Electotechnology Flashcards
Motor Power Equations
Pmech = T * omega
where T = torque, omega = rotational speed
Pmech = Pelec = E * I
where E = Back EMF, I = Current
Difference between Brushed and Brushless Motors
Brushed motors have a commutator ring to flip the direction of current to keep the motor turning in the right direction using a DC power supply. They introduce mechanical and electrical losses and require maintenance.
Breushless motors have a different arcitecture, meaning the permanent magnet is located on the rotor while the windings are found on the casing / stator. The change in the direction of the current is timed by a separate controller that detects the position of the rotor using a Hall-effect sensor.
General Motor Equations
F = πΌd Γ B, force on each wire
T=2r Γ F = 2r Γ πΌd Γ B = k * πΌ, torque from looped wire. So times by n, number of wires, to obtain total torque.
Difference between High pass and Low pass filter
A high pass filter blocks the transmission of low frequency signals, whereas a low pass filter blocks the transmission of high frequency signals.
For low pass filters, Inductor comes before the resistor for a RL filter and the resistor comes first for a RC filter
For high pass filters, resistor comes before the inductor for a RL filter and the capacitor comes first for the RC filter
Cut off Frequency
All low-pass filters are rated at a certain cutoff frequency. That is, the frequency above which the output voltage falls below 70.7% of the input voltage.
f = 1/ (2piR*C)
Resistance of a Wire
R = (rho*l)/A
where rho = specific resistance, l = length, A = area
Kirchhoffβs Voltage Law
The algebraic sum of voltage rises and drops along a closed circuit loop is zero.
e.g. ππ΄ β ππ΅ = πΌπ 1 β 3π + πΌπ 2 + 4π + πΌπ 3
Kirchhoffβs Current Law
The sum of the currents entering a junction must equal the sum of the currents leaving the junction.
Time response of Inductors and Capacitors
Inductors :
I(t) = (V/R)(1-e^(-(R/L)t))
Capacitors :
Vc(t) = V(1-e^(-(1/RC)*t))
Reactance
Reactance results as a ratio between voltage and current, it is purely imaginary.
Units are Ohms.
To compute reactance use the equation for impedance for inductors and capacitors, only difference is that there is no resistor present?
Admittance and susceptance
Y_L = 1/R - j1/(Lomega)
Y_C = 1/R + jComega
where the second part of each equation (complex part) is the susceptance.
Susceptance is the inverse of reactance, It is purely imaginary.
Units are Siemens [S].
Resonance
Occurs when both an inductor and capacitor are present in a circuit, can be both series or parallel.
omega = resonance freq = 1/sqrt(LC)
When a resistor is added to the circuit the current through the resistor is found by
V/R * e^(jomegat)
In series circuits the current maximises at resonance whereas in parallel circuits voltage becomes maximum.
Magnetic fields and Magnets
F = q*V x B = force on moving charge
where B = magnetic field strength and V = velocity of charge
B = mu_0 * H
where mu_0 = The proportionality constant = 4π Γ 10β7 and H = actual magentic field strength.
In a ferromagnetic material: B = ΞΌπΞΌ0H
H = (N*i)/l , where N = number of coils around core, i = current, l = mean length of the core.
Magnetic fluc density = AB = πππ0ΞH = phi
Electromotive force = N*i
Magnetic resistance = F/phi
Analysis of frequency filters
RC low pass : R1 C2
πΊ (ππ) =(πππ’π‘ (ππ)) / (πππ (ππ)) = (ππΆ (ππ))/(ππΆ (ππ) + ππ
(ππ)) = 1/(1 + πππΆR)
LR low pass : L1 R2
πΊ (ππ) = (πR (ππ))/(πL (ππ) + ππ
(ππ)) = π
/(πππΏ + R)
RC high pass : C1 R2
πΊ (ππ) =(πππ’π‘ (ππ)) / (πππ (ππ)) = (ππ
(ππ))/(ππΆ (ππ) + ππ
(ππ)) = (πππΆπ
)/(1 + πππΆπ
)
LR high pass : R1 L2
πΊ (ππ) = (πL (ππ))/(πL (ππ) + ππ
(ππ)) = (jπ(L/R))/(jπ(L/R) +1)
Where G is the transfer function
Sparks
A spark requires a certain energy to stay ionised. It becomes more conductive the more current flows, lowing the voltage.
πΌ β π/U