Measurement of Electrical Parameters in Steam Turbine

As the generator is coupled with a steam turbine, we shall discuss the measurement of some Electrical parameters such as Voltage, Current, Power, Frequency, and Energy are the major parameters measured.

Voltage

  • The other names for voltage are Potential Difference, Electromotive Force (EMF), and pressure of an electrical circuit.
  • This voltage is measured with the help of a voltmeter.
  • Voltmeters are standard items on switchboards and control panels.
  • They are basically single-circuit elements therefore when three phases are to be indicated, either three instruments are used or one with a multipoint switch.
  • The voltmeter is connected across the line and is a high-impedance one.
  • The voltmeter ranges can be varied with high-value resistors connected in series; such resistors are called voltmeter multipliers.
  • For high voltages, the Potential Transformer (PT) is connected to the main line called the primary, and the voltmeter is connected to the secondary.
  • Voltmeters are normally of moving iron types.
  • Moving coil meters can also be used but in conjunction with rectifiers.
Measurement of Electrical Parameters in Steam Turbine

Current

  • The quantity of electrical current flowing through a circuit is measured by an ammeter.
  • The low-impedance ammeter is connected in series with the line.
  • Ammeters connected in parallel to the instruments are accommodated to various ranges with small value resistances.
  • For the measurement of a very large current, these current transformers are connected to the main lines called primary, and the instruments are connected to their secondary.
  • The Current Transformer (CT), is used to measure large currents.
  • Normally the power line itself is considered as primary windings of the current transformer.
  • The secondary windings are practically short-circuited by the measuring ammeters.
  • Current Transformers convert the current to be measured into conveniently measurable secondary current preserving values and phases in proportion.
  • Ammeters are almost identical to voltmeters, but for their input impedances and mode of connections.

Power (Active)

Single Phase Power Measurement
  • The power of a direct current (always active) can be found in one ammeter and one voltmeter.
  • Both voltage and current readings can be multiplied to get the required power.
  • D.C. power can be measured by an Electro-dynamic wattmeter with a voltage coil and current coil.
  • Instrument transformers are connected such that the voltage path is connected ahead of the current path.
  • For safety reasons, the secondary of both transformers are connected to a common earth.
  • Cosφ is the phase angle between the voltage and the current.
  • For an alternating current circuit, the active power is given by P= V*I*Cosφ
  • The active power for a 3φ phase system is the total of the three components.

For star connection, it is given by.

P = 3 Vp I cos φ

For delta connection, it is given by.

P= √3 VL I cos φ

Where

V = RMS values of voltage

I = RMS values of current

P = Total power

Cosφ = Power Factor

Vp = Phase to neutral Voltage

VL= Line Voltage

Some of the common methods used in power plants are

Three-wattmeter is the most accurate method with indications and mechanical adder having a common shaft.

Three-wattmeter Method (Three-phase three-wire system)

WR+WY+WB = (VRC * IR) + (VYC * IY) + (VBC * IB)

WR+WY+WB = (VRN * IR) + (VYN * IY) + (VBN * IB)

WR+WY+WB = PR +PY+ PB = Total Power

It is observed that the sum of the three individual wattmeter readings (WR+WY+WB) indicates the total power consumed by the load (PR +PY+ PB).

Three–Wattmeter Method (3φ 4-wire System)

WR+WY+WB   = (VRC * IR) + (VYC * IY) + (VBC * IB)

WR+WY+WB = (VRN * IR) + (VYN * IY) + (VBN * IB)

WR+WY+W= PR +PY+ PB

The total power consumed by load is given by the summation of three wattmeters.

