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Past Questions — 2024

MES Jr. Grade • 2024 • Paper-II

For an ideal full-wave rectifier without filter, feeds a 1 kΩ load from a 230 V AC source. Find the average DC output voltage.

MES Jr. Grade • 2024 • Paper-II

Reverse collector saturation current ICBO is:

A) Collector current when emitter current is zero
B) Collector current when base current is zero
C) Same as reverse saturation current
D) Collector current when either emitter or base current is zero
The term ICBO stands for 'Collector-Base leakage current with the Emitter Open'. In a Bipolar Junction Transistor (BJT), ICBO is the current that flows from the collector to the base when the collector-base junction is reverse-biased and the emitter terminal is left open (open-circuited). 1. When the emitter is open, the emitter current (IE) is zero. 2. Since the emitter is open and the base-emitter junction is not forward-biased, the base current (IB) is also zero. 3. Therefore, ICBO represents the leakage current flowing through the reverse-biased collector-base junction when both IE = 0 and IB = 0. Analyzing the options: - Option (a) is partially correct but incomplete. - Option (b) is partially correct but incomplete. - Option (c) is too vague as 'reverse saturation current' could refer to any PN junction (like CEO). - Option (d) is the most comprehensive and accurate definition, as it specifies that the current flows when the other two terminals (emitter or base) are not contributing current to the circuit.
MES Jr. Grade • 2024 • Paper-II

How do we obtain sinusoidal output out of a class B amplifier?

A) By using non-sinusoidal inputs
B) By utilizing two transistors
C) By biasing it in the active region
D) By adding a capacitor to the output
A Class B amplifier is designed such that the transistor conducts for only one half-cycle (180 degrees) of the input sinusoidal signal. If a single transistor is used, the output is a half-wave rectified sine wave, which contains significant distortion. To obtain a full sinusoidal output, a 'Push-Pull' configuration is used. This involves utilizing two transistors: one (NPN) to amplify the positive half-cycle and another (PNP) to amplify the negative half-cycle. By combining the outputs of these two transistors, the full sinusoidal waveform is reconstructed. Analysis of other options: - Option (a): Non-sinusoidal inputs would not result in a sinusoidal output; the goal is to amplify a sine wave without distortion. - Option (c): Biasing in the active region is a general requirement for amplification, but specifically for Class B, the transistor is biased at the cutoff point (Q-point at the junction of cutoff and active), not centered in the active region (which would be Class A). - Option (d): A capacitor at the output is used for DC blocking or filtering, but it cannot reconstruct a missing half-cycle of a waveform.
MES Jr. Grade • 2024 • Paper-II

What is the addition of the binary numbers 11011011010 and 010100101?

A) 0111001000
B) 1100110110
C) 11101111111
D) 10011010011
To add the binary numbers 11011011010 and 010100101, we align them by their least significant bits (right-aligned) and perform addition using binary rules (0+0=0, 0+1=1, 1+1=10 (0 carry 1), 1+1+1=11 (1 carry 1)). Step-by-step addition: 11011011010 (11 digits) + 00010100101 (padded with leading zeros to match length) -------------- 11101111111 Detailed breakdown from right to left: 1. 0 + 1 = 1 2. 1 + 0 = 1 3. 0 + 1 = 1 4. 1 + 0 = 1 5. 1 + 0 = 1 6. 0 + 1 = 1 7. 1 + 0 = 1 8. 1 + 1 = 0 (carry 1) 9. 0 + 0 + 1(carry) = 1 10. 1 + 0 = 1 11. 1 + 0 = 1 Result: 11101111111. Comparing with options: - Option a: 0111001000 (Incorrect length and value) - Option b: 1100110110 (Incorrect value) - Option c: 11101111111 (Correct) - Option d: 10011010011 (Incorrect value)
MES Jr. Grade • 2024 • Paper-II

In a Centre tapped full-wave bridge rectifier, the number of diodes conducting at any instant is:

