Basic Electrical Concepts

189 soru

Soru 81Soru →

A technician connects a diagnostic meter into a vehicle wire harness to measure the quantity of electric charge passing through a conductor per second. Which electrical property is the technician measuring?

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Cevap: Electric current

Cevap

Electric current represents the measured rate of electrical charge passing through a conductor per second.
Electric current is defined as the rate at which electrical charge passes a given cross-section of a conductor, mathematically represented by I=QtI = \frac{Q}{t}, where one ampere equals one coulomb of charge per second.

Adım Adım Çözüm

1
Analyze the physical measurement described in the question.
The measurement monitors charge (QQ) moving past a point over elapsed time (tt).
Identifying the relationship between electrical charge and time determines the correct physical quantity.
2
Match the formula I=QtI = \frac{Q}{t} to its standard electrical property.
The rate of charge flow per second defines electric current, measured in amperes (1 A=1 C/s1\text{ A} = 1\text{ C/s}).
Electric current is the formal definition of moving electric charge carriers through a conductor.

Anahtar Kavram

Electric current is the rate of flow of electric charge over time, expressed as I=QtI = \frac{Q}{t} and measured in amperes.
Tahmini Süre:35s
Soru 82Soru →

An electric heating element is rated to dissipate 1.8 kW1.8\text{ kW} of power when connected across a standard 120 V120\text{ V} DC supply line. If a control circuit reduces the direct current flowing through the heating element to 5 A5\text{ A} while its internal resistance remains constant, what is the new power dissipated by the element?

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Cevap: 200 W200\text{ W}

Cevap

200 W200\text{ W}
The correct answer of 200 W200\text{ W} is found by first converting 1.8 kW1.8\text{ kW} to 1800 W1800\text{ W}. Using the initial ratings, the element's resistance is R=V2P=12021800=8 ΩR = \frac{V^2}{P} = \frac{120^2}{1800} = 8\text{ }\Omega. With the current controlled to 5 A5\text{ A}, the dissipated power is P=I2R=(5 A)2×8 Ω=25×8=200 WP = I^2 R = (5\text{ A})^2 \times 8\text{ }\Omega = 25 \times 8 = 200\text{ W}.

Adım Adım Çözüm

1
Convert the rated power from kilowatts to watts
P1=1.8 kW=1800 WP_1 = 1.8\text{ kW} = 1800\text{ W}
Metric prefixes must be converted to base SI units before performing Watt's Law calculations.
2
Calculate the constant internal resistance (RR) of the heating element using the initial rating
R=V12P1=(120 V)21800 W=144001800=8 ΩR = \frac{V_1^2}{P_1} = \frac{(120\text{ V})^2}{1800\text{ W}} = \frac{14400}{1800} = 8\text{ }\Omega
The heating element's resistance remains unchanged and serves as the bridge to calculate power under the new operating current.
3
Calculate the new power dissipation with the reduced current (I2=5 AI_2 = 5\text{ A})
P2=I22×R=(5 A)2×8 Ω=25×8=200 WP_2 = I_2^2 \times R = (5\text{ A})^2 \times 8\text{ }\Omega = 25 \times 8 = 200\text{ W}
Watt's Law specifies that power dissipation across a known resistance is directly proportional to the square of the current.

Anahtar Kavram

Watt's Law Power and Resistance Relationships (P=V2RP = \frac{V^2}{R} and P=I2RP = I^2 R)

Alternatif Yöntem

Determine the initial current I1=P1V1=1800 W120 V=15 AI_1 = \frac{P_1}{V_1} = \frac{1800\text{ W}}{120\text{ V}} = 15\text{ A}. Since P∝I2P \propto I^2 for a constant resistance, scaling the power by the ratio of the currents squared gives P2=P1×(I2I1)2=1800 W×(5 A15 A)2=1800×(13)2=18009=200 WP_2 = P_1 \times \left(\frac{I_2}{I_1}\right)^2 = 1800\text{ W} \times \left(\frac{5\text{ A}}{15\text{ A}}\right)^2 = 1800 \times \left(\frac{1}{3}\right)^2 = \frac{1800}{9} = 200\text{ W}.
Tahmini Süre:1m 30s
Soru 83Soru →

An avionics technician tests a 72 V72\text{ V} direct current (DC) instrument circuit. If the circuit's total resistance is measured at 1.2 kΩ1.2\text{ k}\Omega, what is the current flowing through the circuit?

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Cevap: 60 mA60\text{ mA}

Cevap

60 mA60\text{ mA}
According to Ohm's law, current equals voltage divided by resistance (I=V/RI = V / R). Converting 1.2 kΩ1.2\text{ k}\Omega to base units gives 1200 Ω1200\text{ }\Omega. Dividing 72 V72\text{ V} by 1200 Ω1200\text{ }\Omega produces 0.06 A0.06\text{ A}, which is equivalent to 60 mA60\text{ mA}.

