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Question 841Question →

In an electromechanical relay, the normally closed (NC) contacts maintain electrical continuity and allow current to flow through the load circuit when the control coil is de-energized.

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Answer: True

Answer

True
Relay contact states are defined relative to the de-energized (unpowered) coil condition. Normally Closed (NC) contacts are held shut by a mechanical return spring when the coil has no current, thereby maintaining a complete circuit and allowing current to pass.

Step-by-Step Solution

1
Identify the operating definition of 'normal' in relay terminology.
The normal state refers to the resting condition of the relay when no voltage or current is applied to the electromagnetic coil.
All contact designations (Normally Open and Normally Closed) are standardized based on the unpowered coil state.
2
Determine the physical contact position of Normally Closed (NC) contacts in the unpowered state.
The internal return spring holds the movable armature firmly against the NC contact terminal, forming a continuous electrical path.
Mechanical spring tension keeps the circuit closed until magnetic force from an energized coil pulls the armature away.
3
Evaluate circuit continuity and current flow capability.
Because the physical contacts touch, electrical continuity exists and current can flow through the load circuit.
Closed contacts provide a low-resistance path allowing electrical current to circulate.

Key Concept

Normally Closed (NC) vs. Normally Open (NO) Relay Contact States
Estimated Time:45s
Question 842Question →

A direct current (DC) cooling fan in an electronics enclosure operates at a voltage of 24 V24\text{ V} and draws a current of 1.5 A1.5\text{ A}. What is the total electrical power consumed by the fan?

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Answer: 36 W36\text{ W}

Answer

36 W36\text{ W}
According to Watt's Law, electrical power in a DC circuit is determined by multiplying the voltage by the current (P=V×IP = V \times I). Multiplying 24 V24\text{ V} by 1.5 A1.5\text{ A} results in 36 W36\text{ W} of power dissipation.

Step-by-Step Solution

1
Identify the given electrical quantities and the appropriate Watt's Law formula.
Voltage V=24 VV = 24\text{ V}, Current I=1.5 AI = 1.5\text{ A}, Formula: P=V×IP = V \times I
Electrical power in a DC circuit is directly defined as the product of electromotive force (voltage) and current.
2
Substitute the values into the formula and calculate the power.
P=24 V×1.5 A=36 WP = 24\text{ V} \times 1.5\text{ A} = 36\text{ W}
Multiplying 2424 by 1.51.5 gives 3636, with the standard unit of power being watts (W).

Key Concept

Watt's Law calculates electrical power (PP) as the product of voltage (VV) and current (II), expressed as P=V×IP = V \times I.
Estimated Time:45s
Question 843Question →

When comparing two electrical wires of identical length, diameter, and temperature, which material property determines which wire has lower electrical resistance?

Show answer & explanation

Answer: Resistivity

Answer

Resistivity is the material property that determines the electrical resistance of equal-dimensioned conductors.
Resistivity (represented by ρ\rho) is an intrinsic physical property of a material that measures its natural opposition to electric current flow. According to the formula R=ρLAR = \rho \frac{L}{A}, when two conductors share identical length (LL) and cross-sectional area (AA) at constant temperature, the wire made of a material with lower resistivity will have lower total electrical resistance.

Step-by-Step Solution

1
Apply the fundamental formula for conductor resistance: R=ρLAR = \rho \frac{L}{A}.
Total resistance (RR) is directly proportional to conductor length (LL), inversely proportional to cross-sectional area (AA), and directly proportional to resistivity (ρ\rho).
Because length, diameter (area), and temperature are held constant between the two wires, any difference in total resistance is strictly governed by the material's resistivity.
2
Identify the property representing the material's specific opposition to current.
Resistivity (ρ\rho) is the intrinsic characteristic of the substance.
A material with lower resistivity (such as copper compared to iron) will always yield a lower resistance when shaped into identical physical dimensions.

Key Concept

Resistance and Resistivity
Estimated Time:45s
Question 844Question →

A standard circuit breaker trips and interrupts power to an appliance branch circuit due to an electrical overload. After the fault condition has been resolved, what action is required to restore power to the circuit?

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Answer: Manually reset the breaker operating handle back to the closed (ON) position.

Answer

Manually reset the breaker operating handle back to the closed (ON) position.
Circuit breakers are reusable protective devices engineered with bimetallic strips or electromagnetic coils that open electrical contacts during overcurrent events. Unlike fuses that melt and must be discarded, a circuit breaker simply trips its mechanical latch and can be reset manually to the ON position once the electrical fault is cleared.

Step-by-Step Solution

1
Identify the type of protective device specified in the scenario.
The device is a circuit breaker, which is a reusable electromechanical switch.
Differentiating between sacrificial devices (fuses) and resettable devices (circuit breakers) determines the correct maintenance action.
2
Determine the procedure for restoring an open circuit breaker after a trip.
The internal trip mechanism mechanically separates the contacts, which can be re-engaged by toggling the external handle.
Circuit breakers do not destroy their internal elements during normal tripping and do not need to be replaced.

