Previous Year Questions
Solve previous year questions to understand exam patterns
At resonance, the inductive reactance equals the capacitive reactance, and the circuit behaves like a pure resistor.
However, voltages across L and C can be significantly higher due to energy oscillation between them.
This magnification is quantified by the Q-factor.
Mathematically, voltage magnification = Q-factor = \( \frac{\text{Voltage across } L \text{ or } C}{\text{Applied voltage}} \).
At resonance, the series RLC circuit's impedance is minimum, allowing maximum current.
The voltage across L and C can be much greater than the source voltage due to energy exchange.
This effect is called voltage magnification.
The Q-factor measures how many times the voltage across L or C is greater than the applied voltage.
Thus, voltage magnification and Q-factor are directly related and represent the same concept.
1. Choose a Zener diode with breakdown voltage V_Z = 12 V.
2. Determine the series resistor R_s to limit the current.
Given:
- Input voltage varies from 12 V to 14 V.
- Output voltage V_o = 12 V.
Assuming load current I_L and Zener current I_Z(min) to maintain regulation are known or estimated.
Calculate R_s using:
R_s = (V_in(max) - V_Z) / (I_L + I_Z(min))
Working:
- When input voltage increases, the extra voltage is dropped across R_s.
- The Zener diode maintains 12 V across the load by shunting excess current.
- When input voltage decreases, the Zener diode current decreases but voltage remains constant.
This ensures a stable 12 V output despite input voltage variations.
Select a Zener diode with breakdown voltage equal to desired output voltage (12 V).
Calculate the series resistor to limit current and protect the diode.
The resistor drops the excess voltage when input voltage is higher than 12 V.
The Zener diode maintains constant voltage across the load by operating in breakdown region.
This design ensures output voltage remains at 12 V even if input varies between 12 V and 14 V.
Speed of light \(c = 3 \times 10^{8} \ \text{m/s}\)
Wavelength \(\lambda = \frac{c}{f} = \frac{3 \times 10^{8}}{4.5 \times 10^{14}} = 6.67 \times 10^{-7} \ \text{m}\)
Therefore, the wavelength of the light is \(6.67 \times 10^{-7}\) meters or 667 nm.
To find the wavelength from the frequency, use the relation \(\lambda = \frac{c}{f}\).
Substitute the given frequency and speed of light values.
Perform the division carefully to get the wavelength in meters.
This problem reinforces the direct relationship between frequency and wavelength of electromagnetic waves.
Although robot malfunctions can cause physical injuries, the primary health hazard when humans only monitor robots is the increase in health problems due to inactivity and lack of physical work.
Monitoring robots often leads to sedentary behavior, which can cause various health issues.
Therefore, the main concern is not physical injury but health hazards related to inactivity.
Teachers should emphasize the difference between direct physical risks and indirect health consequences of robotic workplaces.
In the colour coding system for carbon resistors, the first two bands represent the significant digits of the resistance value. The multiplier band determines how many zeros to add or the factor by which to multiply these digits. For example, a multiplier band of Red means multiply by \(10^2\), Orange means multiply by \(10^3\), and so on. This allows a compact representation of a wide range of resistance values using just a few colour bands.
Using the refraction formula:
\[ \frac{n_2}{v} - \frac{n_1}{u} = \frac{n_2 - n_1}{R} \]
Substitute values:
\[ \frac{1.5}{v} - \frac{1.0}{-25} = \frac{1.5 - 1.0}{20} \]
\[ \frac{1.5}{v} + 0.04 = 0.025 \]
\[ \frac{1.5}{v} = 0.025 - 0.04 = -0.015 \]
\[ v = \frac{1.5}{-0.015} = -100 \text{ cm} \]
The image is formed at 100 cm on the same side as the object (virtual image).
This problem is similar to the previous one but with different parameters.
Applying the refraction formula at a spherical surface allows calculation of image distance.
Sign conventions are important: object distance is negative because the object is in front of the surface; radius of curvature is positive for convex surfaces.
The negative image distance indicates a virtual image formed on the same side as the object.
This exercise reinforces understanding of refraction at curved surfaces and the use of sign conventions.
Since these two fields are perpendicular to each other, the resultant field lies along the diagonal of the rectangle formed by \( B_H \) and \( B \).
The needle aligns along this resultant field to minimize potential energy.
This resultant field bisects the angle between the two perpendicular fields, so the needle points along the bisector of the angle between Earth's horizontal magnetic field and the coil's magnetic field.
This explains the observed deflection in the tangent galvanometer experiment.
The magnetic needle experiences torque due to the combined effect of Earth's horizontal magnetic field and the magnetic field from the coil.
Because these two fields are perpendicular, their vector sum forms the resultant field.
The needle aligns along this resultant field to achieve equilibrium.
Since the resultant is the diagonal of the rectangle formed by the two perpendicular fields, it lies along the bisector of the angle between them.
This physical reasoning helps students visualize magnetic field vectors and understand the behavior of magnetic needles in combined fields.
Cathode rays experience forces due to both electric and magnetic fields.
The electric force causes deflection in one direction, while the magnetic force causes deflection in the opposite direction.
Increasing the magnetic field increases the magnetic force, which opposes the electric force.
As a result, the net deflection decreases.