Two Wattmeter Methods

  • This is the most commonly used method for measuring three-phase power.
  • It is useful for both balanced and unbalanced loads.
  • The sum of two watt-meter readings will be equal to the total power consumed as given below.
  • Power consumed by the load

P= VRN * IR + VYN * IY + VBN * IB

Summation of wattmeter readings

W = W1 + W2

W = (VRN -VYN)* IR + (VBN – VYN) * IB

W = (VRN * IR) +(VBN* IB) + VYN (-IR – IB)

By Kirchhoff’s law, we know that,  IR+IB+IY=0, or  IR -IB = IY

W1+W2= VRN * IR + VYN * IY  + VBN * IB = P

For delta connection load

P = VRB * IR + VYR * IY + VBY * IB

W₁ + W₂ = -VYR * (IR-IY) + VBY *(IB-IR)

P= VRB * IR + VYR * IY + VBY * IB

Where (VYR + VBY +VRB = 0)

It can be proved that the total power

W1 + W2= 3*V*I*cos φ

W1 – W2 =√3*V*I*sin φ

 Hence,

tanφ = √3*[(W1 – W2)/(W1 + W2)]

Power factor Cosφ = Cos [tan-1 {√3 ((W1 – W2)/ (W1 + W2))}]

Energy

Single Phase Energy Meter
  • In terms of watt-hour or kilowatt-hour (kWh).
  • The kWh is defined as the energy supplied or consumed at an average rate of 1 kilowatt for one hour.
  • In commercial metering, 1 kWh is called 1 unit of energy.
  • Energy meters are used for the measurement of energy.
  • Energy meters have moving systems that revolve continuously, it deflects only through a fraction of a revolution
  • In energy meters, the speed of revolution is proportional to the power and the total number of revolutions made by the meter moving system over a given period is proportional to the energy.
  • The most commonly used energy meters are Induction type instruments.
  • Such meters have lower friction and a higher torque/weight ratio.
  • These meters are inexpensive but accurate.
  • Constructional details of an induction type single phase energy meter are shown schematically in the Figure above
  • The operating system consists of two electromagnets.
  • The current coil is wound on the series magnet and the pressure coil is wound on the shunt magnet.
  • Shading bands made of copper are used to bring the flux produced by the shunt magnet exactly in quadrature with the applied voltage.
  • The moving system consists of a light aluminum disc mounted on a spindle.
  • The disc is placed in the space between the series and shunt magnets.
  • The disc is positioned such that it intersects the flux produced by both magnets.
  • The deflecting torque on the disc is produced by the interaction between these fluxes and the eddy current they induce in the disc.
  • As there is no control spring, continuous rotation is possible.
  • The braking system consists of a permanent magnet positioned near the edge of the aluminum disc whose position is adjustable.
  • When the braking torque becomes equal to the operating torque, the disc rotates at a steady speed.
  • A registering system consisting of a train of reduction gears makes counting in numerical value possible.

Frequency

  • Frequency meters are more convenient for most practical purposes.
  • These indicate the generated power frequency.
  • a vibrating reed frequency meter mainly consists of more thin steel strips called reeds arranged close electromagnet.
  • The electromagnet is laminated and its winding is connected, in series with a resistance, across the supply whose frequency is to be measured.
  • The external connection is the same as the voltmeter.
  • The reeds are made with slight differences in that their natural frequencies are different.
  • These reeds are arranged in ascending order of frequency from 47 cycles per second up to 53 cycles per second.
  • The natural frequency of the first reed is 47 cycles per second, and the next reed is 47½ cycles per second, and so on.
  • The magnetism of the electromagnet alternates with the supply frequency and exerts an attracting force when the meter is in use.
  • The one whose natural frequency is matching with the supply frequency will vibrate appreciably showing the supply frequency.
  • The flags at the top of the reeds are painted with the corresponding frequency so that one can read directly the frequency by observing the reed which is vibrating most.
  • A great advantage of this type of meter is that its indications are independent of the applied voltage and waveforms.
Don't Miss Our Updates
Be the first to get exclusive content straight to your email.
We promise not to spam you. You can unsubscribe at any time.
Invalid email address

Leave a Comment

Share via
Follow us and never miss an update!