Adım Adım Çözüm

1
Convert the given resistance from kilo-ohms to base ohms
R=1.2 kΩ=1.2×103 Ω=1200 ΩR = 1.2\text{ k}\Omega = 1.2 \times 10^3\text{ }\Omega = 1200\text{ }\Omega
Standard electrical calculations using Ohm's law require values to be expressed in SI base units (volts, amperes, and ohms).
2
Apply Ohm's law formula to solve for current (II)
I=VR=72 V1200 Ω=0.06 AI = \frac{V}{R} = \frac{72\text{ V}}{1200\text{ }\Omega} = 0.06\text{ A}
Current is directly proportional to voltage and inversely proportional to resistance.
3
Convert the current from amperes to milliamperes
I=0.06 A×1000 mA/A=60 mAI = 0.06\text{ A} \times 1000\text{ mA/A} = 60\text{ mA}
Expressing the small current value in milliamperes matches standard electronic measurement conventions.

Anahtar Kavram

Ohm's Law Current Calculation (I=VRI = \frac{V}{R}) with Metric Prefix Conversion

Alternatif Yöntem

Convert the calculation directly using milliamperes: 1 V/1 kΩ=1 mA1\text{ V} / 1\text{ k}\Omega = 1\text{ mA}. Therefore, 72 V/1.2 kΩ=60 mA72\text{ V} / 1.2\text{ k}\Omega = 60\text{ mA}.
Tahmini Süre:1m 0s
Soru 84Soru →

An avionics technician replaces a solid copper grounding wire of length LL and circular diameter dd with a replacement wire made of a resistive alloy. The alloy has 44 times the resistivity of copper (ρalloy=4ρcopper\rho_{\text{alloy}} = 4\rho_{\text{copper}}), and the replacement wire is cut to half the original length (12L\frac{1}{2}L). If the replacement wire must have the exact same electrical resistance as the original copper wire, what must be the diameter of the replacement wire in terms of dd?

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Cevap: 2 d\sqrt{2}\,d

Cevap

2 d\sqrt{2}\,d
Resistance depends on material resistivity and physical dimensions according to R=ρLA=4ρLπd2R = \rho \frac{L}{A} = \frac{4\rho L}{\pi d^2}. Multiplying resistivity by 44 and multiplying length by 12\frac{1}{2} produces a numerator factor of 4×12=24 \times \frac{1}{2} = 2. To keep the overall resistance constant, the denominator area must also increase by a factor of 22. Because cross-sectional area is proportional to the square of diameter (A∝d2A \propto d^2), the diameter must increase by a factor of 2\sqrt{2}, giving 2 d\sqrt{2}\,d.

Adım Adım Çözüm

1
Express the electrical resistance of the original copper wire using its physical dimensions and resistivity.
Rorig=ρcopperLA1=ρcopperLπd24=4ρcopperLπd2R_{\text{orig}} = \rho_{\text{copper}} \frac{L}{A_1} = \rho_{\text{copper}} \frac{L}{\frac{\pi d^2}{4}} = \frac{4\rho_{\text{copper}}L}{\pi d^2}
The resistance of a cylindrical conductor is governed by R=ρLAR = \rho \frac{L}{A}, where circular cross-sectional area is A=πd24A = \frac{\pi d^2}{4}.
2
Express the electrical resistance of the replacement alloy wire in terms of its new parameters ρalloy=4ρcopper\rho_{\text{alloy}} = 4\rho_{\text{copper}}, Lnew=0.5LL_{\text{new}} = 0.5L, and unknown diameter dnewd_{\text{new}}.
Rnew=(4ρcopper)0.5Lπdnew24=4(2ρcopperL)πdnew2=8ρcopperLπdnew2R_{\text{new}} = (4\rho_{\text{copper}}) \frac{0.5L}{\frac{\pi d_{\text{new}}^2}{4}} = \frac{4(2\rho_{\text{copper}}L)}{\pi d_{\text{new}}^2} = \frac{8\rho_{\text{copper}}L}{\pi d_{\text{new}}^2}
Substitute the scaled values of resistivity and length into the conductor resistance equation.
3
Equate the original resistance to the replacement resistance and solve for dnewd_{\text{new}}.
4ρcopperLπd2=8ρcopperLπdnew2  ⟹  1d2=2dnew2  ⟹  dnew2=2d2  ⟹  dnew=2 d\frac{4\rho_{\text{copper}}L}{\pi d^2} = \frac{8\rho_{\text{copper}}L}{\pi d_{\text{new}}^2} \implies \frac{1}{d^2} = \frac{2}{d_{\text{new}}^2} \implies d_{\text{new}}^2 = 2d^2 \implies d_{\text{new}} = \sqrt{2}\,d
The replacement specification mandates identical resistance (Rorig=RnewR_{\text{orig}} = R_{\text{new}}).

Anahtar Kavram

Conductor resistance is directly proportional to resistivity and length, and inversely proportional to the square of conductor diameter (R∝ρLd2R \propto \frac{\rho L}{d^2}).
Tahmini Süre:1m 30s
Soru 85Soru →

Match each circuit modification on the left with its resulting effect on circuit current according to Ohm's law on the right.

