Official curriculum roadmap, subject/topic distribution, negative marking rules, pacing guidelines, and solved sample questions.
🎯 Mapped Subjects & Topic Question Distribution
Total Question Pool100%
20 MCQs
Combined Active Syllabus
Op-Amps & 555 Timers
20 MCQs
Topic Pool
📊 Question Pool Structure
20 MCQs across fundamental, intermediate, and advanced concept tiers.
⚡ Recommended Pacing
45 to 60 seconds per MCQ. Flag complex problems and preserve 10 minutes for final revision.
⚖️ Scoring & Negative Marking
+1 mark per correct answer. In competitive tests with negative marking, -0.25 applies for incorrect guesses.
💡 Strategic Preparation & Exam Hall Guidelines
To maximize your score on Op-Amps & 555 Timers, candidates are advised to follow a structured three-pass approach. In the First Pass, solve all direct recall and formula-based questions within 30 seconds each to secure foundational marks. In the Second Pass, tackle multi-step analytical and quantitative reasoning problems. In the Third Pass, review marked questions and verify calculations.
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An ideal operational amplifier (Op-Amp) has which set of theoretical electrical characteristics?
AInfinite input impedance (Rin = inf), zero output impedance (Rout = 0), infinite open-loop voltage gain (Aol = inf), infinite bandwidth, and zero input offset voltage
BZero input impedance and infinite output impedance
CGain of 1 and bandwidth of 100 kHz
DInverting gain only with high noise figure
✓ Correct Answer:A - Infinite input impedance (Rin = inf), zero output impedance (Rout = 0), infinite open-loop voltage gain (Aol = inf), infinite bandwidth, and zero input offset voltage
📖 Step-by-Step Solution & Conceptual Rationale:
An ideal op-amp draws zero input current (Rin = inf), can drive any load without voltage drop (Rout = 0), has infinite differential gain, infinite bandwidth, infinite CMRR, infinite slew rate, and perfect symmetry (Vout = 0 when V+ = V-).
The 'Virtual Ground' concept in an inverting op-amp configuration is valid only when:
ANegative feedback is present and the op-amp operates in its linear (un-saturated) active region
BPositive feedback is applied
CThe op-amp output is saturated at the power rail
DBoth inputs are tied to VCC
✓ Correct Answer:A - Negative feedback is present and the op-amp operates in its linear (un-saturated) active region
📖 Step-by-Step Solution & Conceptual Rationale:
With negative feedback, Vout = Aol * (V+ - V-). Since Aol is enormous (~10^5 to 10^6) and Vout is finite, the differential input voltage (V+ - V-) = Vout / Aol ≈ 0. If the non-inverting terminal V+ is connected to ground (0 V), the inverting terminal V- is held at 0 V ('virtual ground') without being physically wired to ground.
The closed-loop voltage gain of a non-inverting op-amp amplifier with ground resistor R1 and feedback resistor Rf is:
AAv = 1 + (Rf / R1)
BAv = -Rf / R1
CAv = Rf / R1
DAv = 1 - (Rf / R1)
✓ Correct Answer:A - Av = 1 + (Rf / R1)
📖 Step-by-Step Solution & Conceptual Rationale:
Voltage at the inverting node tracks input voltage by virtual short: V- = V+ = Vin. From the voltage divider across feedback path: Vin = Vout * [R1 / (R1 + Rf)]. Solving gives Av = Vout / Vin = 1 + (Rf / R1). Gain is strictly >= 1 and non-inverting.
An op-amp Voltage Follower (Buffer) is constructed by setting Rf = 0 and R1 = infinity. Its voltage gain, input impedance, and output impedance are:
AAv = 1, Rin ≈ infinity, Rout ≈ 0
BAv = -1, Rin = 0, Rout = infinity
CAv = 100, Rin = 1 kΩ, Rout = 50 Ω
DAv = 0, Rin = 0, Rout = 0
✓ Correct Answer:A - Av = 1, Rin ≈ infinity, Rout ≈ 0
📖 Step-by-Step Solution & Conceptual Rationale:
For a voltage follower, direct negative feedback forces Vout = Vin (Av = 1). It draws zero current from signal sources (Rin ≈ 10^12 ohms for FET inputs) while driving heavy loads with near-zero output impedance, making it the ideal unity-gain impedance buffer.