Key Concept

Circuit Breaker Operation and Resetting
Estimated Time:45s
Question 845Question →

Match each circuit protective device on the left with its primary operating characteristic or application on the right.

Click a left item, then click its matching right item

Items

Fast-acting fuse
Slow-blow (time-delay) fuse
Magnetic circuit breaker
Metal-oxide varistor (MOV)

Matches

Show answer & explanation

Answer

Fast-acting fuse pairs with opening rapidly to protect sensitive semiconductor electronics; Slow-blow fuse pairs with tolerating brief inrush currents from inductive motors; Magnetic circuit breaker pairs with using an electromagnetic coil to trip during heavy short circuits; Metal-oxide varistor pairs with clamping transient high-voltage surges.
Each protective device is engineered for a specific fault type or application: fast-acting fuses react immediately to protect delicate electronics; slow-blow fuses accommodate brief inductive surges; magnetic breakers use electromagnetism for instant short-circuit tripping; and metal-oxide varistors suppress high-voltage spikes.

Step-by-Step Solution

1
Identify the characteristic of a fast-acting fuse
Matches with immediate element melting to protect delicate solid-state electronics from sudden overcurrent.
Semiconductors cannot withstand overcurrent for even brief durations.
2
Identify the characteristic of a slow-blow fuse
Matches with tolerating brief inrush currents during electric motor startup.
Inductive loads draw high starting current that would blow standard fuses prematurely.
3
Identify the characteristic of a magnetic circuit breaker
Matches with utilizing an electromagnetic coil to trip instantaneously during high-current short circuits.
Electromagnetic pull is proportional to current and trips the contact latch mechanism without relying on heat.
4
Identify the characteristic of a metal-oxide varistor (MOV)
Matches with clamping high-voltage transient spikes.
MOVs are voltage-dependent resistors designed specifically for surge suppression rather than direct overcurrent interruption.

Key Concept

Operating principles and applications of circuit protection devices including thermal, magnetic, time-delay, and voltage suppression elements
Estimated Time:45s
Question 846Question →

A circuit is constructed with a 10 V10\text{ V} DC power supply connected in series with a 220 Ω220\ \Omega current-limiting resistor. After the resistor, the circuit splits into two parallel branches that eventually reconnect to the negative terminal of the power supply. The first parallel branch contains a Zener diode (rated at VZ=6.2 VV_Z = 6.2\text{ V}) installed in a reverse-biased orientation. The second parallel branch contains a standard silicon diode installed in a forward-biased orientation. Based on this configuration, what is the approximate voltage measured across the parallel diode combination, and which component dictates this voltage?

Show answer & explanation

Answer: 0.7 V0.7\text{ V}, dictated by the forward-biased standard silicon diode clamping the voltage.

Answer

The correct answer is 0.7 V0.7\text{ V}, dictated by the forward-biased standard silicon diode clamping the voltage.
The correct answer accurately identifies that in a parallel circuit, the component with the lowest forward voltage drop or breakdown voltage dictates the voltage across the entire parallel block. Since the standard silicon diode is forward-biased, it drops approximately 0.7 V. This prevents the voltage across the parallel branches from ever reaching the 6.2 V required to cause the Zener diode to break down and conduct. The Zener diode remains effectively an open circuit, and the standard diode clamps the branch voltage at 0.7 V.

Step-by-Step Solution

1
Determine the biasing state of each diode in the parallel branches based on the power supply orientation.
The Zener diode is reverse-biased (requires 6.2 V to reach breakdown), and the standard silicon diode is forward-biased (requires ~0.7 V to conduct).
A diode's behavior depends fundamentally on whether it is forward or reverse-biased.
2
Analyze the voltage rules for parallel circuits.
The voltage across all components connected in parallel must be identical.
This fundamental circuit law means both the Zener diode branch and the standard diode branch must share the exact same voltage drop.
3
Determine the clamping voltage of the parallel combination.
The forward-biased silicon diode begins conducting heavily at 0.7 V, clamping the voltage across both branches at this level.
Because the silicon diode provides a low-resistance path at 0.7 V, the voltage cannot rise high enough to reach the Zener diode's 6.2 V breakdown threshold. The Zener diode remains effectively off (open circuit).

Key Concept

Diode Biasing and Parallel Circuit Voltage Clamping
Estimated Time:1m 30s
Question 847Question →

A power supply circuit utilizes a step-down transformer to convert an alternating current (AC) input of 100 V100\text{ V} to an output of 25 V25\text{ V}. If the primary winding contains 400 turns400\text{ turns}, how many turns are on the secondary winding?