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Öğeler

Source voltage is doubled while circuit resistance remains constant
Circuit resistance is doubled while source voltage remains constant
Both source voltage and circuit resistance are doubled simultaneously
Source voltage is halved while circuit resistance is doubled

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Cevap

Doubling voltage with constant resistance doubles current; doubling resistance with constant voltage halves current; doubling both voltage and resistance keeps current unchanged; halving voltage while doubling resistance reduces current to one-fourth.
Ohm's law states I=VRI = \frac{V}{R}. Analyzing each case: V×2  ⟹  I×2V \times 2 \implies I \times 2; R×2  ⟹  I×0.5R \times 2 \implies I \times 0.5; both ×2  ⟹  I×1\times 2 \implies I \times 1; and V×0.5V \times 0.5 combined with R×2  ⟹  I×0.25R \times 2 \implies I \times 0.25.

Adım Adım Çözüm

1
Recall Ohm's law relating current, voltage, and resistance
I=VRI = \frac{V}{R}
Current equals voltage divided by resistance.
2
Apply proportional reasoning for each condition
Direct proportionality for voltage, inverse proportionality for resistance.
Changes in numerator directly multiply the result, while changes in denominator inversely divide the result.

Anahtar Kavram

Ohm's law governs the relationship between voltage, current, and resistance (I=VRI = \frac{V}{R}), establishing that current is directly proportional to voltage and inversely proportional to resistance.
Tahmini Süre:45s
Soru 86Soru →

In direct current (DC) electronics, which of the following statements correctly describes the fundamental distinction between electromotive force (EMF) and electrical current?

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Cevap: Electromotive force is the electrical potential difference that drives charge carriers, whereas electrical current is the rate at which charge flows through the circuit.

Cevap

Electromotive force is the electrical potential difference that drives charge carriers, whereas electrical current is the rate at which charge flows through the circuit.
Electromotive force (EMF) is the electric potential difference produced by a source (such as a battery or generator) that provides the energy and pressure needed to push free electrons through a closed circuit. Electrical current is the rate of flow of that electric charge, typically measured in amperes (coulombs per second).

Adım Adım Çözüm

1
Identify the definition and physical role of electromotive force (EMF).
EMF represents the electric potential difference (measured in volts) generated by a source, acting as the electrical pressure that drives charges.
Establishing the source of electrical push is required to distinguish cause from effect in an electrical circuit.
2
Identify the definition and physical role of electrical current.
Current represents the flow rate of electric charge (measured in amperes, or coulombs per second) passing through a conductor.
Differentiating the driving force from the resulting flow clarifies the core relationship between voltage and current.
3
Evaluate the statements to select the one that accurately pairs both concepts.
The statement describing EMF as the driving potential difference and current as the rate of charge flow is correct.
This matches standard electrical definitions without confusing units, formulas, or circuit types.

Anahtar Kavram

Electromotive Force (EMF) vs. Current
Tahmini Süre:1m 0s
Soru 87Soru →

Match each electromagnetic component or induction phenomenon with its precise operational principle.

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Öğeler

Electromagnetic Relay
Inductive Back-EMF
Step-Down Transformer
Ferromagnetic Core Solenoid

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Cevap

Electromagnetic Relay pairs with low-current coil energization pulling isolated contacts; Inductive Back-EMF pairs with counter-EMF resisting instantaneous current changes; Step-Down Transformer pairs with mutual induction reducing voltage while increasing current capacity; Ferromagnetic Core Solenoid pairs with concentrating flux lines via high permeability to maximize mechanical force.
Each electromagnetic concept directly reflects its physical mechanism: relays isolate circuits through electromagnetically actuated mechanical contacts, back-EMF generates an opposing counter-voltage during current shifts, step-down transformers exchange voltage for current via mutual AC induction, and iron-core solenoids maximize pull force by concentrating magnetic flux density.

Adım Adım Çözüm

1
Analyze the electrical isolation and mechanical switching mechanism of an electromagnetic relay.
Identify that a relay enables a low-power circuit to safely switch a separate heavy-duty circuit via magnetic pull on an armature.
Relays function as electrically operated mechanical switches where the control coil is isolated from the load contacts.
2
Apply Lenz's Law and Faraday's Law to evaluate inductive back-EMF behavior.
Determine that the self-induced voltage always acts in the opposite polarity to the change in circuit current (V=−LdidtV = -L \frac{di}{dt}).
Inductors store energy in magnetic fields and resist rapid current fluctuations by generating counter-electromotive force.
3
Examine power conservation and mutual induction relationships in a step-down transformer.
Confirm that fewer secondary turns reduce secondary voltage while stepping up current proportionally under AC operation.
Assuming ideal transformer efficiency (Pin=PoutP_{in} = P_{out}), a decrease in voltage requires an inverse, proportional increase in current.
4
Assess the effect of magnetic core material on solenoid pulling performance.
Recognize that a ferromagnetic core lowers magnetic reluctance and concentrates flux lines, amplifying linear physical force.
High-permeability materials channel magnetic flux far more effectively than air, boosting magnetic field density.

Anahtar Kavram

Fundamental principles of electromagnetism, self-induction, mutual induction, and magnetic flux concentration
Tahmini Süre:2m 0s
Soru 88Soru →

When a direct-current (DC) circuit is energized, which of the following statements correctly describes the physical movement of electrical charge through a solid metallic conductor?

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Cevap: Electrons move from the negative terminal toward the positive terminal.

Cevap

Electrons move from the negative terminal toward the positive terminal.
In solid conductors like copper wire, electrical current is physically composed of negatively charged free electrons drifting away from the negative power source terminal and toward the positive terminal.

