Semblance analysis

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The open-circuit test, or "no-load test", is one of the methods used in electrical engineering to determine the no-load impedance in the excitation branch of a transformer.

Circuit diagram for open-circuit test
Circuit diagram for open-circuit test

Method

The secondary of the transformer is left open-circuited. A wattmeter is connected to the primary. An ammeter is connected in series with the primary winding. A voltmeter is optional since the applied voltage is the same as the voltmeter reading. Rated voltage is applied at primary.

If the applied voltage is normal voltage then normal flux will be set up. Since iron loss is a function of applied voltage, normal iron loss will occur. Hence the iron loss is maximum at rated voltage. This maximum iron loss is measured using the wattmeter. Since the impedance of the series winding of the transformer is very small compared to that of the excitation branch, all of the input voltage is dropped across the excitation branch. Thus the wattmeter measures only the iron loss. This test only measures the combined iron losses consisting of the hysteresis loss and the eddy current loss. Although the hysteresis loss is less than the eddy current loss, it is not negligible. The two losses can be separated by driving the transformer from a variable frequency source since the hysteresis loss varies linearly with supply frequency and the eddy current loss varies with the square.

Since the secondary of the transformer is open, the primary draws only no-load current, which will have some copper loss. This no-load current is very small and because the copper loss in the primary is proportional to the square of this current, it is negligible. There is no copper loss in the secondary because there is no secondary current.

Current, voltage and power are measured at the primary winding to ascertain the admittance and power-factor angle.

Another method of determining the series impedance of a real transformer is the short circuit test.

Calculations

The current I0 is very small.

If W is the wattmeter reading then,


W=V1I0cosϕ0

That equation can be rewritten as,

cosϕ0=WV1I0

Thus,

Im=I0sinϕ0
Iw=I0cosϕ0

Impedance

By using the above equations, X0 and R0 can be calculated as,

X0=V1Im


R0=V1Iw

Thus,

Z0=R02+X02

or

Z0=R0+jX0

Admittance

The admittance is the inverse of impedance. Therefore,

Y0=1Z0

The conductance G0 can be calculated as,

G0=WV12

Hence the susceptance,

B0=Y02G02

or

Y0=G0+jB0


Here,

W is the wattmeter reading

V1 is the applied rated voltage

I0 is the no-load current

Im is the magnetizing component of no-load current

Iw is the core loss component of no-load current

Z0 is the exciting impedance

Y0 is the exciting admittance

References

  • 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

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  • 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

    My blog: http://www.primaboinca.com/view_profile.php?userid=5889534
  • 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

    My blog: http://www.primaboinca.com/view_profile.php?userid=5889534

See also