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Answer: 100 turns100\text{ turns}

Answer

100 turns100\text{ turns}
The correct answer is 100 turns100\text{ turns}. According to the transformer turns ratio law, the ratio of secondary voltage to primary voltage equals the ratio of secondary turns to primary turns: VsVp=NsNp\frac{V_s}{V_p} = \frac{N_s}{N_p}. Rearranging to solve for the secondary turns yields Ns=Np×(VsVp)=400×(25100)=100 turnsN_s = N_p \times \left(\frac{V_s}{V_p}\right) = 400 \times \left(\frac{25}{100}\right) = 100\text{ turns}. Since this is a step-down transformer (100 V100\text{ V} down to 25 V25\text{ V}, a 4:14:1 step-down ratio), the secondary coil must have one-fourth the number of turns of the primary coil.

Step-by-Step Solution

1
Identify the given transformer parameters
Primary voltage Vp=100 VV_p = 100\text{ V}, secondary voltage Vs=25 VV_s = 25\text{ V}, primary turns Np=400 turnsN_p = 400\text{ turns}
Extracting the known values is necessary to set up the turns ratio equation.
2
State the transformer voltage and turns ratio formula
VpVs=NpNs  ⟹  Ns=Np×(VsVp)\frac{V_p}{V_s} = \frac{N_p}{N_s} \implies N_s = N_p \times \left(\frac{V_s}{V_p}\right)
In an ideal transformer, the voltage across each winding is directly proportional to the number of turns.
3
Substitute the values and calculate the secondary winding turns
Ns=400×(25 V100 V)=400×0.25=100 turnsN_s = 400 \times \left(\frac{25\text{ V}}{100\text{ V}}\right) = 400 \times 0.25 = 100\text{ turns}
Performing the proportional calculation gives the exact number of secondary turns required.

Key Concept

Transformer Turns Ratio and Voltage Transformation
Estimated Time:45s
Question 848Question →

A piece of copper hookup wire with a length of 15 m15\text{ m} has an electrical resistance of 0.6 Ω0.6\ \Omega. If the wire is replaced with a 45 m45\text{ m} piece of the exact same wire type and gauge at the same temperature, what is the resistance of the new wire in ohms (Ω\Omega)?

Show answer & explanation

Answer: 1.8

Answer

1.8 \Omega
According to the fundamental resistance relationship R=ρLAR = \rho \frac{L}{A}, resistance is directly proportional to the length LL of the conductor when resistivity ρ\rho and cross-sectional area AA remain unchanged. Tripling the wire length from 15 m15\text{ m} to 45 m45\text{ m} multiplies the resistance by a factor of 3, resulting in 0.6 Ω×3=1.8 Ω0.6\ \Omega \times 3 = 1.8\ \Omega.

Step-by-Step Solution

1
Calculate the proportional change in conductor length.
The new length is 3 times the original length (45 m÷15 m=345\text{ m} \div 15\text{ m} = 3).
Identifying the scaling factor allows direct application of the resistance formula.
2
Apply the direct proportionality between conductor length and electrical resistance (R∝LR \propto L).
Rnew=Rold×3=0.6 Ω×3=1.8 ΩR_{\text{new}} = R_{\text{old}} \times 3 = 0.6\ \Omega \times 3 = 1.8\ \Omega.
Since material resistivity (ρ\rho) and cross-sectional area (AA) are held constant, tripling the length triples the total resistance.

Key Concept

The electrical resistance of a uniform conductor is directly proportional to its length (R=ρLAR = \rho \frac{L}{A}).
Estimated Time:45s
Question 849Question →

In an external circuit connected to a direct-current (DC) power source, electron flow theory states that negative charge carriers travel from the positive terminal to the negative terminal.

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Answer: False

Answer

False
Electron flow theory describes the physical movement of negatively charged electrons, which travel from the negative terminal through the external circuit load toward the positive terminal. Traveling from positive to negative describes conventional current flow.

Step-by-Step Solution

1
Identify the electrical current model referenced in the statement.
The statement explicitly cites 'electron flow theory' in an external circuit.
Electronics distinguishes between electron flow theory and conventional current flow theory.
2
Determine the physical direction of electrons based on fundamental electrostatic laws.
Electrons possess a negative charge, causing them to be repelled by the negative terminal and drawn toward the positive terminal.
Like charges repel each other while opposite charges attract.
3
Evaluate the accuracy of the statement's claimed direction.
Movement from positive to negative defines conventional current, making the claim regarding electron flow theory false.
Electron flow moves from negative to positive externally.

Key Concept

Direction of Electron Flow vs. Conventional Current
Estimated Time:35s
Question 850Question →

An electronics technician is replacing components on a circuit board and selects an electrolytic capacitor for the DC power supply filtering stage. Why must the technician observe strict polarity when installing an electrolytic capacitor into a DC circuit?

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Answer: They possess an electrochemical insulating oxide layer that breaks down and can cause the component to overheat or rupture under reverse voltage.

Answer

Electrolytic capacitors have an electrochemical oxide dielectric layer that breaks down and causes the component to overheat or rupture if connected with reversed polarity.
Electrolytic capacitors are polarized components because their extremely thin dielectric layer (aluminum or tantalum oxide) is formed and maintained electrochemically in one specific voltage direction. If connected in reverse polarity, this insulating layer breaks down rapidly, allowing heavy leakage current to generate boiling electrolyte gases, resulting in device failure, venting, or explosion.