Adım Adım Çözüm

1
Identify the charge carriers responsible for current in solid metal conductors.
Free (valence) electrons carry electrical charge in metals, while positive atomic nuclei remain stationary in the lattice.
Establishing the physical particle involved distinguishes electron flow from atomic or ionic movement.
2
Determine the direction of electrostatic force exerted on negative charges by the power source.
Negatively charged electrons are repelled by the negative terminal and attracted to the positive terminal.
Like charges repel and opposite charges attract, establishing the direction of electron drift.

Anahtar Kavram

Physical current in metallic conductors consists of electron flow traveling from negative potential to positive potential.
Tahmini Süre:30s
Soru 89Soru →

Match each voltage and electromotive force (EMF) concept on the left with its correct technical definition or operating behavior on the right.

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Öğeler

Electromotive Force (EMF)
Terminal Voltage
Internal Voltage Drop
Open-Circuit Voltage

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Cevap

Electromotive Force (EMF) pairs with total electrical energy generated per unit charge; Terminal Voltage pairs with actual electrical potential delivered across the load under current; Internal Voltage Drop pairs with potential difference consumed within the source due to internal resistance; Open-Circuit Voltage pairs with potential difference measured across terminals when no current is drawn.
Electromotive Force (EMF) represents the total energy supplied per unit charge inside an electrical generator or chemical cell. Under no-load conditions (zero current), the open-circuit voltage equals the EMF. When connected to a load, current produces an internal voltage drop across the internal resistance, resulting in a lower measured terminal voltage available to the circuit.

Adım Adım Çözüm

1
Identify the fundamental energy conversion definition of source potential
Electromotive Force (EMF) corresponds to the total work converted to electrical energy per unit charge (1 Volt=1 Joule per Coulomb1\text{ Volt} = 1\text{ Joule per Coulomb}).
EMF defines the driving force created by non-electrical mechanisms before any internal losses occur.
2
Differentiate between loaded operating potential and no-load terminal potential
Terminal Voltage is the operational output under load, whereas Open-Circuit Voltage is the static terminal measurement when current is zero.
When an external circuit is closed, current flowing through internal resistance reduces terminal voltage below the generated EMF.
3
Isolate the effect of internal resistance on source performance
Internal Voltage Drop represents the product of load current and internal resistance (I⋅rintI \cdot r_{int}).
Internal losses account for the discrepancy between total EMF and measured terminal voltage under load.

Anahtar Kavram

Distinction between source electromotive force, internal resistance drop, and loaded versus unloaded terminal voltage
Tahmini Süre:1m 0s
Soru 90Soru →

A copper feed wire in a naval radar subsystem has a length of 50 m50\text{ m}, a circular cross-sectional diameter of 2.0 mm2.0\text{ mm}, and a measured DC resistance of 0.27 Ω0.27\ \Omega. During maintenance, this line is replaced with an alloy wire that has a resistivity 4.04.0 times that of copper, a total length of 75 m75\text{ m}, and a diameter of 3.0 mm3.0\text{ mm}. What is the electrical resistance of the replacement wire in ohms?

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Cevap: 0.72

Cevap

The electrical resistance of the replacement wire is 0.72 ohms.
Electrical resistance is given by the formula R=ρLA=4ρLπd2R = \rho \frac{L}{A} = \frac{4\rho L}{\pi d^2}. Comparing the replacement wire to the original: resistivity increases by a factor of 4.04.0, length increases by a factor of 7550=1.5\frac{75}{50} = 1.5, and cross-sectional area increases by a factor of (3.02.0)2=2.25\left(\frac{3.0}{2.0}\right)^2 = 2.25. Combining these factors gives an overall resistance change factor of 4.0×1.52.25=83\frac{4.0 \times 1.5}{2.25} = \frac{8}{3}. Multiplying the baseline resistance of 0.27 Ω0.27\ \Omega by 83\frac{8}{3} gives exactly 0.72 Ω0.72\ \Omega.

Adım Adım Çözüm

1
Relate electrical resistance to material resistivity and conductor dimensions.
R=ρLA=4ρLπd2R = \rho \frac{L}{A} = \frac{4\rho L}{\pi d^2}
Resistance is directly proportional to resistivity and length, and inversely proportional to cross-sectional area (which depends on the square of the diameter).
2
Determine the relative scaling factors for resistivity, length, and diameter.
Resistivity factor =4.0= 4.0; Length factor =7550=1.5= \frac{75}{50} = 1.5; Diameter factor =3.02.0=1.5= \frac{3.0}{2.0} = 1.5
Proportional scaling allows direct calculation without calculating intermediate microscopic values.
3
Calculate the combined scaling factor for resistance.
R2R1=ρ2ρ1×L2L1×(d1d2)2=4.0×1.5×(11.5)2=4.01.5=83\frac{R_2}{R_1} = \frac{\rho_2}{\rho_1} \times \frac{L_2}{L_1} \times \left(\frac{d_1}{d_2}\right)^2 = 4.0 \times 1.5 \times \left(\frac{1}{1.5}\right)^2 = \frac{4.0}{1.5} = \frac{8}{3}
Area scales quadratically with diameter, so diameter increase reduces resistance by a factor of 1.52=2.251.5^2 = 2.25.
4
Calculate the final resistance of the replacement wire.
R2=0.27 Ω×83=0.72 ΩR_2 = 0.27\ \Omega \times \frac{8}{3} = 0.72\ \Omega
Multiplying the original resistance by the overall scaling factor yields the new total resistance.

