Module 1—Introduction to Matter, Energy, and Direct CurrentPages
i  ix, 11 to 110,
111 to 120, 121 to 130,
141 to 150, 151 to 160,
161 to 165, 21 to 210,
211 to 220, 221 to 229,
31 to 310, 311 to 320,
321 to 330, 331 to 340,
341 to 350, 351 to 360,
361 to 370, 371 to 380,
381 to 390, 391 to 3100,
3101 to 110, 3111 to 3120,
3121 to 3126, Appendix I,
II, III,
IV, V,
Index
circuit involved. To illustrate this point, figure 362 shows a seriesparallel network in which shorts
are developed. In figure 362 (A) the normal circuit is shown. RT = 40 ohms and IT = 3 amps.
Figure 362.—Seriesparallel circuit with shorts.
In figure 362 (B), R1 has shorted. R1 now has zero ohms resistance. The total the resistance the
circuit is now equal to the resistance the parallel network R2 and R3, or 20 ohms. Circuit current has increased
to 6 amps. All this current goes through the parallel network (R2, R3) and this increase in current would most
likely damage the components.
In figure 362 (C), R3 has shorted. With R3 shorted there is a short
circuit in parallel with R2 . The short circuit routes the current around R2, effectively removing R2 from the
circuit. Total circuit resistance is now equal to the resistance R1, or 20 ohms.
As you know, R2 and R3
form a parallel network. Resistance the network can be calculated as follows:
Given:
391
Solution:
The total circuit current with R3 shorted is 6 amps. All this current flows through R1 and would most
likely damage R1. Notice that even though only one portion the parallel network was shorted, the entire paralleled
network was disabled.
Opens and shorts alike, if occurring in a circuit, result in an overall change in
the equivalent resistance. This can cause undesirable effects in other parts the circuit due to the corresponding
change in the total current flow. A short usually causes components to fail in a circuit which is not properly
fused or otherwise protected. The failure may take the form a burnedout resistor, damaged source, or a fire
in the circuit components and wiring.
Fuses and other circuit protection devices are installed in
equipment circuits to prevent damage caused by increases in current. These circuit protection devices are designed
to open if current increases to a predetermined value. Circuit protection devices are connected in series with the
circuit or portion the circuit that the device is protecting. When the circuit protection device opens, current
flow ceases in the circuit.
A more thorough explanation fuses and other circuit protection devices is
presented in Module 3, Introduction to Circuit Protection, Control, and Measurement.
Q46. What is the
effect on total resistance and total current in a circuit if an open occurs in (a) a parallel branch, and (b) in a
series portion?
Q47. What is the effect on total resistance and total current in a circuit if a short
occurs in (a) a parallel branch, and (b) in a series portion?
Q48. If one branch a parallel network is shorted, what portion circuit current flows through the
remaining branches?
VOLTAGE DIVIDERS Most electrical and electronics equipment
use voltages various levels throughout their circuitry. One circuit may require a 90volt supply, another a
i50volt supply, and still another a i80volt supply. These voltage requirements could be supplied by three
individual power sources. This method is expensive and requires a considerable amount room. The most common method
supplying these voltages is to use a single voltage source and a VOLTAGE DIVIDER. Before voltage dividers are
explained, a review what was discussed earlier concerning voltage references may be help.
392
As you know, some circuits are designed to supply both positive and negative voltages. Perhaps now you
wonder if a negative voltage has any less potential than a positive voltage. The answer is that 100 volts is 100
volts. Whether it is negative or positive does not affect the feeling you get when you are shocked.
Voltage polarities are considered as being positive or negative in respect to a reference point, usually ground.
Figure 363 will help to illustrate this point.
Figure 363.—Voltage polarities.
Figure 363(A) shows a series circuit with a voltage source 100 volts and four 50ohm resistors connected
in series. The ground, or reference point, is connected to one end resistor R1. The current in this circuit
determined by Ohm’s law is .5 amp. Each resistor develops (drops) 25 volts. The five tapf points indicated in the
schematic are points at which the voltage can be measured. As indicated on the schematic, the voltage measured at
each the points from point A to point E starts at zero volts and becomes more positive in 25 volt steps to a value
positive 100 volts.
In figure 363(B), the ground, or reference point has been moved to point B. The current in the circuit is
still .5 amp and each resistor still develops 25 volts. The total voltage developed in the circuit remains at 100
volts, but because the reference point has been changed, the voltage at point A is negative 25 volts. Point E,
which was at positive 100 volts in figure 363(A), now has a voltage positive 75 volts. As you can see the voltage
at any point in the circuit is dependent on three factors; the current through the resistor, the ohmic value the
resistor, and the reference point in the circuit.
A typical voltage divider consists two or more resistors
connected in series across a source voltage (Es). The source voltage must be as high or higher than any voltage
developed by the voltage divider. As the source voltage is dropped in successive steps through the series
resistors, any desired
393
portion the source voltage may be “tapped f“ to supply individual voltage requirements. The values the
series resistors used in the voltage divider are determined by the voltage and current requirements the loads.
Figure 364 is used to illustrate the development a simple voltage divider. The requirement for this voltage
divider is to provide a voltage 25 volts and a current 910 milliamps to the load from a source voltage 100 volts.