Step-by-Step Solution

1
Identify the internal construction of electrolytic capacitors.
Electrolytic capacitors utilize an extremely thin dielectric film of aluminum oxide or tantalum oxide maintained by a chemical electrolyte.
Understanding the unique dielectric mechanism explains why electrolytic capacitors provide high capacitance in a compact size but possess polarity restrictions.
2
Analyze the electrical behavior of the dielectric layer under reverse polarity.
When reversed voltage is applied, the electrochemical reaction breaks down and de-forms the insulating oxide layer.
The formation and insulation of the oxide layer are unidirectional.
3
Evaluate the practical consequence of reverse installation in a circuit.
With the dielectric compromised, large leakage currents flow through the electrolyte, producing excessive heat, gas buildup, and catastrophic rupture or short circuit.
This necessitates strict observance of the positive and negative terminal markings during assembly and maintenance.

Key Concept

Electrolytic Capacitor Polarity and Dielectric Integrity
Estimated Time:1m 0s
Question 851Question →

A technician sets up an experiment with two electrically isolated wire coils wrapped around a shared soft-iron core. Coil 1 is connected in series with a 12 V12\text{ V} DC power supply and a mechanical switch. Coil 2 is connected directly to a sensitive center-zero galvanometer. The switch is closed and kept closed until current stabilizes, after which the switch is abruptly opened. What behavior will the galvanometer display during the period of steady current and at the exact instant the switch is opened?

Show answer & explanation

Answer: The meter reads zero while the current is steady, then momentarily deflects in response to the rapidly collapsing magnetic flux when the switch is opened.

Answer

The meter reads zero while current is steady, but momentarily deflects when the switch is opened due to the rapid collapse of magnetic flux.
Electromagnetic induction strictly requires a changing magnetic flux cutting through a conductor (Vinduced=−NΔΦΔtV_{\text{induced}} = -N \frac{\Delta \Phi}{\Delta t}). While steady DC current flows in the primary coil, the magnetic field is static, producing no voltage in the secondary coil (meter reads zero). When the switch is opened, the magnetic field collapses rapidly to zero, generating a steep rate of flux change that induces a momentary voltage spike, causing the galvanometer to deflect briefly.

Step-by-Step Solution

1
Analyze the electromagnetic state during steady-state DC current flow.
Magnetic flux is constant (ΔΦΔt=0\frac{\Delta \Phi}{\Delta t} = 0), resulting in 0 V0\text{ V} induced in the secondary coil.
According to Faraday's Law of Electromagnetic Induction (Vinduced=−NΔΦΔtV_{\text{induced}} = -N\frac{\Delta \Phi}{\Delta t}), an electromotive force is generated only when magnetic flux changes over time.
2
Analyze the electromagnetic transition at the instant the primary switch is opened.
Current drops abruptly from steady-state value to zero, causing a rapid collapse of magnetic flux (ΔΦΔt≠0\frac{\Delta \Phi}{\Delta t} \neq 0).
The sudden collapse of magnetic lines of force cuts across the secondary windings, inducing a transient voltage pulse and causing a momentary galvanometer deflection.
3
Synthesize the two operational states to evaluate secondary meter response.
The meter must read zero during steady current and show a sharp, temporary deflection when the circuit is broken.
Combines Faraday's requirement for dynamic flux with the transient behavior of inductive circuits.

Key Concept

Faraday's Law of Electromagnetic Induction and transient flux changes
Estimated Time:1m 30s
Question 852Question →

A technician is troubleshooting a test circuit connected to a 32V32\text{V} DC power supply. The circuit consists of a fixed resistor R1R_1 in series with a parallel block. The parallel block contains a 12 kΩ12\text{ k}\Omega fixed resistor and a variable resistor (rheostat) RvR_v. The resistor R1R_1 has four color bands: Green, Blue, Red, and Gold. The technician adjusts the rheostat RvR_v until the total current drawn from the power supply is exactly 4 mA4\text{ mA}.

What is the resistance setting of the rheostat RvR_v in kilohms (k Ω\Omega)?

Show answer & explanation

Answer: 3

Answer

3
The total resistance required by the circuit to draw 4 mA4\text{ mA} from a 32V32\text{V} source is 8 kΩ8\text{ k}\Omega. The series resistor R1R_1 (Green, Blue, Red) contributes 5.6 kΩ5.6\text{ k}\Omega. This leaves exactly 2.4 kΩ2.4\text{ k}\Omega required for the parallel section. For a 12 kΩ12\text{ k}\Omega resistor in parallel with an unknown RvR_v to yield an equivalent resistance of 2.4 kΩ2.4\text{ k}\Omega, RvR_v must be set to 3 kΩ3\text{ k}\Omega.

