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6.1 Alternating current and power
AC is used for power distribution because the peak voltage can be easily changed using transformers * An AC repeatedly reverses its direction * In one cycle the charge carriers move in one direction then the other. AC measurements * Mains frequency is 50 Hz , one cycle lasts 1/50 sec = sec = time period T Frequency: f (Hz) f = 1 T Peak value Peak to peak value
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6.1 Alternating current and power
AC is used for power distribution because the peak voltage can be easily changed using transformers * An AC repeatedly reverses its direction * In one cycle the charge carriers move in one direction then the other. AC measurements * Mains frequency is 50 Hz , one cycle lasts 1/50 sec = sec = time period T Frequency: f (Hz) f = 1 T Peak value Peak to peak value
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6.1 Alternating current and power
AC is used for power distribution because the peak voltage can be easily changed using transformers * An AC repeatedly reverses its direction * In one cycle the charge carriers move in one direction then the other. AC measurements * Mains frequency is 50 Hz , Frequency: f (Hz) Peak value Peak to peak value
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6.1 Alternating current and power
AC is used for power distribution because the peak voltage can be easily changed using transformers * An AC repeatedly reverses its direction * In one cycle the charge carriers move in one direction then the other. AC measurements * Mains frequency is 50 Hz , Frequency: f (Hz)
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6.1 Alternating current and power
AC is used for power distribution because the peak voltage can be easily changed using transformers * An AC repeatedly reverses its direction * In one cycle the charge carriers move in one direction then the other. AC measurements * Mains frequency is 50 Hz , Frequency: f (Hz) Peak value
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6.1 Alternating current and power
AC is used for power distribution because the peak voltage can be easily changed using transformers * An AC repeatedly reverses its direction * In one cycle the charge carriers move in one direction then the other. AC measurements * Mains frequency is 50 Hz , Frequency: f (Hz) Peak value Peak to peak value
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6.1 Alternating current and power
* Mains frequency is 50 Hz , one cycle lasts 1/50 sec = sec = time period T One cycle f = 1 T Peak value Peak to peak value
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P = I V = I2R R = resistance of heater
6.1 Alternating current and power The heating effect of an alternating current: varies according to the square of the current P = I V = I2R R = resistance of heater At peak current Io maximum power is supplied = Io2 R At zero current zero power is supplied Equal areas above and below mean value also Av value of a sin 2 plot = 1/2 Mean power supplied = ½ Io2 R
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P = I V = I2R R = resistance of heater
6.1 Alternating current and power The heating effect of an alternating current: varies according to the square of the current P = I V = I2R R = resistance of heater At peak current Io maximum power is supplied = Io2 R At zero current zero power is supplied Equal areas above and below mean value also Av value of a sin 2 plot = 1/2 Mean power supplied = ½ Io2 R
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P = I V = I2R R = resistance of heater
6.1 Alternating current and power The heating effect of an alternating current: varies according to the square of the current P = I V = I2R R = resistance of heater At peak current Io maximum power is supplied = Io2 R At zero current zero power is supplied Equal areas above and below mean value also Av value of a sin 2 plot = 1/2 Mean power supplied = ½ Io2 R
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P = I V = I2R R = resistance of heater
6.1 Alternating current and power The heating effect of an alternating current: varies according to the square of the current P = I V = I2R R = resistance of heater At peak current Io maximum power is supplied = Io2 R At zero current zero power is supplied Equal areas above and below mean value also Av value of a sin 2 plot = 1/2 Mean power supplied = ½ Io2 R
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P = I V = I2R R = resistance of heater
6.1 Alternating current and power The heating effect of an alternating current: varies according to the square of the current P = I V = I2R R = resistance of heater At peak current Io maximum power is supplied = Io2 R At zero current zero power is supplied Equal areas above and below mean value Mean power supplied = ½ Io2 R
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P = I V = I2R R = resistance of heater
6.1 Alternating current and power The heating effect of an alternating current: varies according to the square of the current P = I V = I2R R = resistance of heater At peak current Io maximum power is supplied = Io2 R At zero current zero power is supplied Equal areas above and below mean value also Av value of a sin 2 plot = 1/2 Mean power supplied = ½ Io2 R
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6.1 Alternating current and power
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6.1 Alternating current and power
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6.1 Alternating current and power
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6.1 Alternating current and power
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6.1 Alternating current and power
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6.1 Alternating current and power
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The mean power supplied to a resistor:
6.1 Alternating current and power The mean power supplied to a resistor:
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The mean power supplied to a resistor:
6.1 Alternating current and power The mean power supplied to a resistor:
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6.1 Alternating current and power
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6.1 Alternating current and power
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