For a single phase, two winding transformer, the supply frequency and voltage are both increased by 10%. The percentage changes in the hysteresis loss and eddy current loss, respectively, are
10 and 21
This solution explains how changes in supply voltage and frequency affect the hysteresis and eddy current losses in a single-phase transformer. We are given that both the supply voltage and frequency are increased by 10%.
Hysteresis loss ($P_h$) occurs due to the magnetic hysteresis effect in the transformer core. It represents the energy lost as the magnetic domains within the core material are repeatedly rearranged due to the alternating magnetic field.
The formula for hysteresis loss is generally given by:
$$ P_h \propto f \cdot B_{max}^{x} $$
where:
Eddy current loss ($P_e$) is caused by circulating currents (eddy currents) induced within the transformer core by the changing magnetic flux. These currents flow through the resistance of the core material, generating heat and causing energy loss.
The formula for eddy current loss is:
$$ P_e \propto f^2 \cdot B_{max}^{2} $$
where the symbols have the same meaning as above.
In a transformer, the induced voltage ($V$) is directly proportional to the rate of change of flux, and the maximum flux ($ \Phi_{max}$) is related to the supply voltage ($V$) and frequency ($f$) by the following relationship:
$$ V \propto f \cdot \Phi_{max} $$
The maximum magnetic flux density ($B_{max}$) is proportional to the maximum flux ($ \Phi_{max}$):
$$ B_{max} \propto \Phi_{max} $$
Combining these, we get:
$$ B_{max} \propto \frac{V}{f} $$
Now, let's consider the given changes:
Let's calculate the new maximum flux density ($B'_{max}$):
$$ B'_{max} \propto \frac{V'}{f'} = \frac{1.10V}{1.10f} = \frac{V}{f} $$
This shows that $B'_{max} = B_{max}$. The maximum flux density remains unchanged when both voltage and frequency are increased by the same percentage.
We know $P_h \propto f \cdot B_{max}^{x}$. Let the original loss be $P_{h,old}$ and the new loss be $P_{h,new}$.
$$ \frac{P_{h,new}}{P_{h,old}} = \frac{f' \cdot (B'_{max})^{x}}{f \cdot B_{max}^{x}} $$
Since $f' = 1.10f$ and $B'_{max} = B_{max}$, we substitute these values:
$$ \frac{P_{h,new}}{P_{h,old}} = \frac{(1.10f) \cdot (B_{max})^{x}}{f \cdot B_{max}^{x}} = 1.10 $$
So, $P_{h,new} = 1.10 \cdot P_{h,old}$.
The percentage change in hysteresis loss is:
$$ \% \Delta P_h = \frac{P_{h,new} - P_{h,old}}{P_{h,old}} \times 100 = \frac{1.10 P_{h,old} - P_{h,old}}{P_{h,old}} \times 100 $$
$$ \% \Delta P_h = \frac{0.10 P_{h,old}}{P_{h,old}} \times 100 = 10\% $$
Therefore, the hysteresis loss increases by 10%.
We know $P_e \propto f^2 \cdot B_{max}^{2}$. Let the original loss be $P_{e,old}$ and the new loss be $P_{e,new}$.
$$ \frac{P_{e,new}}{P_{e,old}} = \frac{(f')^2 \cdot (B'_{max})^{2}}{f^2 \cdot B_{max}^{2}} $$
Substituting $f' = 1.10f$ and $B'_{max} = B_{max}$:
$$ \frac{P_{e,new}}{P_{e,old}} = \frac{(1.10f)^2 \cdot (B_{max})^{2}}{f^2 \cdot B_{max}^{2}} = \frac{(1.10)^2 f^2 \cdot B_{max}^{2}}{f^2 \cdot B_{max}^{2}} $$
$$ \frac{P_{e,new}}{P_{e,old}} = (1.10)^2 = 1.21 $$
So, $P_{e,new} = 1.21 \cdot P_{e,old}$.
The percentage change in eddy current loss is:
$$ \% \Delta P_e = \frac{P_{e,new} - P_{e,old}}{P_{e,old}} \times 100 = \frac{1.21 P_{e,old} - P_{e,old}}{P_{e,old}} \times 100 $$
$$ \% \Delta P_e = \frac{0.21 P_{e,old}}{P_{e,old}} \times 100 = 21\% $$
Therefore, the eddy current loss increases by 21%.
Based on the calculations, when the supply voltage and frequency are both increased by 10%:
The percentage changes are 10% and 21%, respectively.
Eddy current loss in a transformer can be reduced by _________.
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A single-phase, 4 kVA, 200 V/100 V, 50 Hz transformer with laminated CRGO steel core has rated no-load loss of 450 W. When the high-voltage winding is excited with 160 V, 40 Hz sinusoidal ac supply, the no-load losses are found to be 320 W. When the high-voltage winding of the same transformer is supplied from a 100 V, 25 Hz sinusoidal ac source, the no-load losses will be_________ W (rounded off to 2 decimal places).