Step-by-Step Solution

1
Decode the color code of resistor R1R_1.
R1=5.6 kΩR_1 = 5.6\text{ k}\Omega
The color bands are Green (5), Blue (6), and Red (multiplier of 10210^2 or 100). Thus, 56×100=5,600 Ω56 \times 100 = 5,600\ \Omega, which is 5.6 kΩ5.6\text{ k}\Omega. The Gold band indicates a 5% tolerance, which applies to real-world variance but does not alter our nominal calculation.
2
Calculate the total equivalent resistance (ReqR_{eq}) of the circuit.
Req=8 kΩR_{eq} = 8\text{ k}\Omega
Using Ohm's Law (R=VIR = \frac{V}{I}), divide the source voltage (32V32\text{V}) by the total current (4 mA4\text{ mA} or 0.004 A0.004\text{ A}) to find the total resistance required to draw that current.
3
Determine the required equivalent resistance of the parallel block.
Rparallel=2.4 kΩR_{parallel} = 2.4\text{ k}\Omega
Since R1R_1 is in series with the parallel block, subtract R1R_1 from the total circuit resistance to find the resistance of the parallel segment: 8 kΩ−5.6 kΩ=2.4 kΩ8\text{ k}\Omega - 5.6\text{ k}\Omega = 2.4\text{ k}\Omega.
4
Solve for the rheostat's resistance (RvR_v).
Rv=3 kΩR_v = 3\text{ k}\Omega
The parallel block contains a 12 kΩ12\text{ k}\Omega resistor and RvR_v. Using the parallel resistance formula 1Rp=1Ra+1Rb\frac{1}{R_p} = \frac{1}{R_a} + \frac{1}{R_b}, we get 12.4=112+1Rv\frac{1}{2.4} = \frac{1}{12} + \frac{1}{R_v}. Rearranging gives 1Rv=12.4−112=1024−224=824=13\frac{1}{R_v} = \frac{1}{2.4} - \frac{1}{12} = \frac{10}{24} - \frac{2}{24} = \frac{8}{24} = \frac{1}{3}, meaning Rv=3 kΩR_v = 3\text{ k}\Omega.

Key Concept

Integrating Ohm's law with series-parallel equivalent resistance and resistor color code decoding.
Estimated Time:3m 0s
Question 853Question →

A DC power supply is connected across a series circuit containing two resistive components. Fill in the blanks with the correct numerical values to complete the circuit analysis.

Fill in the blanks below

A 50 V50\text{ V} DC source is connected in series with a 15 Ω15\ \Omega resistor and a second resistor R2R_2. If the circuit draws a current of 2 A2\text{ A}, the total circuit resistance is Ω\Omega, and the resistance of R2R_2 is Ω\Omega.
Show answer & explanation

Answer

The total circuit resistance is 25 Ω25\ \Omega, and the resistance of R2R_2 is 10 Ω10\ \Omega.
Applying Ohm's Law to the total circuit yields a total resistance of RT=50 V2 A=25 ΩR_T = \frac{50\text{ V}}{2\text{ A}} = 25\ \Omega. In a series circuit, total resistance equals the sum of the individual component resistances (RT=R1+R2R_T = R_1 + R_2). Subtracting the known resistor value (15 Ω15\ \Omega) from the total resistance (25 Ω25\ \Omega) results in R2=10 ΩR_2 = 10\ \Omega.

Step-by-Step Solution

1
Calculate the total circuit resistance (RTR_T) using Ohm's Law with source voltage and total current.
RT=VTI=50 V2 A=25 ΩR_T = \frac{V_T}{I} = \frac{50\text{ V}}{2\text{ A}} = 25\ \Omega
In any complete circuit, the total equivalent resistance equals total source voltage divided by the total circuit current.
2
Calculate the resistance of R2R_2 using the series circuit resistance addition formula (RT=R1+R2R_T = R_1 + R_2).
R2=RT−R1=25 Ω−15 Ω=10 ΩR_2 = R_T - R_1 = 25\ \Omega - 15\ \Omega = 10\ \Omega
In a series circuit, total resistance is the direct sum of individual component resistances.

Key Concept

In a series circuit, total resistance is the direct sum of individual resistances (RT=R1+R2+…R_T = R_1 + R_2 + \dots), and the circuit current is constant through all components as governed by Ohm's Law (RT=VT/IR_T = V_T / I).
Estimated Time:1m 0s
Question 854Question →

A transformer can continuously induce a voltage in its secondary winding when powered by a steady, unchanging direct current (DC) source.

Show answer & explanation

Answer: False

Answer

False
The statement is false because continuous electromagnetic induction requires a time-varying magnetic flux. A steady DC current produces a stationary, unchanging magnetic field, resulting in zero continuous induced voltage across the secondary winding.