Slew Rate (SR) of an operational amplifier is defined as:
AThe maximum time rate of change of output voltage under large-signal step conditions, expressed in V/μs
BThe ratio of common-mode gain to differential gain
CThe input bias current divided by temperature
DThe frequency at which open-loop gain drops to zero
✓ Correct Answer:A - The maximum time rate of change of output voltage under large-signal step conditions, expressed in V/μs
📖 Step-by-Step Solution & Conceptual Rationale:
Slew Rate SR = (dVout / dt)_max, typically measured in Volts per microsecond (V/μs). It is caused by the finite internal charging current (I_tail) available to charge the internal Miller frequency-compensation capacitor (Cc): SR = I_tail / Cc. Standard 741 has SR ≈ 0.5 V/μs.
What is the Full-Power Bandwidth (fm) of an op-amp with slew rate SR delivering an undistorted sinusoidal output of peak amplitude Vp?
Afm = SR / (2 * pi * Vp)
Bfm = 2 * pi * SR * Vp
Cfm = Vp / SR
Dfm = SR / Vp^2
✓ Correct Answer:A - fm = SR / (2 * pi * Vp)
📖 Step-by-Step Solution & Conceptual Rationale:
For Vout(t) = Vp * sin(2*pi*f*t), maximum rate of change is (dVout/dt)_max = 2*pi*f*Vp. For distortion-free reproduction without slewing (triangular distortion), this must not exceed SR: 2*pi*fm*Vp <= SR, giving fm = SR / (2 * pi * Vp).
An ideal op-amp Integrator circuit has a resistor R connected to the inverting input and a capacitor C in the feedback loop. Its output voltage vout(t) in response to input vin(t) is:
Current through input resistor is i = vin / R. Because no current enters the op-amp input, this current charges the feedback capacitor: i = -C * (dvout / dt). Equating gives dvout/dt = -(1 / RC) * vin, so vout(t) = -(1 / RC) * integral vin(tau) dtau.
Why must a practical op-amp integrator include a high-value feedback resistor (Rf) in parallel with the integrating capacitor C?
ATo limit DC gain and prevent tiny DC input offset voltages and bias currents from integrating continuously and driving the output into saturation
BTo increase high-frequency noise
CTo convert the integrator into a differentiator
DTo eliminate negative feedback
✓ Correct Answer:A - To limit DC gain and prevent tiny DC input offset voltages and bias currents from integrating continuously and driving the output into saturation
📖 Step-by-Step Solution & Conceptual Rationale:
At DC (f = 0), a pure capacitor acts as an open circuit, making the op-amp operate at its massive open-loop gain (~10^5). Any tiny input offset voltage Vio is multiplied by Aol, saturating the output at the power rail. Shunting C with Rf clamps the DC closed-loop gain to -Rf / R1.
An op-amp Differentiator circuit has input capacitor C and feedback resistor R. Its major practical design limitation is:
AGain increases with frequency (Av ∝ omega*R*C), amplifying high-frequency noise and making the circuit prone to instability and oscillation
BIt draws infinite DC current
COutput voltage is zero for all AC inputs
DIt requires dual power supplies
✓ Correct Answer:A - Gain increases with frequency (Av ∝ omega*R*C), amplifying high-frequency noise and making the circuit prone to instability and oscillation
📖 Step-by-Step Solution & Conceptual Rationale:
Differentiator gain magnitude is |Av| = omega * R * C. High-frequency noise components are amplified violently, and the 90-degree phase lead combined with internal op-amp poles can induce Barkhausen oscillation. Practical differentiators add a small series input resistor and feedback capacitor to roll off high-frequency gain.
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