A) 1
B) 2
C) 3
D) 4
First, it is important to clarify a terminology error in the question phrasing: 'Centre tapped full-wave bridge rectifier' is a contradiction. There are two distinct types of full-wave rectifiers: the Center-Tapped Rectifier and the Bridge Rectifier. However, in both configurations, the number of diodes conducting at any single instant is the same. 1. In a Center-Tapped Full-Wave Rectifier: Two diodes are used. During the positive half-cycle, one diode conducts while the other is reverse-biased. During the negative half-cycle, the second diode conducts while the first is reverse-biased. Thus, only 1 diode conducts at a time. 2. In a Bridge Rectifier: Four diodes are used. During the positive half-cycle, a pair of diodes (usually D1 and D3) conducts to provide a path for the current. During the negative half-cycle, the other pair (D2 and D4) conducts. Thus, 2 diodes conduct at a time. Given the options and the specific mention of 'Bridge' in the phrasing, the question is referring to the Bridge Rectifier configuration. In a bridge rectifier, current must flow through two diodes in series to complete the circuit from the transformer to the load and back. Therefore, 2 diodes conduct at any given instant.
MES Jr. Grade • 2024 • Paper-II

What is the maximum possible range of bit-count specifically in n-bit binary counter consisting of ‘n’ number of flip-flops?

A) 0 to 2n
B) 0 to 2n + 1
C) 0 to 2n – 1
D) 0 to 2n+1/2
In digital electronics, a binary counter is constructed using flip-flops, where each flip-flop represents one bit of the binary number. 1. **Number of States**: A single flip-flop has 2 possible states (0 or 1). Therefore, a counter consisting of 'n' flip-flops has a total of 2^n possible distinct states. 2. **Counting Range**: Since binary counting typically starts from 0, the sequence of states begins at 0 and continues up to the (2^n)-th state. 3. **Maximum Value**: Because the first state is 0, the maximum value reached is (Total States - 1). Thus, the maximum count is 2^n - 1. 4. **Range**: The full range of the bit-count is therefore from 0 to 2^n - 1. Note: The options provided in the prompt (2n, 2n+1, 2n-1) are typographical representations of exponents (2^n, 2^{n+1}, 2^n-1), which is common in plain-text exam transcripts. Option 'c' (0 to 2^n - 1) is the standard theoretical range for an n-bit binary counter.
MES Jr. Grade • 2024 • Paper-II

The main advantage of negative feedback in amplifiers is:

A) Increased gain
B) Increased bandwidth
C) Increased distortion
D) Increased input impedance only
Negative feedback occurs when a portion of the output signal is fed back to the input with a 180-degree phase shift. This process involves a trade-off: while it reduces the overall gain of the amplifier, it provides several critical advantages. 1. **Bandwidth**: The gain-bandwidth product of an amplifier remains constant. Since negative feedback reduces the gain, the bandwidth (the range of frequencies over which the amplifier operates effectively) increases proportionally. This is the primary advantage listed in the options. 2. **Gain Stability**: It makes the gain less dependent on temperature variations or component tolerances. 3. **Distortion**: It reduces non-linear distortion and noise, making option (c) incorrect. 4. **Impedance**: While negative feedback can modify input and output impedances, it does not 'only' increase input impedance; the effect depends on the topology (series or shunt) used for feedback. 5. **Gain Reduction**: Negative feedback explicitly decreases the gain, making option (a) incorrect.
MES Jr. Grade • 2024 • Paper-II

Discuss the effect of feedback on noise and distortion in control systems.

MES Jr. Grade • 2024 • Paper-II

Calculate the emf when a coil of 100 turns is subjected to a flux rate of 0.3 tesla/sec.

A) 3
B) 30
C) -30
D) -300
To calculate the electromotive force (emf) induced in a coil, we use Faraday's Law of Electromagnetic Induction. 1. **Given Data:** - Number of turns (N) = 100 - Rate of change of flux (dΦ/dt) = 0.3 Tesla/sec (Note: The question uses 'tesla/sec', which refers to the rate of change of magnetic flux density per unit area, effectively representing the rate of change of flux per turn, dΦ/dt). 2. **Formula:** The magnitude of the induced emf (ε) is given by: |ε| = N * (dΦ/dt) 3. **Calculation:** |ε| = 100 turns * 0.3 Wb/s (or T·m²/s) |ε| = 30 Volts 4. **Analysis of Options:** - Option (a) 3: Incorrect calculation. - Option (b) 30: Correct magnitude of the induced emf. - Option (c) -30: While Lenz's Law states the emf opposes the change (introducing a negative sign), in standard multiple-choice technical exams, if the magnitude is provided as a positive value and the direction is not specified, the positive magnitude is typically selected. However, if the question specifically asks for the vector/directional value, -30 could be argued. In the context of this specific exam's marking scheme for this question, the magnitude 30 is the intended answer. - Option (d) -300: Incorrect calculation. Therefore, the correct magnitude is 30 V.
MES Jr. Grade • 2024 • Paper-II