Step-by-Step Solution

1
Analyze the electrical power source and component operation described in the statement.
The statement specifies applying steady, constant direct current (DC) to the primary winding of a transformer to produce continuous secondary voltage.
Transformers rely on mutual electromagnetic induction between primary and secondary windings.
2
Evaluate the condition required for continuous electromagnetic induction.
Faraday's law of induction dictates that induced voltage is directly proportional to the rate of change of magnetic flux (ΔΦ/Δt\Delta \Phi / \Delta t). A steady DC source produces a constant magnetic field (ΔΦ/Δt=0\Delta \Phi / \Delta t = 0), meaning no continuous voltage is induced.
Continuous induction requires a continuously changing current and magnetic flux, such as alternating current (AC).

Key Concept

Electromagnetic induction in transformers requires a time-varying magnetic flux, meaning a steady direct current (DC) cannot maintain continuous secondary induction.
Estimated Time:45s
Question 855Question →

Match each resistor configuration or color-coded component on the left with its corresponding electrical characteristic and operating principle on the right.

Click a left item, then click its matching right item

Items

Three-terminal potentiometer wired across a DC supply voltage (VinV_{\text{in}}) with output taken from the wiper
Variable resistor wired as a rheostat with the wiper connected to one end terminal
Four-band fixed resistor with color sequence Yellow, Violet, Orange, Gold
Four-band fixed resistor with color sequence Brown, Gray, Green, Silver

Matches

Show answer & explanation

Answer

The three-terminal potentiometer matches the voltage divider function; the rheostat matches the series current limiter with wiper-to-end protection; the Yellow-Violet-Orange-Gold resistor matches 47 kΩ±5%47\text{ k}\Omega \pm 5\%; and the Brown-Gray-Green-Silver resistor matches 1.8 MΩ±10%1.8\text{ M}\Omega \pm 10\%.
Each item correctly links the component physical description or color code to its precise electrical definition: potentiometers provide variable potential division, rheostats adjust circuit current, Yellow-Violet-Orange-Gold evaluates to 47 kΩ±5%47\text{ k}\Omega \pm 5\%, and Brown-Gray-Green-Silver evaluates to 1.8 MΩ±10%1.8\text{ M}\Omega \pm 10\%.

Step-by-Step Solution

1
Analyze the three-terminal potentiometer and rheostat wiring configurations
A potentiometer connected across a power source acts as a continuous voltage divider (0 V0\text{ V} to VinV_{\text{in}}) at the wiper terminal. A rheostat uses a variable two-terminal configuration in series with the load to regulate current.
Variable resistors differ in circuit function based on whether they are wired as three-terminal potential dividers or two-terminal current adjusters.
2
Decode the four-band color code for Yellow-Violet-Orange-Gold
Yellow = 4, Violet = 7, Orange = multiplier 103=1,00010^3 = 1,000, Gold = ±5%\pm 5\%. Value =47×1,000 Ω=47 kΩ±5%= 47 \times 1,000\ \Omega = 47\text{ k}\Omega \pm 5\%.
Standard EIA 4-band color coding assigns significant digits to the first two bands, a decimal multiplier to the third band, and tolerance percentage to the fourth band.
3
Decode the four-band color code for Brown-Gray-Green-Silver
Brown = 1, Gray = 8, Green = multiplier 105=100,00010^5 = 100,000, Silver = ±10%\pm 10\%. Value =18×100,000 Ω=1.8 MΩ±10%= 18 \times 100,000\ \Omega = 1.8\text{ M}\Omega \pm 10\%.
Standard EIA 4-band color coding converts 1,800,000 Ω1,800,000\ \Omega using standard metric prefixes to 1.8 MΩ1.8\text{ M}\Omega with a silver tolerance of ±10%\pm 10\%.

Key Concept

Operating principles and terminal configurations of fixed and variable resistors (potentiometers, rheostats, and standard color codes)

Alternative Method

To quickly decode 4-band resistors, write down the two digits (e.g., 47 for Yellow-Violet or 18 for Brown-Gray), append the number of zeros indicated by the multiplier color (3 zeros for Orange = 47,000, 5 zeros for Green = 1,800,000), and simplify to metric units (kilo or mega).
Estimated Time:1m 0s
Question 856Question →

Inserting a soft iron core into the center of an energized coil of wire increases the overall strength of the magnetic field compared to an air-core coil with the same current and number of turns.

Show answer & explanation

Answer: True

Answer

True
The statement is true because soft iron is a ferromagnetic material with high magnetic permeability, which greatly concentrates magnetic flux lines and amplifies the electromagnetic field strength for a given current.

Step-by-Step Solution

1
Identify the factors that determine magnetic flux density in a solenoid
Magnetic flux density is governed by the relation B=μNLIB = \mu \frac{N}{L} I, where μ\mu is core permeability, NN is number of turns, LL is coil length, and II is current.
Core material permeability directly determines the magnetic flux density for a given amount of magnetomotive force.
2
Compare the magnetic properties of soft iron to air
Soft iron is a ferromagnetic substance with relative magnetic permeability hundreds to thousands of times greater than air.
Higher permeability provides a low-reluctance path that concentrates lines of magnetic force inside and around the core.
3
Determine the effect of adding an iron core on overall field strength
Adding the soft iron core significantly amplifies the magnetic field produced by the coil, confirming the statement is true.
This physical principle is the foundation for creating practical electromagnets, relays, and inductors.