Anahtar Kavram

Dependence of electrical resistance on resistivity, conductor length, and cross-sectional area

Alternatif Yöntem

Calculate the resistivity of copper first using ρCu=R1A1L1=0.27×π(0.001)250≈1.696×10−8 Ω⋅m\rho_{\text{Cu}} = \frac{R_1 A_1}{L_1} = \frac{0.27 \times \pi (0.001)^2}{50} \approx 1.696 \times 10^{-8}\ \Omega\cdot\text{m}. Then calculate ρalloy=4.0×ρCu≈6.786×10−8 Ω⋅m\rho_{\text{alloy}} = 4.0 \times \rho_{\text{Cu}} \approx 6.786 \times 10^{-8}\ \Omega\cdot\text{m}, and compute R2=ρalloy×75π(0.0015)2=0.72 ΩR_2 = \frac{\rho_{\text{alloy}} \times 75}{\pi (0.0015)^2} = 0.72\ \Omega.
Tahmini Süre:1m 30s
Soru 91Soru →

A direct current (DC) heating element is connected to a 120 V120\text{ V} power supply. If an ammeter measures a current of 4 A4\text{ A} flowing through the element, what is its electrical resistance?

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Cevap: 30 Ω30\text{ }\Omega

Cevap

30 Ω30\text{ }\Omega
According to Ohm's law, electrical resistance (RR) is defined as the ratio of voltage (VV) across a component to the current (II) passing through it: R=VIR = \frac{V}{I}. Substituting 120 V120\text{ V} and 4 A4\text{ A} gives R=1204=30 ΩR = \frac{120}{4} = 30\text{ }\Omega.

Adım Adım Çözüm

1
Identify the given values and the required quantity
Voltage V=120 VV = 120\text{ V}, Current I=4 AI = 4\text{ A}, Resistance RR is unknown
Establishing the known circuit parameters determines which Ohm's law formula variation to use.
2
Apply Ohm's law rearranged to solve for resistance: R=VIR = \frac{V}{I}
R=120 V4 A=30 ΩR = \frac{120\text{ V}}{4\text{ A}} = 30\text{ }\Omega
Resistance represents the opposition to current flow and is calculated as the ratio of electromotive force to electrical current.

Anahtar Kavram

Ohm's Law Resistance Calculation (R=VIR = \frac{V}{I})
Tahmini Süre:45s
Soru 92Soru →

A solid copper wire used in an industrial application has a length of 200 meters200\text{ meters} and a cross-sectional area of 0.85 mm20.85 \, mm^2. The resistivity of copper at 20∘C20^\circ C is 1.7×10−8 Ω⋅m1.7 \times 10^{-8} \, \Omega\cdot m, and its temperature coefficient of resistance is 0.004 per ∘C0.004 \text{ per } ^\circ C. What is the resistance of this wire, in ohms, when its operating temperature reaches 70∘C70^\circ C?

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Cevap: 4.8

Cevap

4.8
The solution requires a synthesis of two core resistance principles. First, the baseline resistance is found by dividing the length by the area (converted to square meters) and multiplying by the resistivity, yielding 4.0 ohms. Second, the 50°C temperature increase is multiplied by the coefficient (0.004) to find a 20% increase in total resistance, raising the final value to 4.8 ohms.

Adım Adım Çözüm

1
Convert the cross-sectional area from mm2mm^2 to m2m^2.
0.85 mm2=0.85×10−6 m20.85 \, mm^2 = 0.85 \times 10^{-6} \, m^2
Standard SI units must be used to cancel with the meters in the resistivity value.
2
Calculate the resistance at 20∘C20^\circ C (R20R_{20}) using Pouillet's law (R=ρLAR = \rho \frac{L}{A}).
R20=(1.7×10−8)×2000.85×10−6=4.0 ΩR_{20} = (1.7 \times 10^{-8}) \times \frac{200}{0.85 \times 10^{-6}} = 4.0 \, \Omega
This establishes the baseline resistance of the wire before temperature effects are considered.
3
Calculate the change in temperature (ΔT\Delta T).
ΔT=70∘C−20∘C=50∘C\Delta T = 70^\circ C - 20^\circ C = 50^\circ C
The temperature coefficient is applied to the difference between the operating temperature and the reference temperature.
4
Calculate the new resistance at 70∘C70^\circ C using the temperature coefficient formula: Rnew=Rref[1+α(ΔT)]R_{new} = R_{ref}[1 + \alpha(\Delta T)].
R70=4.0×[1+0.004×50]=4.0×[1+0.2]=4.0×1.2=4.8 ΩR_{70} = 4.0 \times [1 + 0.004 \times 50] = 4.0 \times [1 + 0.2] = 4.0 \times 1.2 = 4.8 \, \Omega
As temperature increases, the resistance of a standard conductor like copper increases proportionally.

