From MetroAmp Wiki
A series circuit is a circuit in which electrical current has only 1 path to flow. The circuit imposes a certain amount of resistance on the power supply. This resistance value and the supply voltage determines how much current will flow through the circuit, and that current flow will be the same value at all points in the circuit.
Laws Of Series Circuits
Current flow is the same at all points in a series circuit.
Total circuit resistance and supply voltage determine the amount of current flow through the circuit.
Each component in the circuit will drop a certain amount of voltage, which is known as a "voltage drop". The value of the voltage drop will appear across the component. The value of the voltage drop across a particular component in a series circuit is determined by the resistance value of the component and the amount of total circuit current.
The sum of the voltage drops across each component in a series circuit will always equal the supply voltage.
Component resistance is additive in a series circuit. In other words, the sum of each component's resistance values will equal the total circuit resistance.
A break (i.e. disconnection) anywhere in a series circuit will stop all current flow.
Some basic math skills are required in the study of electricity and electronics. The equation most used in electricity and electronics is known as Ohms Law. The main equation of Ohm's Law is -
E = I x R where -
E = Electromotive Force in Volts
I = Current flow in Amps
R = Electrical resistance in Ohms
Two of the three above mentioned values must be known before you can find the third value. The above equation can be rearranged one of the following two ways -
If Voltage and Resistance are known and you need to find current flow (Amps) -
I = E / R
If Voltage and Current (Amps) are known and you need to find resistance (ohms) -
R = E / I
In series circuits, "I" (current flow in amps) will always be a constant value.
Ohm's Law HowTo
Here are the instructions for using Ohm's Law in series circuits.
1) Multiplying total circuit current by total circuit resistance will give you total supply voltage.
2) Multiplying total circuit current by the resistance value of 1 component will give you the voltage drop across that one component.
3) Dividing the supply voltage by total circuit resistance will give you total circuit current.
4) Dividing the supply voltage by total circuit current will give you total circuit resistance.
5) Multiplying total circuit current by the combined resistance value of two or more components in line with each other will give you the voltage drop across those two or more components.
6) Adding the voltage drops of all components in a series circuit together will equal the total supply voltage.
7) The only time total supply voltage is used in Ohm's Law is when trying to find either total circuit current or total circuit resistance.
8) Once total circuit current is found in a series circuit, this value remains constant for that circuit unless -
a) Supply voltage changes b) the resistance value of a circuit component changes
9) Measuring the voltage drop across 1 component in a series circuit, then dividing that voltage by the resistance value of that one component will give you total circuit current (current remains the same at all points in a series circuit).
Typical Series Circuit
Below is a link to a schematic of a typical series circuit.
This circuit is the same circuit used in the bias supply of a 100 watt Marshall plexi and is known as a "voltage divider" circuit. The supply voltage is divided up between the three resistors as current flows through them.
The arrows indicate the direction of current flow. The positive charge on the positive terminal of battery B1 pulls negative electrons from the negative terminal of B1 (opposite charges attract), through R3, R2 and R1, then back to the positive terminal. R1, R2 and R3 limit the amount of electrons (current) the positive terminal can pull through the circuit.
If we take a look at the circuit, we can see that we know the total supply voltage of battery B1 (80VDC) as well as the values of R1, R2 and R3 (R1 = 27K ohm, R2 = 15K ohm and R3 = 47K ohm). Since total circuit resistance = the sum of the resistance of all components in the circuit, we can add the values of R1, R2 and R3 to get our total circuit resistance.
Rt = R1 + R2 + R3 where -
Rt is the total circuit resistance in Ohms
R1 is the value of R1 in ohms
R2 is the value of R2 in ohms
R3 is the value of R3 in ohms
Since the value of R1 is 27K ohms, the value of R2 is 15K ohms, and the value of R3 is 47K ohms, we'll plug these values into the above equation to get our total circuit resistance.
Rt = 27K ohms + 15K ohms + 47K ohms
Rt = 89K ohms
So our total circuit resistance is 89K ohms. We can now use our total circuit resistance and the supply voltage to find how much current is flowing through the circuit. Since current flow is the same at all points in a series circuit, this current value will be constant throughout the remaining equations.
It = Es / Rt where -
It = total circuit current in Amps
Es = total supply voltage
Rt = total circuit resistance in ohms
It = 80VDC / 89,000 ohms (89K)
It = 0.0009 Amps, or 0.9mA (milliamps)
Now that we know the total circuit current (0.0009 amps), we can multiply this by the value of R3 to find the value of the voltage drop across R3 (voltage between points Ground and A).