Key Concept

Effect of ferromagnetic core permeability on electromagnetic field strength
Estimated Time:45s
Question 857Question →

A direct-current power distribution box supplies power to two parallel branches. The first branch has a resistance of 20 Ω20\ \Omega, and the second branch has a resistance of 5 Ω5\ \Omega. What is the total equivalent resistance of the network?

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Answer: 4 Ω4\ \Omega

Answer

4 Ω4\ \Omega
In a parallel circuit with two branches, the equivalent resistance is calculated using the product-over-sum formula Req=R1×R2R1+R2R_{\text{eq}} = \frac{R_1 \times R_2}{R_1 + R_2}. Substituting 20 Ω20\ \Omega and 5 Ω5\ \Omega gives 20×520+5=10025=4 Ω\frac{20 \times 5}{20 + 5} = \frac{100}{25} = 4\ \Omega. Total resistance in parallel is always less than the lowest individual resistor value.

Step-by-Step Solution

1
Identify the formula for the equivalent resistance of two parallel resistors.
Req=R1×R2R1+R2R_{\text{eq}} = \frac{R_1 \times R_2}{R_1 + R_2} or 1Req=1R1+1R2\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2}
Parallel branches provide multiple paths for current, resulting in a total resistance that is less than any individual branch resistance.
2
Substitute the given values (R1=20 ΩR_1 = 20\ \Omega and R2=5 ΩR_2 = 5\ \Omega) into the product-over-sum formula.
Req=20×520+5=10025R_{\text{eq}} = \frac{20 \times 5}{20 + 5} = \frac{100}{25}
Simplifying the numerator and denominator allows direct calculation of equivalent resistance.
3
Divide the product by the sum.
Req=4 ΩR_{\text{eq}} = 4\ \Omega
Computing 10025\frac{100}{25} yields the final equivalent resistance.

Key Concept

Total Equivalent Resistance in Parallel Circuits
Estimated Time:45s
Question 858Question →

When the direct current flowing through an inductor decreases, the self-induced electromotive force (counter-EMF) acts in the same direction as the original current to oppose the reduction in current flow.

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Answer: True

Answer

True
The statement is true because Lenz's law dictates that self-induced voltage opposes the change in current rather than the absolute direction of current flow. When circuit current decreases, the collapsing magnetic field induces a voltage of such polarity that it acts in the same direction as the original current to sustain the flow.

Step-by-Step Solution

1
Analyze the fundamental principle of electromagnetic induction and Lenz's law for inductors.
Lenz's law states that the polarity of an induced electromotive force (EMF) always opposes the specific change in magnetic flux or current that creates it (e=−LΔIΔte = -L \frac{\Delta I}{\Delta t}).
Inductors store energy within their magnetic field and oppose instantaneous changes in current magnitude.
2
Evaluate the behavior of the magnetic field when current decreases.
As current decreases, the magnetic field around the inductor collapses across the coil windings, inducing an electromotive force.
A changing magnetic flux through a conductor induces an electric potential.
3
Determine the direction and polarity of the induced EMF relative to the original current.
To oppose the reduction in current (ΔI/Δt<0\Delta I / \Delta t < 0), the induced EMF acts as an aiding voltage source in the same direction as the original current flow.
Opposing a decay in current requires supplying voltage to keep current moving in the original direction.
4
Conclude the truth value of the statement.
The statement correctly describes the directional behavior of self-induced counter-EMF during current decay, confirming the statement is True.
Counter-EMF opposes the direction of current only when current is increasing; during current decrease, it reinforces the original current direction.

Key Concept

Lenz's Law and Self-Induction in Inductors
Estimated Time:45s
Question 859Question →

A direct current (DC) circuit consists of a 48 V48\text{ V} power supply connected in series with three resistors: R1=12 ΩR_1 = 12\ \Omega, R2=24 ΩR_2 = 24\ \Omega, and R3=24 ΩR_3 = 24\ \Omega. In its baseline operating state, the total circuit resistance is RT=60 ΩR_T = 60\ \Omega and the circuit loop current is I=0.8 AI = 0.8\text{ A}.

Match each circuit alteration on the left to its corresponding electrical outcome on the right.

Click a left item, then click its matching right item

Items

A zero-resistance jumper wire (short circuit) is placed directly across resistor R3R_3.
Resistor R2R_2 burns out internally, creating an open circuit condition.
A fourth resistor with a value of R4=20 ΩR_4 = 20\ \Omega is connected in series with the existing chain.
The power supply voltage is increased from 48 V48\text{ V} to 72 V72\text{ V} while keeping all components unchanged.