Anahtar Kavram

Calculating absolute resistance using dimensions and resistivity, followed by applying temperature coefficients.
Tahmini Süre:3m 0s
Soru 93Soru →

Match each direct current (DC) circuit scenario on the left with its corresponding calculated electrical quantity on the right using Ohm's law (V=I×RV = I \times R).

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Öğeler

A 120 V120\text{ V} line connected across a load with a resistance of 2.4 kΩ2.4\text{ k}\Omega
A 5 V5\text{ V} logic circuit branch drawing a current of 20 mA20\text{ mA}
A current of 400 mA400\text{ mA} flowing through a 50 Ω50\text{ }\Omega heating element
A 36 V36\text{ V} industrial sensor loop carrying a current of 3 mA3\text{ mA}

Eşleşmeler

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Cevap

The 120 V120\text{ V} load with 2.4 kΩ2.4\text{ k}\Omega matches the resulting current of 50 mA50\text{ mA}; the 5 V5\text{ V} circuit drawing 20 mA20\text{ mA} matches the circuit resistance of 250 Ω250\text{ }\Omega; the 400 mA400\text{ mA} current through 50 Ω50\text{ }\Omega matches the voltage drop of 20 V20\text{ V}; and the 36 V36\text{ V} loop carrying 3 mA3\text{ mA} matches the loop resistance of 12 kΩ12\text{ k}\Omega.
Each circuit condition correctly maps to its target electrical parameter by converting metric prefixes (1 kΩ=1000 Ω1\text{ k}\Omega = 1000\text{ }\Omega, 1 mA=0.001 A1\text{ mA} = 0.001\text{ A}) and applying the appropriate algebraic form of Ohm's law: I=VRI = \frac{V}{R}, R=VIR = \frac{V}{I}, and V=I×RV = I \times R.

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1
Calculate current for the 120 V120\text{ V}, 2.4 kΩ2.4\text{ k}\Omega circuit
I=120 V2400 Ω=0.05 A=50 mAI = \frac{120\text{ V}}{2400\text{ }\Omega} = 0.05\text{ A} = 50\text{ mA}
Ohm's law states I=VRI = \frac{V}{R}, requiring resistance in fundamental ohms (1 kΩ=1000 Ω1\text{ k}\Omega = 1000\text{ }\Omega).
2
Calculate resistance for the 5 V5\text{ V}, 20 mA20\text{ mA} circuit branch
R=5 V0.02 A=250 ΩR = \frac{5\text{ V}}{0.02\text{ A}} = 250\text{ }\Omega
Rearranging Ohm's law gives R=VIR = \frac{V}{I}, requiring current in amperes (20 mA=0.02 A20\text{ mA} = 0.02\text{ A}).
3
Calculate voltage drop across the 50 Ω50\text{ }\Omega element carrying 400 mA400\text{ mA}
V=0.4 A×50 Ω=20 VV = 0.4\text{ A} \times 50\text{ }\Omega = 20\text{ V}
Ohm's law formula V=I×RV = I \times R computes potential difference when current and resistance are known.
4
Calculate total resistance for the 36 V36\text{ V}, 3 mA3\text{ mA} sensor loop
R=36 V0.003 A=12000 Ω=12 kΩR = \frac{36\text{ V}}{0.003\text{ A}} = 12000\text{ }\Omega = 12\text{ k}\Omega
Applying R=VIR = \frac{V}{I} with 3 mA=0.003 A3\text{ mA} = 0.003\text{ A} yields 12000 Ω12000\text{ }\Omega, or 12 kΩ12\text{ k}\Omega.

Anahtar Kavram

Ohm's law mathematically relates voltage (VV), current (II), and resistance (RR) via V=I×RV = I \times R, I=VRI = \frac{V}{R}, and R=VIR = \frac{V}{I}, requiring consistent base metric units.
Tahmini Süre:1m 15s
Soru 94Soru →

A technician wraps two separate copper wire coils, Coil 1 and Coil 2, around a single soft iron core. Coil 1 is connected to a steady 12V DC power supply, and the current has reached a steady state. Coil 2 is connected only to a sensitive digital voltmeter. If the technician rapidly pulls the soft iron core completely out of the coils while Coil 1 remains connected to the power supply, which of the following best describes the reading on the voltmeter during the exact moment the core is moving?

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Cevap: A voltage reading that spikes momentarily and then returns to zero, because the sudden decrease in magnetic permeability causes a rapid change in magnetic flux.

Cevap

The correct answer is a voltage reading that spikes momentarily and then returns to zero, because the sudden decrease in magnetic permeability causes a rapid change in magnetic flux.
Electromagnetic induction requires a changing magnetic flux over time. While a steady DC current normally produces a constant, unchanging magnetic field, the physical act of rapidly removing the highly permeable iron core drastically reduces the magnetic flux. This rapid change in flux induces a temporary voltage spike in the secondary coil. The induction ceases as soon as the core is completely removed, because the flux becomes constant again, returning the voltmeter reading to zero.