Standing wave ratio is defined as the

A) Ratio of voltage maxima to voltage minima
B) Ratio of current maxima to current minima
C) Product of voltage maxima and voltage minima
D) Product of current maxima and current minima
In a transmission line, when a load is not perfectly matched to the characteristic impedance of the line, a portion of the incident wave is reflected back toward the source. The interference between the incident wave and the reflected wave creates a 'standing wave' pattern along the line. The Voltage Standing Wave Ratio (VSWR or SWR) is a measure of this mismatch. It is mathematically defined as the ratio of the maximum voltage amplitude (Vmax) to the minimum voltage amplitude (Vmin) found along the line: VSWR = Vmax / Vmin. Because the current standing wave ratio is identical to the voltage standing wave ratio (Imax / Imin = Vmax / Vmin), option 'a' is the standard definition. Options 'c' and 'd' are incorrect because SWR is a ratio, not a product. While option 'b' is numerically equivalent, the primary and standard definition of SWR in electrical engineering textbooks is based on voltage magnitudes.
MES Jr. Grade • 2024 • Paper-II

A magnetron is commonly used in:

A) Radar transmitters
B) Satellite receivers
C) Mobile phones
D) Optical fibers
A magnetron is a high-power vacuum tube that functions as a cross-field microwave generator. It uses the interaction between a magnetic field and an electric field to generate high-frequency electromagnetic waves (microwaves). Due to its ability to produce very high peak power outputs, it is the primary source of microwave energy used in radar transmitters and microwave ovens. Analysis of other options: - b. Satellite receivers: These typically use Low Noise Amplifiers (LNAs) and mixers, not high-power generators like magnetrons, as they are designed to receive weak signals, not transmit high-power pulses. - c. Mobile phones: These use solid-state power amplifiers (SSPAs) and integrated circuits (RFICs) based on CMOS or GaAs technology for efficiency and miniaturization. - d. Optical fibers: These transmit data using light (photons) via lasers or LEDs, not microwave radiation generated by vacuum tubes.
MES Jr. Grade • 2024 • Paper-II

State and explain ampere’s circuital law.

MES Jr. Grade • 2024 • Paper-II

Implement a full subtractor using demultiplexer.

MES Jr. Grade • 2024 • Paper-II

Define gain margin and phase margin. What is their significance in stability analysis?

MES Jr. Grade • 2024 • Paper-II

Explain the working of a CMOS NAND gate.

MES Jr. Grade • 2024 • Paper-II

An inverting amplifier has R1 = 500 kΩ and Rf = 5 kΩ. Determine the amplifier circuit voltage gain, input resistance and output resistance. Also determine the output voltage and input current if the input voltage is 0.1 V. Assume opamp to be ideal one.

MES Jr. Grade • 2024 • Paper-II

What is transistor biasing? What are the requirements of a good biasing circuit?

MES Jr. Grade • 2024 • Paper-II

In a synchronous counter:

A) All flip-flops are clocked together
B) Flip-flops are clocked in sequence
C) No clock is required
D) It cannot count in reverse
In digital electronics, counters are classified into two main types based on how they are clocked: 1. **Synchronous Counters**: In these counters, the clock input of every flip-flop is connected to a common clock signal. This means all flip-flops trigger simultaneously (at the same time), ensuring that all state transitions occur synchronously. This eliminates the 'ripple' effect and allows for higher operating frequencies. 2. **Asynchronous (Ripple) Counters**: In these counters, the clock is applied only to the first flip-flop. The output of the first flip-flop then serves as the clock for the second, and so on. This creates a sequential delay (ripple) as the signal propagates through the chain. Evaluating the options: - **Option a** is correct because it describes the fundamental definition of a synchronous counter. - **Option b** describes an asynchronous or ripple counter. - **Option c** is incorrect because all counters require a clock signal to trigger state changes. - **Option d** is incorrect because synchronous counters can be designed to count both up and down (Up/Down Counter).
MES Jr. Grade • 2024 • Paper-II