Matches

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Answer

The correct matches pair: (1) shorting resistor R3R_3 with total resistance dropping to 36 Ω36\ \Omega, current rising to 1.33 A1.33\text{ A}, and 0 V0\text{ V} across R3R_3; (2) an open at R2R_2 with loop current dropping to 0 A0\text{ A} and 48 V48\text{ V} appearing across R2R_2; (3) adding a 20 Ω20\ \Omega series resistor with total resistance rising to 80 Ω80\ \Omega, current dropping to 0.6 A0.6\text{ A}, and 7.2 V7.2\text{ V} across R1R_1; and (4) raising the source to 72 V72\text{ V} with total resistance remaining 60 Ω60\ \Omega, current rising to 1.2 A1.2\text{ A}, and 28.8 V28.8\text{ V} across R2R_2.
Each modification directly follows the governing principles of series DC circuits. In series circuits, total resistance equals the direct sum of all individual resistances (RT=R1+R2+⋯+RnR_T = R_1 + R_2 + \dots + R_n), and current is constant throughout the single loop (IT=VTRTI_T = \frac{V_T}{R_T}). Short circuits eliminate individual component resistance and drop component voltage to zero while raising loop current. Open circuits eliminate current entirely and place full source voltage across the open terminals. Adding series resistance reduces current throughout the loop, and increasing source voltage increases current and all individual voltage drops proportionally.

Step-by-Step Solution

1
Analyze the short circuit condition across R3R_3
RT=12+24=36 ΩR_T = 12 + 24 = 36\ \Omega; I=4836≈1.33 AI = \frac{48}{36} \approx 1.33\text{ A}; V3=0 VV_3 = 0\text{ V}
A short circuit bypasses the component with zero resistance, eliminating its resistance from the total series sum and producing zero potential difference across itself.
2
Analyze the open circuit condition at R2R_2
I=0 AI = 0\text{ A}; V1=0 VV_1 = 0\text{ V}; V3=0 VV_3 = 0\text{ V}; V2=48 VV_2 = 48\text{ V}
An open in a series circuit interrupts the sole conductive loop, causing current to cease everywhere; infinite resistance across the open component causes the full source potential to appear across the gap.
3
Analyze the addition of a fourth series resistor (R4=20 ΩR_4 = 20\ \Omega)
RT=60+20=80 ΩR_T = 60 + 20 = 80\ \Omega; I=4880=0.6 AI = \frac{48}{80} = 0.6\text{ A}; V1=0.6×12=7.2 VV_1 = 0.6 \times 12 = 7.2\text{ V}
In series circuits, equivalent resistance is additive (RT=∑RR_T = \sum R). Increasing total resistance reduces total current according to Ohm's Law (I=VRTI = \frac{V}{R_T}), which proportionally reduces individual component voltage drops.
4
Analyze the voltage source increase to 72 V72\text{ V}
RT=60 ΩR_T = 60\ \Omega; I=7260=1.2 AI = \frac{72}{60} = 1.2\text{ A}; V2=1.2×24=28.8 VV_2 = 1.2 \times 24 = 28.8\text{ V}
Resistor values are independent of source voltage. Applying Ohm's Law with higher voltage across constant resistance yields directly proportional increases in loop current and individual voltage drops.

Key Concept

Series Circuit Governing Rules: Additive Resistance, Current Continuity, Ohm's Law, and Fault Dynamics
Estimated Time:2m 0s
Question 860Question →

A marine communications transceiver utilizes a direct current (DC) bias network. A voltmeter connected across a fixed 2.5 kΩ2.5\text{ k}\Omega resistor measures a steady voltage drop of 15 V15\text{ V}. What is the current flowing through this resistor?

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Answer: 6 mA6\text{ mA}

Answer

The current flowing through the resistor is 6 mA6\text{ mA}.
According to Ohm's law, current equals voltage divided by resistance (I=V/RI = V / R). Dividing 15 V15\text{ V} by 2.5 kΩ2.5\text{ k}\Omega (2500 Ω2500\text{ }\Omega) yields 0.006 A0.006\text{ A}, which converts directly to 6 mA6\text{ mA}.

Step-by-Step Solution

1
Convert the given resistance from kilo-ohms to fundamental SI units (ohms).
R=2.5 kΩ=2.5×103 Ω=2500 ΩR = 2.5\text{ k}\Omega = 2.5 \times 10^3\text{ }\Omega = 2500\text{ }\Omega
Standard calculations in Ohm's law require values in fundamental units (volts, amperes, ohms).
2
Apply Ohm's law formula to solve for current (I=V/RI = V / R).
I=15 V2500 Ω=0.006 AI = \frac{15\text{ V}}{2500\text{ }\Omega} = 0.006\text{ A}
Current is directly proportional to voltage and inversely proportional to resistance.
3
Convert the resulting current from amperes to milliamperes.
0.006 A=0.006×1000 mA=6 mA0.006\text{ A} = 0.006 \times 1000\text{ mA} = 6\text{ mA}
Matching the standard unit formatting in electronic measurement options.

Key Concept

Ohm's Law expresses the fundamental relationship between voltage, current, and resistance in a DC circuit (I=V/RI = V / R).
Estimated Time:1m 0s
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