Er3 = It x Rr3 where -
Er3 = voltage drop across R3
It = total circuit current in amps
Rr3 = resistance value of R2 in ohms
Er3 = 0.0009 Amps x 47,000 ohms (47K)
Er3 = 42 Volts across R3
To find the voltage drop across R2 (voltage between points A and B), we can multiply the value of R2 by the total circuit current in amps.
Er2 = It x Rr2 where -
Er2 = voltage drop across R2
It = total circuit current in amps
Rr2 = resistance value of R2 in ohms
Er2 = 0.0009 Amps x 15,000 ohms (15K)
Er2 = 14 Volts across R2
To find the voltage drop across R1 (voltage between points B and C), we can multiply the value of R1 by the total circuit current in amps.
It x Rr1 = Vr1 (Voltage across R1)
0.0009 amps x 27,000 ohms (27K) = 24 volts across R1
To check our math, we use one of the laws of series circuits.
"The sum of all voltage drops in a series circuit always equals the total supply voltage."
24 volts + 14 Volts + 42 Volts = 80 Volts
Our math checks out.
Another Series Circuit
Now let's add a fourth resistor into the circuit.
This circuit is the same circuit, but with the addition of R4. Since it's value is 25K, this adds 25K to the total circuit resistance.
R1 + R2 + R3 + R4 = Rt
27K + 15K + 47K + 25K = 114K ohms Rt (total circuit resistance)
Since the total circuit resistance went up, the total circuit current (It) has dropped.
Total Supply Voltage / Rt = It
80 Volts / 114,000 (114K) = 0.0007 amps 0.7mA (milliamps)
The voltage between ground and test point B will be the voltage drop across R3.
It x R3 = Voltage R3
0.0007 Amps x 25,000 ohms (25K) = 17.5 volts
The voltage at test point A will be the voltage drop across both R3 and R2 together. This is because when measuring between ground and test point A, you're reading the voltage across both resistors together.
To find the voltage at test point A, we must first add the resistance values of R3 and R4 together to get the total resistance between test point A and ground.
R3 + R2 = Ra (resistance to ground at test point A)
25K + 47K = 72K
Resistance to ground at test point A (Ra) is 72K ohms.
Voltage at test point A = It x Ra
0.0007 Amps x 72,000 (72K) = 50.4
Voltage at test point A = 50.4 Volts
Another way we could've done that was to find the voltage drop across R3 by multiplying the total circuit current (It) by the value of R3. Then add that value to the voltage drop across R4.
It x R3 = Voltage drop across R3
0.0007 amps x 47,000 ohms (47K) = 32.9 Volts across R3
Then we add the voltage across R3 to the voltage across R4.
Vr3 + Vr4 = Voltage at test point A where -
Vr3 = Voltage drop across R3
Vr4 = Voltage drop across R4
32.9 volts + 17.5 volts = 50.4 Volts
Voltage at test point A = 50.4 Volts
Now that we have our total circuit current, we can go through and find the voltage drops across the last two resistors.
It x R2 = Vr2
It x R1 = Vr1
0.0007 amps x 15,000 (15K) = 10.5 volts
0.0007 amps x 27,000 (27K) = 18.9 Volts
Vr2 = 10.5 Volts
Vr1 = 18.9 Volts
Now let's add up our voltage drops -
Vr1 + Vr2 + Vr3 + Vr4 = Vsupply
18.9 + 10.5 + 32.9 + 17.5 = 79.8 Volts
Vsupply = 79.8 Volts
- Note - When performing math functions on any kind of circuit with high circuit resistance, answers will be within a couple of tenths of each other due to the math involved with such tiny amounts of current. But you get the idea.
In circuit 1, we ended up with around 42 volts from test point A to ground.
In circuit 2, we ended up with around 50 volts from test point A to ground.
Circuit 1's "A" voltage was taken across a 47K ohm resistor. Circuit 2's "A" voltage was taken across both the 47K ohm and the 25K ohm resistor.
That is essentially how the adjustable bias supply in a Marshall amplifier works. Rotating the pot 1 way removes the pot from the circuit by shorting the 47K ohm resistor to ground, while rotating it the other way adds 25K ohms of resistance between the 47K ohm to ground. This decreases and increases the voltage drop between ground and the 47K ohm resistor, giving you an adjustable voltage supply.
For simplification, the transformer was replaced with a battery, and the rectifier and the filter caps in the bias supply were removed from the above circuits, but -
The rectifier is what converts the AC from the transformer to "pulsed DC".
The capacitors in the supply act as "temporary batteries" by charging on the pulses, then discharging through the bias circuit in between pulses, thereby keeping the voltage at a steady state between pulses.
The only other difference between the above two circuits and the bias supply is that the polarity of an actual bias supply is reversed to give a negative voltage. But the math works exactly the same.