Circuit Analysis and Power Electronics Flashcards

1
Q

Decibel described in terms of Vout and Vin

A
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2
Q

What does the plot of the magnitude response as a function of frequency look like?

A
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3
Q

What dictates the linearity of a circuit?

A
  • An input signal v1 gives an output signal v1out = Av1
  • an input signal v2 gives an output signal v2out = Av2
  • an input signal (v1 + v2) gives an output signal v1out + v2out = A(v1 + v2)
  • So, for a sinusoidal input voltage of frequency f, any output of the circuit is also sinusoidal with frequency f. Note that the output need not be in phase with the input.
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4
Q

Active vs Passive circuits

A

Active circuits include devices that draw power from a power supply.

Passive circuits don’t draw extra power.

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5
Q

What is the best representation to add and subtract impedances?

A

cartesian coordinates

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6
Q

what is the best representation to multiply and divide?

A

Polar coordinates

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7
Q

Finding Polar from Cartesian

A
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8
Q

What is the instantaneous power of a resistor? (what does plot look like )

A

For the resistor the +ve instantaneous power p(t) corresponds to energy being transferred to the resistor – the average power P =

averaged over a cycle is non- zero as shown on the previous slide. This net transfer of energy is that dissipated in the resistor per cycle, i.e. lost as heat into the surroundings.

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9
Q

What does the instantaneous power of an inductor look like? (relationship between current and voltage)

A

Voltage leads current by pi/2.

Average power is zero.

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10
Q

What does the instantaneous power of a capacitor look like?

A

Voltage lags Current by pi/2

Average power is zero.

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11
Q

Impedance and Admittance of R L C components.

A
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12
Q

To calculate the average power dissipated in a resistor over a cycle what equation would you use.

A
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13
Q

Mathematical expression for mean value value of a waveform v(t) over an interval T

A
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14
Q

How would you calculate the RMS of a waveform?

A

To calculate the root-mean-squared:

First, square the function.

Then, calculate the mean of the square.

Lastly, take the square root.

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15
Q

For sinusoidal signals, what is a quick way of determining the RMS?

Can this be used for other sorts of waveforms?

A

Amplitude divided by the square root of 2 gives RMS.

This cannot be used for other signals. Important that you only use this on sinusoidal signals! Other waveforms will need to have their RMS through the longer procedure.

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16
Q

Calculate RMS for this signal

A
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17
Q

What is the power factor?

A

cos(ϕ) is the power factor.

If loads in a circuit are purely resistive, cos(ϕ)=1.

If cos(ϕ) = 0 (i.e. ϕ = ±90), then purely reactive loads.

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18
Q

For a driven LCR circuit, how does the phase angle change across a range of frequencies?

Why is this?

A

The phase is negative for frequencies lower than the resonance, this is because the voltage across the inductor becomes small (for lower frequencies) and the capacitor dominates. Since the current leads the voltage in a capacitor, the resultant phase is negative.

It is the opposite for positive phase angle… The inductor dominates at higher frequencies and with an inductor the voltage leads the current.

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19
Q

The equation relating Rin and Rout of a transformer.

What generalisation can you make for the load?

A

Can be generalized for any complex load ZL. The impedance seen on the primary side is that of the load multiplied by the square of the turns ratio*.

*Note carefully here that the turns ratio is usually defined as Np:Ns not Ns:Np

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20
Q

What is something that all cables have at high frequencies?

A

At high freq all cables have characteristic RF impedance Z0. It is independent of the cable length and is real(resistive).

Again, it is only seen by high-frequency RF signals and it isn’t the resistance of the wire nor is it the impedance you measure at lower frequencies.

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21
Q

Mutual inductance: what does M depend on?

A

M will not depend on I1 (which will cancel) but only on geometric factors such as the dimensions, separation, relative orientation, number of turns (of both coils) and the relative permeability (µr) of the medium between the coils.

22
Q

How do you calculate the normalized coupling parameter?

A
23
Q

Why do the coils in a transformer have a k ~0.99?

A

Coils on a transformer have a k ~0.99 because it is wound a closed ferromagnetic core with high relative permeability mu_r > 100. Acts as a magnetic circuit, all the flux generated by the first coil is concentrated inside the core with only a very small fraction leaking out.

24
Q

What are the major applications of transformers?

A
  1. To step up (increase) or step down (decrease) the amplitude of ac voltages, e.g. in power transmission or in home electronics
  2. To match the impedance of electrical components to maximize power transfer for lower frequency signals (or minimize signal reflection for rf signals).
  3. To isolate circuits from one another for safety or other issues.
  4. To couple resonant circuits together - e.g. radio detection
25
Q

Why the Ns

Turns of secondary

A

The reason is that in faradays law the emf is related to the change of flux-linkage rather than just “flux”

26
Q

emf related to the turns ratio

A
27
Q

How can you change the sign of the secondary coil voltage output with respect to the primary?

A

Changing out the coils are wound affects the sign.

28
Q

What does the dot notation represent in terms of transformers?

A

The polarity of the voltage is the same at the dots.

With a load, if the primary current is going in at the primary dot, then it is coming out at the secondary dot.

29
Q

What is the net effect of adding a load to the secondary outputs of a transformer?

A

Primary current increases.

When we add the load the increase in primary current means that more energy is now being drawn from the source and this is the energy that is being dissipated in the load.

30
Q

When you compare this to the voltage turns ratio, what does it tell you?

A

It tells you that if the transformer steps up the voltage to the load, the current must step down by the same ratio (vice-versa). The transformer cannot supply more power than is supplied by the source.

