Hi again,
Short-circuit test:
The short circuit test in which the secondary is short circuited provides information about winding loss and voltage regulation of the secondary.
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On the other hand, the core loss is negligibly small, since the applied voltage and therefore the flux are only about one-twentieth to one-thirtieth of the rated voltage and flux, and the core loss is approximately proportional to the square of the flux. Hence the power registered on wattmeter W can be taken as the I 2R loss in the windings."
Source:
https://www.electro-tech-online.com/attachments/transformer_open_short_circuit-jpg.122039/
Question:
How can the power registered on wattmeter W be taken as the I²R loss in the winding
s. It could only be taken as the loss in primary winding. Yes, the wattmeter reading would give us the loss in windings only when the reading is multiplied by "2". Could you please help me? Thank you.
Note to self:
Open-circuit test:
The open circuit provides information on core loss. The terms core loss and iron loss mean the same. There are three core losses: eddy current losses, hysteresis losses, and anomalous losses. (Source:
https://en.wikipedia.org/wiki/Magnetic_core#Core_loss)
Suppose when no load is connected or open-circuit transformer test shows that 9 watt is core loss at 120 V.
Magnetizing current is the term used to denote the total current that flows into the primary of a transformer when the transformer is energized at a specific voltage and frequency, with the secondary open circuited. Although known as magnetizing current it is actually the combination of the current required to magnetize the core (I1) and the current required to supply the losses in the core (I2). (Source: **broken link removed**)
The wattmeter reading shows real power dissipated and that's the core loss. The voltmeter and ammeter give RMS values for voltage and current respectively.
Irms is magnetizing current. It contributes toward real power (i.e. core loss) and reactive power. Real power is converted into work done while reactive power shuffles between the source and load every half cycle.
It can be written that: real power = Vrms*Irms*pf where pf = cos(θv-θi). Therefore, pf=(wattmeter_reading)/(Vrms*Irms), so θv-θi=cos⁻¹(pf)
In an ideal case, core loss would be zero and all power would be reactive for open circuit test because primary is just an inductor and current lags voltage by 90 degrees.
Short-circuit test:
(insert question statement here)
Think like this. In case of a short-circuit test a small AC voltage is applied across the primary winding which is nothing more than inductor. Suppose you apply a small voltage across primary but the secondary is still an open circuit. Only a small voltage would be induced across the secondary and wattmeter reading would be really small because the current in an inductor is I=V/jωL and as 'V' is smaller therefore only a small current would flow.
An inductor resists the flow of current as a result of self-inductance which generates an opposing voltage across its terminals, or informally you can say in order for the current to increase in an inductor, it needs to push against the already present magnetic field around the inductor.
Now when the secondary is short circuited, a huge current flows through the secondary. The current in the secondary generates opposing flux to the primary flux and it results into reduction of voltage across the primary. As the primary voltage reduces, more current flows through primary which means primary voltage once again goes back to its value as the supply voltage. During short circuit test maximum rated current should flow through the primary which means the supply should be able to provide full load current.
Informally, when the secondary is open circuit, a certain amount of current flows through primary. When a load is connected to the secondary, an additional amount of current flows through primary to provide power to the load. How is power transferred from primary to the secondary? Suppose 120 V is connected to the primary and the load connected to secondary consumes 1A at 120 V but initially the secondary side circuit is open. The voltage across secondary would be same as the primary, i.e. 120 V. As soon as the switch is turned on and the current starts flowing through load, the voltage across secondary would go down temporarily but at the same time the flow of current through secondary generates its own flux which runs opposite to that of the primary. This counter flux reduces the net self inductance of primary and as a result more current starts flowing through the primary. This increase in current generates more flux and this flux induces more voltage in the secondary. This would go on until the current has reached its maximum value, 1A, through the load. Actually current in the primary generates flux and this flux gets 'converted' into voltage on the secondary side. The counter flux generated by secondary makes the primary to supply the required power although the flux generated by primary as result of turning on load and counter flux generated by secondary results into net zero flux.
Source:
https://electronics.stackexchange.c...rmer-why-is-the-excitation-branch-in-parallel
Helpful links:
1:
https://www.quora.com/What-is-magnetization-current-of-transformer
2:
https://circuitglobe.com/low-power-factor-wattmeter.html
3:
https://www.quora.com/Why-core-loss-is-constant-in-a-transformer