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1
Analyze the initial steady state of the circuit.
Coil 1 produces a constant magnetic flux that is concentrated by the soft iron core. Because the flux is not changing over time, the induced voltage in Coil 2 is zero.
Faraday's Law of Induction requires a changing magnetic field to induce an electromotive force (EMF).
2
Evaluate the physical change caused by the technician's action.
The technician removes the soft iron core, replacing a material with high magnetic permeability with air, which has very low magnetic permeability.
Magnetic permeability directly determines how well a material can support the formation of a magnetic field within itself.
3
Determine the effect of this physical change on the magnetic flux.
The total magnetic flux passing through both coils drops rapidly as the highly permeable core is removed.
Less permeability means weaker magnetic field strength for the same amount of current.
4
Apply Faraday's Law to the changing magnetic flux.
The rapidly decreasing magnetic flux induces a temporary voltage (a spike) in Coil 2.
An EMF is induced in a coil whenever there is a change in magnetic flux passing through it, proportional to the rate of change (E=−N×ΔΦΔtE = -N \times \frac{\Delta\Phi}{\Delta t}).
5
Determine the final state after the core is completely removed.
The magnetic flux stabilizes at a new, much lower constant value. Since the flux is no longer changing, the induced voltage in Coil 2 returns to zero.
Induction only occurs during the period of change.

Anahtar Kavram

Faraday's Law of Induction and Magnetic Permeability
Soru 95Soru →

In standard metallic conductors such as copper wire, electric current consists of the directed movement of free valence electrons drifting through the material.

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Cevap: True

Cevap

True
The statement is true because the physical flow of electric current in metallic conductors like copper is carried exclusively by free valence electrons drifting through the atomic lattice under an applied electric field.

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1
Identify the charge carriers present in solid metallic conductors.
Metals have an atomic structure characterized by a lattice of fixed positive ions surrounded by loosely held, mobile valence electrons.
Determining which atomic particles are free to move establishes the physical mechanism of conduction.
2
Evaluate the particle movement that constitutes electrical current.
When a voltage source is applied, these free valence electrons drift collectively through the conductor, which defines the physical flow of electric current.
Atomic nuclei remain locked in the crystal lattice while only the free electrons travel through the wire.

Anahtar Kavram

Physical electric current in solid metallic conductors is the collective drift of free valence electrons.
Tahmini Süre:30s
Soru 96Soru →

A technician connects a primary coil wound around a soft iron core to a constant 12 V12\text{ V} direct current (DC) supply, establishing a steady magnetic field through an adjacent secondary coil. Which of the following modifications will produce a continuous, sustained output voltage across the secondary coil?

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Cevap: Replacing the DC supply with an alternating current (AC) source to continuously vary the magnetic flux

Cevap

Replacing the DC supply with an alternating current (AC) source to continuously vary the magnetic flux
According to Faraday's law of induction, an electromotive force (EMF) is only induced when there is relative motion or a changing magnetic flux linking the conductor. An alternating current (AC) continuously cycles in amplitude and direction, generating an expanding and collapsing magnetic field that sustains a continuous output voltage in the secondary coil.

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1
Apply Faraday's Law of Electromagnetic Induction
The induced electromotive force is given by E=−NdΦdt\mathcal{E} = -N \frac{d\Phi}{dt}, where dΦdt\frac{d\Phi}{dt} represents the rate of change of magnetic flux.
Induction strictly depends on a dynamic, changing magnetic field rather than a static magnetic field.
2
Evaluate the magnetic field produced by steady DC
A steady direct current creates a constant magnetic flux (dΦdt=0\frac{d\Phi}{dt} = 0), producing 0 V0\text{ V} across the secondary winding in steady state.
Static direct currents cannot sustain continuous transformer action or mutual induction.
3
Determine the condition for continuous, sustained induction
Supplying alternating current (AC) causes the magnetic flux to expand and collapse continuously, providing a perpetual non-zero dΦdt\frac{d\Phi}{dt}.
Continuous induction requires a continuously oscillating or varying current source.

Anahtar Kavram

Electromagnetic Induction and Time-Varying Magnetic Flux
Tahmini Süre:1m 0s
Soru 97Soru →

A direct current (DC) solenoid valve in an industrial pneumatic system has an internal coil resistance of 15 Ω15\text{ }\Omega. When connected to a 30 V30\text{ V} DC power supply, what is the current flowing through the solenoid coil in amperes (A\text{A})?

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Cevap: 2

Cevap

The current flowing through the solenoid coil is 2 A2\text{ A}.
According to Ohm's law, electrical current (II) equals voltage (VV) divided by resistance (RR). Substituting the given values yields I=30 V15 Ω=2 AI = \frac{30\text{ V}}{15\text{ }\Omega} = 2\text{ A}.

Adım Adım Çözüm

1
Identify the given circuit parameters
Voltage V=30 VV = 30\text{ V}, Resistance R=15 ΩR = 15\text{ }\Omega
Extract the given values to identify which Ohm's law formula variation is required.
2
State Ohm's law formula for current
I=VRI = \frac{V}{R}
Current is directly proportional to applied voltage and inversely proportional to total circuit resistance.
3
Substitute the values and evaluate
I=30 V15 Ω=2 AI = \frac{30\text{ V}}{15\text{ }\Omega} = 2\text{ A}
Dividing 3030 by 1515 yields the circuit current in amperes.

