high current (say 60 A).  The battery itself has a low internal resistance (say 0.01 Ω).  The headlamps themselves draw a much lower current (they have a higher resistance) Lamp R   Starter motor Ignition switch 12V What will happen to the lights?
A use of high internal resistance
Quick Questions ,[object Object],[object Object],[object Object],[object Object],[object Object],V = E – I r  V = IR E = I(R +r) You need to set up a simultaneous equation
Answers 1. (a) pd = E – I r = 9 – (50 x 10 -3  x 12) = 8.4 V (b) Max current = E/r = 9 / 12 = 0.75 A 2. E = I(R +r) E = 25 x 10 -3  (400 + r)  and  E = 60 x 10 -3  (100 + r) So 25 x 10 -3  (400 + r) = 60 x 10 -3  (100 + r) so r = 114.3   E = 10 + (25 x 10 -3  x 114.3) = 12.86 V I V
Oscilloscope Use the signal generator to create A/C (alternating current) on the Oscilloscope Draw 2 signals of 2 different frequencies  Work out the frequency of the  Oscilloscope  Add the magnitude of the wave height How do you use an oscilloscope  as a dc and ac voltmeter? How do you use it to measure frequency?
Voltage what the average value of an ac voltage or current is over a whole number of cycles? power is calculated by  P = IV , both I and V change sign together, so power is always positive
Positive power calling the maximum value of I  p  V p  and a minimum of zero 0V P = I  p  V p Average power = ½ I  p  V p P =  1/2 I  p V  p  =  1/2 I  p   2  R  =  1/2 V  p   2  / R          (using V = I R)
RMS voltage (root mean squared) RMS links the  dc  equivalent values to  ac  peak values.  The point is that a sinusoidal ac supply of peak value V p  delivers the  same average power  as steady dc of value V p  / √2 The same power would be delivered by a  dc  with values I and V if:   P = I 2 R= 1/2 I  p   2  R                  and                     P = V  2  / R = 1/2 V p   2  / R   I 2 R= 1/2 I  p   2  R  (divide both sides by R)   V  2  / R = 1/2 V p   2  / R  (multiply by R) These lead to the equations:   I 2  = I  p   2  / 2   V  2  = V  p   2  / 2  (square root) I = I p  / √2          V = V p  / √2
RMS Graph listed voltages for power outlets, e.g. 120 V (USA) or 230 V (Europe), are almost always quoted in RMS values, and not peak values
Questions ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],V p  =r.m.s x √ 2  Wavelength = 1 / frequency
Answers and Worked Solutions 1. (a) 110 x √ 2 = 155.6 V  (b)  2 x 155.6 = 311 V (c) 1 / 50 Hz = 0.02s (d)  P = V 2  /R  R = 12100/100 = 121    2.  12 V peak ac is equivalent to 12/√ 2  V = 8.5 V dc equivalent.  So 12 V peak to peak is dimmer. 3. 230 x √ 2  V = 325V, so graph varies between + 325 V and -325 V.  One time period = 1 / 50 Hz = 0.02s 4.  P = V 2  /R  so the ratio of powers is ratio of voltages squared.  20 V peak ac is equivalent to 20/ √ 2 V dc  i.e. 14.14 V so dc power / ac power = 20 2  /14.14 2  = 2  or  dc V 2  / (ac peak / √ 2) 2  = (√ 2) 2  =2

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Internal Resistance, EMF and Oscilloscopes.ppt

  • 1. Internal Resistance, EMF and Oscilloscopes
  • 2.
  • 3. Using lemons, limes and potatoes to power an LED zinc copper
  • 4. Making Batteries There is nothing special about batteries – but these have a high internal resistance. R l What do you think the best way to minimise the internal resistance of your battery? Think about resistivity (lemon is a poor conductor)
  • 5. Batteries What is the main energy transfer in a battery? Electrical energy This is powered by two 1.5 V AA cells in series - what is the supply voltage? What is the emf of the supply? After a while the battery needs to be replaced; why? What determines how quickly it runs down? What determines how much current is drawn from the supply?
  • 6.