The root locus is symmetric about:

A) jv axis
B) Real axis
C) Both real and imaginary axes
D) None of the above
In control systems, the root locus is a plot of the poles of the closed-loop transfer function as a system parameter (usually the gain K) varies from 0 to infinity. The characteristic equation of the system is given by 1 + KG(s)H(s) = 0. Since the coefficients of the characteristic equation for physical systems are always real numbers, any complex roots must occur in conjugate pairs. If a complex number 's = σ + jω' is a root of the characteristic equation, its conjugate 's* = σ - jω' must also be a root. Geometrically, this means that for every point on the root locus in the upper half of the s-plane, there is a corresponding mirror image point in the lower half of the s-plane. Therefore, the root locus is always symmetric about the real axis. It is not necessarily symmetric about the imaginary (jv) axis unless the system has specific properties (like being purely oscillatory or having a specific structure), which is not a general rule for all root loci.
MES Jr. Grade • 2024 • Paper-II

In free space, the wave impedance is:

A) 50Ω
B) 120πΩ
C) 150Ω
D) 377Ω
The wave impedance (also known as intrinsic impedance) of a medium is the ratio of the electric field intensity (E) to the magnetic field intensity (H). For free space, it is calculated using the formula: η₀ = √(μ₀ / ε₀), where μ₀ is the permeability of free space (4π × 10⁻⁷ H/m) and ε₀ is the permittivity of free space (≈ 8.854 × 10⁻¹² F/m). Substituting these values: η₀ = √( (4π × 10⁻⁷) / (8.854 × 10⁻¹²) ) ≈ 376.73 Ω. This value is commonly approximated as 120π Ω (since 120 * 3.14159 ≈ 376.99 Ω). While option (d) 377Ω is a very close numerical approximation, in technical examinations for Electromagnetics, the exact symbolic form 120πΩ is the standard theoretical answer. Option (a) 50Ω is a common characteristic impedance for coaxial cables, not free space. Option (c) 150Ω is incorrect.
MES Jr. Grade • 2024 • Paper-II

Which class of power amplifier conducts for more than 180° but less than 360°?

A) Class A
B) Class B
C) Class AB
D) Class C
Power amplifiers are classified based on their conduction angle (the portion of the input cycle during which the output transistor conducts current). 1. **Class A**: The transistor conducts for the full 360° of the input cycle. It provides the highest linearity but lowest efficiency. 2. **Class B**: The transistor conducts for exactly 180° (half the cycle). This is typically used in push-pull configurations to eliminate crossover distortion, though a single Class B amplifier only handles half the waveform. 3. **Class AB**: This is a hybrid between Class A and Class B. The transistor is biased such that it conducts for more than 180° but less than 360°. This is specifically designed to eliminate 'crossover distortion' found in Class B amplifiers while maintaining better efficiency than Class A. 4. **Class C**: The transistor conducts for less than 180°. These are highly efficient but produce significant distortion, making them suitable primarily for RF tuned amplifiers. Since the question asks for the class that conducts for more than 180° but less than 360°, the correct answer is Class AB.
MES Jr. Grade • 2024 • Paper-II

Which code changes only one bit between successive numbers?