Anahtar Kavram

Ohm's Law (I=VRI = \frac{V}{R})
Tahmini Süre:45s
Soru 98Soru →

In electronics and solid-state physics, materials are fundamentally classified by the number of valence electrons in their outermost atomic shell and their conductivity characteristics. An element contains exactly four valence electrons in its outer shell, forming covalent bonds in a crystalline lattice that exhibits moderate resistivity at room temperature and increased conductivity as temperature rises. Which of the following substances possesses these specific atomic and electrical properties?

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Cevap: Silicon

Cevap

Silicon, because it is a semiconductor with four valence electrons in its outer shell and a negative temperature coefficient of resistance.
Silicon is an elemental semiconductor belonging to Group IV of the periodic table, meaning each atom has four valence electrons. In a solid crystal lattice, these four electrons form covalent bonds with adjacent atoms. At room temperature, thermal excitation frees a small fraction of these electrons across the narrow energy gap into the conduction band, giving silicon an intermediate level of conductivity that increases as thermal energy rises.

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1
Identify the material category based on the outer shell valence electron count.
An atom with exactly four valence electrons is classified as a semiconductor (Group IV element).
Good conductors typically have 1 to 3 valence electrons, semiconductors have exactly 4, and insulators generally have 5 to 8 tightly held valence electrons.
2
Evaluate the electrical conduction behavior described in the scenario.
The material exhibits moderate resistivity and a negative temperature coefficient of resistance (conductivity increases with temperature).
In intrinsic semiconductors, added thermal energy breaks covalent bonds, releasing electron-hole pairs into the conduction band to facilitate charge flow.
3
Match the specified atomic and electrical characteristics to the given material choices.
Silicon is a Group IV semiconductor, whereas copper and aluminum are conductors and mica is an insulator.
Silicon has an atomic number of 14 with an electron configuration of 2-8-4, giving it precisely four valence electrons.

Anahtar Kavram

Semiconductor atomic structure and valence electron properties
Tahmini Süre:1m 15s
Soru 99Soru →

A direct current (DC) emergency lighting circuit operates from a 28 V28\text{ V} power supply. An in-line ammeter measures a steady current flow of 350 mA350\text{ mA} through the circuit. What is the total electrical resistance of the lighting circuit?

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Cevap: 80 Ω80\text{ }\Omega

Cevap

The total electrical resistance of the lighting circuit is 80 Ω80\text{ }\Omega.
According to Ohm's law, resistance is found by dividing voltage by current (R=V/IR = V / I). Converting 350 mA350\text{ mA} into amperes yields 0.35 A0.35\text{ A}. Dividing 28 V28\text{ V} by 0.35 A0.35\text{ A} gives the correct value of 80 Ω80\text{ }\Omega.

Adım Adım Çözüm

1
Convert the current measurement from milliamperes to amperes.
I=350 mA=3501000 A=0.35 AI = 350\text{ mA} = \frac{350}{1000}\text{ A} = 0.35\text{ A}
Standard Ohm's law calculations require current to be in base SI units (amperes) to produce resistance in ohms.
2
Rearrange Ohm's law (V=I×RV = I \times R) to solve for resistance (RR).
R=VIR = \frac{V}{I}
Resistance equals the electromotive force (voltage) across the circuit divided by the resulting current flow.
3
Substitute the known voltage and converted current values into the rearranged formula.
R=28 V0.35 A=280035 Ω=80 ΩR = \frac{28\text{ V}}{0.35\text{ A}} = \frac{2800}{35}\text{ }\Omega = 80\text{ }\Omega
Dividing 28 V28\text{ V} by 0.35 A0.35\text{ A} determines the load resistance in ohms.

Anahtar Kavram

Ohm's Law (V=I×RV = I \times R) defines the mathematical relationship between voltage, current, and resistance in DC circuits, requiring proper metric unit conversion before calculation.
Tahmini Süre:1m 0s
Soru 100Soru →

A remote weather station is powered by a battery bank containing two identical parallel branches. Each branch is composed of three 12 V12\text{ V} batteries connected in series aiding. What total electromotive force (EMF) is delivered across the main output terminals of the bank?

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Cevap: 36 V36\text{ V}

Cevap

36 V36\text{ V}
In a battery bank containing series strings wired in parallel, each series branch sums the voltages of its three 12 V12\text{ V} batteries to produce 36 V36\text{ V} (12 V+12 V+12 V=36 V12\text{ V} + 12\text{ V} + 12\text{ V} = 36\text{ V}). Connecting two identical 36 V36\text{ V} strings in parallel keeps the potential difference across the output terminals at 36 V36\text{ V} while doubling current capacity.

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1
Calculate the total electromotive force of a single series-connected branch.
12 V+12 V+12 V=36 V12\text{ V} + 12\text{ V} + 12\text{ V} = 36\text{ V}
When DC voltage sources are wired in series aiding, their individual voltages add directly.
2
Determine the combined electromotive force delivered by the parallel configuration.
36 V36\text{ V}
Connecting identical voltage branches in parallel provides the same terminal voltage as a single branch while expanding overall current capacity.

Anahtar Kavram

Series-parallel voltage principles dictate that series-connected sources sum their electromotive forces, whereas connecting identical strings in parallel maintains that branch voltage across the load terminals.
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