# Losses in Alternator – Power Stages & Efficiency of Synchronous Generator

### Losses in Synchronous Generator – Power Stages & Efficiency of Alternator

An alternator (synchronous generator) and synchronous motor is the same machine except the different power flow stages and as a matter of applications. In short, if the machine converts electrical power into mechanical power, it is known to be a synchronous generator (alternator). If the same machine is used to convert electrical energy into mechanical energy, it is known to be a synchronous motor. The same is the case for losses in synchronous motor and generator as follows.

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**Losses in Alternator**

The are different types of losses that occur in an alternator. All these losses can be classified into.

**Electrical Losses****Magnetic Losses****Mechanical Losses**

**Electrical Losses**

The electrical losses also known as the **copper losses** are the most prominent losses in an alternator. It depends on the amount of current passing through a conductor and its resistance. It is usually known as I^{2}R losses. it occurs in both the stator and rotor of the alternator as mentioned below.

**Stator Loss:** It occurs due to the armature winding resistance and the induced current in the stator. Since the armature current is large, this loss is significant given by

P_{Stator_loss }= (I_{Stator})^{2} (R_{Stator})

Where

- P
_{Stator_loss }= power loss in stator - I
_{Stator}= current induced in stator (armature winding) - R
_{Stator}= resistance of stator (armature winding)

**Rotor Loss: **this loss is relatively very smaller than stator loss due to a small DC rotor current. It is given by

P_{Rotor_loss} = (I_{Rotor})^{2} (R_{Rotor})

Where

- P
_{Rotor_loss}= Power loss in rotor - I
_{Rotor}= Current induced in rotor (field winding) - R
_{Rotor}= Resistance of rotor (field winding)

Similarly, the copper I^{2}R losses occur in the other parts of the alternator relatively in a small amount such as

**Brushes Loss**

P_{Brush_loss} = (I_{Rotor})^{2} (R_{Brush})

**Diode Rectifier Loss**

P_{Diode_loss} = I_{Diode} V_{d}

**Regulator Loss**

P_{Regulator_loss} = I_{Rotor} V_{d}

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**Magnetic Losses**

The magnetic losses are also known as **core losses or iron losses**. These losses occur in the core of the alternator due to the magnetic property of the material. These losses are classified into two types

- Hysteresis loss
- Eddy current loss

Magnetic Losses = P_{Hys }+ P_{Eddy}

**Hysteresis Loss:** it occurs due to the magnetization and demagnetization of the ferromagnetic core due to changing magnetic field. A ferromagnetic material does not have the ability to suddenly reverses its magnetization. During a magnetic reversal, it gradually demagnetizes. However, the applied magnetic field changes rapidly. A chunk of applied power is used in the demagnetization of the core. This is known as hysteresis loss given by

P_{Hys }= η B_{Max}^{1.6 }*f*V

Where

- P
_{Hys}= Hysteresis losses - η = Hysteresis coefficient
- B
_{Max}= Maximum flux density *f*= Supply frequency- V = Volume of the magnetic material

**Eddy Current Loss:** Eddy current loss occurs due to the current induced in the core of the alternator. As we know, a varying magnetic field induces a current in a conductor and the core is made of iron which is a good conductor. The induced current is called Eddy current that circulates in the core and opposes the induced voltage thus wasting the power in the form of heat known as Eddy current loss. It is given by

P_{Eddy} = k_{e} B^{2} *f*^{2}t^{2}V

Where

- P
_{Eddy}= Eddy current losses - K
_{e}= Eddy current coefficient - B
_{Max}= Maximum flux density *f*= Supply frequency- t = Thickness of lamination
- V = Volume of the magnetic material

The Eddy current loss is reduced by laminating the core. The core is designed of thin sheets with lamination between them to reduce the induce (Eddy) current.

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**Mechanical Losses**

The mechanical losses occur due to the moving parts of the alternator. These are constant losses as the rotor speed is constant in a synchronous generator. There are two types of mechanical losses in an alternator

**Friction Losses:** In the alternator, friction losses occur in the bearings due to the friction between the rotating part and stationery body. It is given by

P_{Friction }= k N

Where ‘k’ is constant and ‘N’ is the speed in RPM

**Windage Losses:** the windage losses occur due to the friction between the rotating parts and air. It is given by

P_{Windage} = k N^{3}

Windage losses increase with the cube of speed and also depend on the design of the rotor. A salient pole rotor has higher windage losses due to its protruding poles. Therefore speed is taken into account while designing the rotor.

**Stray Losses:** stray losses are the miscellaneous small losses that occur in an alternator due to various reasons but they cannot be easily accounted for such as flux distortion, non-uniform current distribution in the armature, etc. It is taken as 1% or 0.01 of the total losses.

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**Efficiency of Alternator**

The efficiency of an alternator is the ratio of output electrical power P_{out} to the input mechanical power P_{in}. It is given by

Efficiency, η = P_{Out }÷ P_{in}

Efficiency, η = P_{Out} ÷ (P_{Out }+ P_{Losses})

% Efficiency, η = P_{Out} ÷ (P_{Out} + P_{Losses}) x 100%

The alternator efficiency is inversely proportional to the losses. Where the losses depend on the speed as well as the load current. For a specific alternator, its efficiency only depends on the load current as the speed is constant. An alternator can have a maximum efficiency of around 80%.

The following fig shows the power stages in an Alternator (Power flow of a Synchronous Generator).

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**Expression for Alternator Efficiency**

Here is the expression for efficiency of the 3-phase alternator

Efficiency, η = P_{Out} ÷ (P_{out} + P_{Losses})

Its output power is given by

P_{Out }= 3VI_{a} cosθ

Where

- V = voltage per phase
- I
_{a }= armature current per phase - Cosθ = power factor

Where the power losses can be classified as variable and constant losses.

P_{Losses }= P_{Variable }+ P_{Constant}

The variable losses depend on the load current such as copper losses while the constant losses only depend on speed which is constant in a synchronous generator. Therefore

P_{ Variable }= 3I_{a}^{2}R_{a}

The field winding losses and the mechanical losses are constant given by.

P_{Constant }= P_{Rotor }+ P_{Mechanical }+ P_{Misc}

P_{c }= I_{f}^{2}R + P_{Hys }+ P_{Eddy }+ P_{Misc}

Therefore the total power losses become

P_{Losses} = 3I_{a}^{2}R_{a} + P_{c}

Hence the expression for the efficiency of an alternator becomes

η = P_{Out} ÷ (P_{Out} + P_{Losses})

η = 3VI_{a}cosθ ÷ (3VI_{a}cosθ +3I_{a}^{2}R_{a} + P_{c})

**Condition for Maximum Efficiency**

The efficiency of an alternator will be maximum when its variable losses become equal to the constant losses.

P_{Variable }= P_{c}

3I_{a}^{2}R_{a} = P_{c}

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