A) BCD
B) Gray code
C) Excess-3
D) ASCII
The question asks for a code where only one bit changes between successive numbers. This is the defining characteristic of a 'unit-distance code'. 1. **Gray Code (Correct):** Also known as reflected binary code, it is specifically designed so that two successive values differ by only one bit. This property is crucial in digital systems to prevent 'glitches' or spurious outputs during transitions in hardware like rotary encoders or asynchronous FIFO pointers. 2. **BCD (Binary Coded Decimal):** This is a weighted code where each decimal digit is represented by 4 bits. For example, moving from 1 (0001) to 2 (0010) involves two bit changes (the last bit changes from 1 to 0, and the second-to-last changes from 0 to 1). 3. **Excess-3:** This is a non-weighted code derived by adding 3 to the BCD value. Like BCD, it does not maintain a unit-distance property. For example, 0 (0011) to 1 (0100) involves three bit changes. 4. **ASCII (American Standard Code for Information Interchange):** This is a character encoding standard for text, not a numerical sequence designed for unit-distance transitions.
MES Jr. Grade • 2024 • Paper-II

The dominant mode in a circular waveguide is:

A) TE 11
B) TM 01
C) TE 01
D) TM 11
In waveguide theory, the 'dominant mode' is defined as the mode with the lowest cutoff frequency. For a circular waveguide of radius 'a', the cutoff frequency for any mode is given by the formula: fc = (chi_mn / 2πa) * c, where chi_mn is the root of the Bessel function (for TM modes) or the root of the derivative of the Bessel function (for TE modes). 1. For TE modes, the smallest root is chi'_11 ≈ 1.841 (for TE11). 2. For TM modes, the smallest root is chi_01 ≈ 2.405 (for TM01). 3. The TE01 mode has a root chi'_01 ≈ 3.832. Comparing these values, the TE11 mode has the smallest root (1.841), which results in the lowest cutoff frequency. Therefore, TE11 is the dominant mode in a circular waveguide. - Option b (TM 01) is the dominant TM mode, but its cutoff frequency is higher than TE 11. - Option c (TE 01) has a significantly higher cutoff frequency than TE 11. - Option d (TM 11) has a higher cutoff frequency than both TE 11 and TM 01.
MES Jr. Grade • 2024 • Paper-II

Find the standing wave ratio, when a load impedance of 250Ω is connected to a 75Ω line.

A) 0.3
B) 75
C) 250
D) 3.33
To find the Standing Wave Ratio (SWR), we follow these steps: 1. **Identify Given Values**: - Characteristic Impedance of the line ($Z_0$) = $75\Omega$ - Load Impedance ($Z_L$) = $250\Omega$ 2. **Calculate the Reflection Coefficient ($\Gamma$)**: The reflection coefficient is given by the formula: $$\Gamma = \frac{Z_L - Z_0}{Z_L + Z_0}$$ $$\Gamma = \frac{250 - 75}{250 + 75} = \frac{175}{325} \approx 0.5385$$ 3. **Calculate the Standing Wave Ratio (SWR)**: The SWR is related to the reflection coefficient by the formula: $$SWR = \frac{1 + |\Gamma|}{1 - |\Gamma|}$$ Alternatively, for purely resistive loads, SWR can be calculated directly as the ratio of the larger impedance to the smaller impedance: $$SWR = \frac{Z_L}{Z_0} \text{ (if } Z_L > Z_0\text{)}$$ $$SWR = \frac{250}{75} = 3.333...$$ 4. **Conclusion**: The calculated SWR is approximately 3.33. - Option (a) 0.3 is incorrect as SWR must always be $\ge 1$. - Option (b) 75 and (c) 250 are simply the given impedance values and do not represent the ratio. - Option (d) 3.33 matches our calculation.
MES Jr. Grade • 2024 • Paper-II

The root locus of a system starts at:

A) Zeros and ends at poles
B) Poles and ends at zeros
C) Origin and ends at infinity
D) None of the above
In control systems, the Root Locus is a graphical representation of the paths (loci) of the closed-loop poles as a system parameter (usually the gain 'K') is varied from 0 to infinity. 1. **Starting Point (K = 0):** The characteristic equation of a closed-loop system is given by 1 + KG(s)H(s) = 0. When K = 0, the equation reduces to the open-loop characteristic equation. Therefore, the root locus starts at the open-loop poles. 2. **Ending Point (K → ∞):** As K approaches infinity, the closed-loop poles move toward the open-loop zeros of the system. If there are more poles than zeros, the remaining branches move toward infinity along specific asymptotes. Comparing this to the options: - Option (a) is the reverse of the actual behavior. - Option (b) correctly states that the locus starts at poles and ends at zeros. - Option (c) is incorrect as the origin is not the universal starting point.
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