  • 7. Batteries have internal resistance The circuit now has two resistors in The internal resistance of the battery, r is very small. R is much larger The total resistance of this circuit is R total = R +r I = E / (R+r)
  • 8. Batteries have internal resistance As charge goes around the circuit the sum of emfs must equal the sum of voltage drops leading to EMF = I R + I r The terminal voltage is equal to I R so this can be rearranged to give: V = E – I r and interpreted as terminal voltage = emf – ‘lost volts’
  • 9. R -small R total = r + R -small The current will now be larger as the total resistance of the circuit is much lower The voltage lost across r V = I (large) r The voltage lost will now be a problem This case is of a small load resistance connected to a battery is seen in a starter motor on a car http://www.youtube.com/watch?v=al6Yz3Nv7dY http://www.youtube.com/watch?v=Ut7yBdIehYY&NR=1
  • 10. Starter motor on a conventional car The headlamps are connected in parallel across a twelve-volt battery. The starter motor is also in parallel controlled by the ignition switch. Since the starter motor has a very low resistance it demands a very high current (say 60 A). The battery itself has a low internal resistance (say 0.01 Ω). The headlamps themselves draw a much lower current (they have a higher resistance) Lamp R Starter motor Ignition switch 12V What will happen to the lights?
  • 11. A use of high internal resistance
  • 12.
  • 13. Answers 1. (a) pd = E – I r = 9 – (50 x 10 -3 x 12) = 8.4 V (b) Max current = E/r = 9 / 12 = 0.75 A 2. E = I(R +r) E = 25 x 10 -3 (400 + r) and E = 60 x 10 -3 (100 + r) So 25 x 10 -3 (400 + r) = 60 x 10 -3 (100 + r) so r = 114.3  E = 10 + (25 x 10 -3 x 114.3) = 12.86 V I V
  • 14. Oscilloscope Use the signal generator to create A/C (alternating current) on the Oscilloscope Draw 2 signals of 2 different frequencies Work out the frequency of the Oscilloscope Add the magnitude of the wave height How do you use an oscilloscope as a dc and ac voltmeter? How do you use it to measure frequency?
  • 15. Voltage what the average value of an ac voltage or current is over a whole number of cycles? power is calculated by  P = IV , both I and V change sign together, so power is always positive
  • 16. Positive power calling the maximum value of I  p V p  and a minimum of zero 0V P = I  p V p Average power = ½ I  p V p P = 1/2 I  p V  p  = 1/2 I  p   2  R = 1/2 V  p   2  / R         (using V = I R)
  • 17. RMS voltage (root mean squared) RMS links the dc equivalent values to ac peak values. The point is that a sinusoidal ac supply of peak value V p  delivers the  same average power  as steady dc of value V p  / √2 The same power would be delivered by a dc with values I and V if:   P = I 2 R= 1/2 I  p   2  R                  and                     P = V  2  / R = 1/2 V p   2  / R   I 2 R= 1/2 I  p   2  R (divide both sides by R) V  2  / R = 1/2 V p   2  / R (multiply by R) These lead to the equations:   I 2  = I  p   2  / 2 V  2  = V  p   2  / 2 (square root) I = I p  / √2         V = V p  / √2
  • 18. RMS Graph listed voltages for power outlets, e.g. 120 V (USA) or 230 V (Europe), are almost always quoted in RMS values, and not peak values
  • 19.
  • 20. Answers and Worked Solutions 1. (a) 110 x √ 2 = 155.6 V (b) 2 x 155.6 = 311 V (c) 1 / 50 Hz = 0.02s (d) P = V 2 /R R = 12100/100 = 121  2. 12 V peak ac is equivalent to 12/√ 2 V = 8.5 V dc equivalent. So 12 V peak to peak is dimmer. 3. 230 x √ 2 V = 325V, so graph varies between + 325 V and -325 V. One time period = 1 / 50 Hz = 0.02s 4. P = V 2 /R so the ratio of powers is ratio of voltages squared. 20 V peak ac is equivalent to 20/ √ 2 V dc i.e. 14.14 V so dc power / ac power = 20 2 /14.14 2 = 2 or dc V 2 / (ac peak / √ 2) 2 = (√ 2) 2 =2