31
Q

What is the equation that relates Rin to RL of a transformer?

A

*Note*

Here the turns ratio is flipped compared to the voltage/turns ratio equation.

So remember that for this equation the primary is the numerator and secondary denominator.

32
Q

What does decreasing the secondary coils relative to the primary do?

A

It increases the RLtrans (RLtrans is equivalent Rin)

33
Q

At high frequencies what are all cables characterized by?

A

By characteristic impedance Z0

Which relates the voltage drop dV and the current I along an infinitesimal length dl.

Note: the characteristic impedance is only something that is seen by high frequency rf signals.

34
Q

How does the autotransformer use less copper than a regular transformer?

And what is one of its disadvantages?

A

It prevents you from having to use thicker wires when having to transfer larger current due to a step up.

35
Q

What are the 4 types of losses?

A
  1. Copper losses (ohmic losses) - currents flowing in the electrical resistance of the wire making up the windings of the transformer result in losses. Since windings are usually made out of copper, they are called “copper losses”.
    1. Copper losses in primary = ip2(rms) x Rp
    2. Copper losses in secondary = is2 (rms) x Rs
  2. Imperfect Coupling - imperfect magnetic coupling. These losses can be minimized by winding the transformer on a ferromagnetic core.
  3. Eddy currents - When the flux in the transformer core changes as a function of time, a current will be induced in the core itself if it is made of a conducting material and hence there will be losses in the resistance of the core.
    1. The usual way of overcoming eddy currents is to make the core out of thin sheets of ferromagnetic material insulated from each other. The laminations are oriented to break up the eddy current flow and minimize the dissipation.
  4. Hysteresis - magnetism in ferromagnetic materials is attributable to the orientation of tiny magnetic domains, whose magnetic fields align with an externally applied magnetic field.
    1. Magnetic domains have a certain inertia to this change, energy is required to continually cause them to reverse, commonly known as hysteresis loss.
    2. The term hysteresis comes from a loop formed when you plot the magnetization of a ferromagnetic material versus the applied field. The resulting area enclosed by the loop is the work that needs to be done.

Sum of the eddy current and hysteresis losses is collectively known as the core loss.

36
Q

How do we represent the effect of leakage flux?

A

Lp and Ls are the total inductances of primary and secondary respectively.

Lpm refers to the mutual flux

Lpl refers to the leakage flux

Same for secondary.

37
Q

What are the high/ low-frequency behaviors of real transformers?

A

At very high frequencies capacitative effects become important.

At high frequencies the ‘capacitors’ tend to acts as shorts. At low frequencies the primary inductance Lpm tends to short the load.

38
Q

What does the frequency response of a real transformer look like?

A

Remember, that the impedance of an inductor is jw L and the impedance of a capacitor is 1/jwC.

39
Q

What are the stages in the analysis of real transformers?

A
40
Q

How do you determine the emf of a loop rotating in a magnetic field?

A
41
Q

Whats the difference between phase and line voltage?

A

Phase voltage is between any phase (live wire) and neutral

Line voltage is between any two phases (two live wires)

42
Q

What generator is this?

A

Four wire ‘Star’ connected generator

Has a neutral wire.

So it has a phase and line voltage.

43
Q

What generator is this ?

What ‘voltages’ does it have

A

Three-wire delta configuration

Name comes from triangular shape.

The delta doesn’t have neutral wire.

So only line voltages.

44
Q

How do you find the voltage across two components that are out of phase with each other?

What about currents?

A

Determined using phasor diagram

They need to be determined using a phasor diagram.

45
Q

Why use three-phase electricity?

A
  1. Can deliver more kVa (power) than single-phase or DC using the same total amount of conductor (copper).
    1. For a given power requirement can use much less material (thinner wire) ⇒ cheaper because less material is used and less maintenance costs. Lighter lines are easier to install, supporting structures not as big.
  2. Lower transmission losses over long distances compared to single phase.
  3. 3-phase loads like 3-phase induction motors have several advantages:
    1. doesn’t need slip rings or require heavy insulated coils to turn.
    2. runs more smoothly than single phase - single phase falls to 0 every cycle, for 3 phase it is constant.
    3. They have self-starting properties
  4. Flexibility/Ease of supply and distribution. You can either use the large line voltage between 2 phases in the star arrangement or each phase on its own e.g. to houses in a street.
46
Q

What is the relationship between phase (load resistance) and line voltage for star configuration?

And current ?

A

Vph * √(3) = VL

or

Vph = VL/ √(3)

The current through each load resistance is the same as the line current

47
Q

What is the current and voltage relationship between the load resistance and the line voltage for a balanced delta load?

A

The voltage across each load resistance is the same as the line voltage.

The current through each connecting line is √3 times the load current.

48
Q

What is the relationship between load currents in a balanced delta load configuration?

How do you find the line current?

A

they are 120 degrees out of phase

line current is found to be the vector difference of the two load currents

49
Q

Explain why a 3 phase star configuration has less energy loss than single phase.

A

Comes down to the fact that the current is spread between three wires compared to 1 wire for one phase.

From P = I2R you can see that multiple I2RT by 3 will lead to a lower transmission loss than (3I)2RT .

50
Q

How do you draw the equivalent circuit for a real transformer?

A
51
Q

Kirchoffs 1st law

A

At any node (junction) in an electrical circuit, the sum of currents flowing into that node is equal to the sum of currents flowing out of that node.

52
Q

kirchoffs 2nd law

A

The algebraic sum of all the voltages around any closed loop in a circuit is zero