Figure 364(A) provides a circuit in which 25 volts is available at point B. If the load was connected between
point B and ground, you might think that the load would be supplied with 25 volts. This is not true since the load
connected between point B and ground forms a parallel network the load and resistor R1. (Remember that the value
resistance a parallel network is always less than the value the smallest resistor in the network.)
Figure 364.—Simple voltage divider.
Since the resistance the network would now be less than 25 ohms, the voltage at point B would be less than
25 volts. This would not satisfy the requirement the load.
To determine the size resistor used in the
voltage divider, a rulethumb is used. The current in the divider resistor should equal approximately 10 percent
the load current. This current, which does not flow through any the load devices, is called bleeder current.
Given this information, the voltage divider can be designed using the following steps.
1. Determine the
load requirement and the available voltage source.
394
2. Select bleeder current by applying the 10% rulethumb.
3. Calculate bleeder resistance.
The value R1 may be rounded f to 275 ohms:
4. Calculate the total current (load plus bleeder).
5. Calculate the resistance the other divider resistor(s).
The voltage divider circuit can now be drawn as shown in figure 364(B).
Q49. What information
must be known to determine the component values for a voltage divider?
395
Q50. If a voltage divider is required for a load that will use 450 mA current, what should be the
value bleeder current?
Q51. If the load in question 50 requires a voltage +90 V, what should be the value
the bleeder resistor?
Q52. If the source voltage for the voltage divider in question 50 supplies 150
volts, what is the total current through the voltage divider?
MULTIPLELOAD VOLTAGE DIVIDERS
A multipleload voltage divider is shown in figure 365. An important point that was not emphasized before is
that when using the 10% rulethumb to calculate the bleeder current, you must take 10% the total load current.
Figure 365.—Multipleload voltage divider.
Given the information shown in figure 365, you can calculate the values for the resistors needed in the
voltagedivider circuits. The same steps will be followed as in the previous voltage divider problem.
396
Given:
The bleeder current should be 10% the total load current. Solution:
Since the voltage across R1 (ER1) is equal to the voltage requirement for load 1, Ohm’s law can be used
to calculate the value for R1.
Solution:
The current through R2 (IR2) is equal to the current through R1 plus the current through load 1.
Solution:
The voltage across R2 (ER2) is equal to the difference between the voltage requirements load 1 and load
2.
397
Ohm’s law can now be used to solve for the value R2 . Solution:
The current through R3 (IR3) is equal to the current through R2 plus the current through load 2.
The voltage across R3 (ER3) equals the difference between the voltage requirement load 3 and load 2.
Ohm’s law can now be used to solve for the value R3 . Solution:
The current through R4 (IR4) is equal to the current through R3 plus the current through load 3. IR4 is
equal to total circuit current (IT).
The voltage across R4 (ER4) equals the difference between the source voltage and the voltage requirement
load 3.
398
Ohm’s law can now be used to solve for the value R4 . Solution:
With the calculations just explained, the values the resistors used in the voltage divider are as follows:
POWER IN THE VOLTAGE DIVIDER
Power in the voltage divider is an extremely
important quantity. The power dissipated by the resistors in the voltage divider should be calculated to determine
the power handling requirements the resistors. Total power the circuit is needed to determine the power
requirement the source.
The power for the circuit shown in figure 365 is calculated as follows: Given:
Solution:
The power in each resistor is calculated just as for R1. When the calculations are performed, the
following results are obtained:
399
To calculate the power for load 1: Given:
Solution:
The power in each load is calculated just as for load 1. When the calculations are performed, the
following results are obtained.
Total power is calculated by summing the power consumed by the loads and the power dissipated by the
divider resistors. The total power in the circuit is 15.675 watts.
The power used by the loads and divider
resistors is supplied by the source. This applies to all electrical circuits; power for all components is supplied
by the source.
Since power is the product voltage and current, the power supplied by the source is equal to the source
voltage multiplied by the total circuit current (Es x IT).
In the circuit figure 365, the total power
can be calculated by: Given:
Solution:
VOLTAGE DIVIDER with POSITIVE and NEGATIVE VOLTAGE REQUIREMENTS
In many cases the
load for a voltage divider requires both positive and negative voltages. Positive and negative voltages can be
supplied from a single source voltage by connecting the ground (reference point) between two the divider
resistors. The exact point in the circuit at which the reference point is placed depends upon the voltages
required by the loads.
3100
Introduction to Matter, Energy, and Direct Current, Introduction
to Alternating Current and Transformers, Introduction to Circuit Protection,
Control, and Measurement, Introduction to Electrical Conductors, Wiring Techniques,
and Schematic Reading, Introduction to Generators and Motors,
Introduction to Electronic Emission, Tubes, and Power Supplies,
Introduction to SolidState Devices and Power Supplies,
Introduction to Amplifiers, Introduction to
WaveGeneration and WaveShaping Circuits, Introduction to Wave Propagation, Transmission
Lines, and Antennas, Microwave Principles,
Modulation Principles, Introduction to Number Systems and Logic Circuits, Introduction
to Microelectronics, Principles of Synchros, Servos, and Gyros,
Introduction to Test Equipment, RadioFrequency
Communications Principles, Radar Principles, The Technician's Handbook,
Master Glossary, Test Methods and Practices, Introduction to Digital Computers,
Magnetic Recording, Introduction to Fiber Optics