This explains why increasing magnetic field strength reduces the deflection of cathode rays.
This means the current either leads or lags the voltage by 90°.
Because of this phase difference, the average power consumed over a cycle is zero.
The current component that is 90° out of phase with voltage does not contribute to real power consumption and is called wattless current.
It represents energy that is alternately stored and released by the inductor or capacitor without being dissipated.
In inductors and capacitors, energy is stored temporarily in magnetic and electric fields respectively.
The current associated with this energy storage leads or lags the voltage by 90 degrees.
Because power is the product of voltage and current, and these are out of phase, the net power over a cycle is zero.
This current is called wattless because it does not perform any real work but affects the circuit's reactive properties.
Understanding wattless current is important for power factor correction and efficient circuit design.
Fringe width \( \beta = \frac{\lambda D}{d} = \frac{600 \times 10^{-9} \times 1}{0.2 \times 10^{-3}} = 3 \times 10^{-3} \text{ m} = 3 \text{ mm} \).
Fringe width is 3 mm.
Fringe width in interference is the distance between two consecutive bright or dark fringes.
It depends on the wavelength of light, distance between the sources, and distance to the screen.
The formula \( \beta = \frac{\lambda D}{d} \) is used to calculate fringe width.
Substituting the given values yields the fringe width.
This problem illustrates the practical application of interference in optics.
For example, differential equations and linear algebra are used to model quantum mechanical effects in nanoparticles, helping researchers design materials with desired optical or electronic properties.
Applied mathematics is fundamental in nanotechnology because it allows scientists to create models that describe how nanoscale systems behave.
These models help in simulating physical phenomena like electron transport, heat transfer, and mechanical properties at the nanoscale.
By solving these mathematical models, researchers can predict how nanomaterials will perform before physically creating them, saving time and resources.
For example, using mathematical modeling, one can simulate how quantum dots absorb and emit light, which is essential for designing new optical devices.
1. Two protons fuse to form a deuterium nucleus, a positron, and a neutrino.
2. The deuterium nucleus fuses with another proton to form helium-3 and emits a gamma ray.
3. Two helium-3 nuclei fuse to form helium-4 and release two protons.
These reactions convert hydrogen into helium, releasing energy in the form of gamma rays, positrons, and neutrinos.
The energy released balances gravitational collapse and sustains the star's radiation output.
The proton-proton cycle is the primary fusion process in stars like the Sun.
Each step releases energy by converting mass into energy.
The cycle ensures continuous energy production as hydrogen nuclei fuse.
Understanding this cycle helps students appreciate how stars generate energy over billions of years.
The Biot-Savart law helps us calculate the magnetic field created by a small segment of current-carrying wire.
It shows how the magnetic field depends on the current, the size and orientation of the wire segment, and the distance to the observation point.
The vector nature of the formula means the magnetic field direction is perpendicular to both the current element and the line to the point.
This law is fundamental for understanding magnetic fields from any shaped conductor by integrating over the entire wire.
Teachers emphasize the cross product and the inverse square dependence to help students visualize the magnetic field generation.
For Uranium-238, the alpha decay is:
\[ _{92}^{238}U \rightarrow _{90}^{234}Th + _{2}^{4}He \]
Alpha decay involves emission of an alpha particle which is a helium nucleus containing 2 protons and 2 neutrons.
Thus, the parent nucleus loses 2 protons and 2 neutrons.
This reduces the atomic number by 2 and mass number by 4.
The nuclear equation represents this transformation clearly.
The electric furnace is designed to generate very high temperatures for industrial processes, so it produces the highest heat. Electric heaters are used for domestic heating and produce significant heat but less than furnaces. Electric lamp filaments produce heat as a byproduct of light generation but less than heaters. Fuse wires produce heat only to the extent necessary to melt and break the circuit, so they generate the least heat among these devices.
Density of oil drop, \( \rho = 900 \) kg/m\(^3\)
Radius, \( r = 1 \times 10^{-6} \) m
Terminal velocity, \( v = 3 \times 10^{-5} \) m/s
Density of air, \( \sigma = 1.2 \) kg/m\(^3\)
Viscosity of air, \( \eta = 1.8 \times 10^{-5} \) Ns/m\(^2\)
Step 1: Calculate the radius using formula
\[ r = \sqrt{ \frac{9 \eta v}{2 (\rho - \sigma) g} } \]
Substitute values:
\( g = 9.8 \) m/s\(^2\)
\[ r = \sqrt{ \frac{9 \times 1.8 \times 10^{-5} \times 3 \times 10^{-5}}{2 \times (900 - 1.2) \times 9.8} } \]
\[ r = \sqrt{ \frac{4.86 \times 10^{-9}}{17642.5} } = \sqrt{2.756 \times 10^{-13}} = 1.66 \times 10^{-6} \text{ m} \]
Step 2: Calculate viscous force using Stokes' law
\[ F_v = 6 \pi r \eta v \]
\[ F_v = 6 \times 3.1416 \times 1.66 \times 10^{-6} \times 1.8 \times 10^{-5} \times 3 \times 10^{-5} \]
\[ F_v = 1.68 \times 10^{-14} \text{ N} \]
Therefore, the radius of the drop is approximately \(1.66 \times 10^{-6}\) m and the viscous force acting on it is \(1.68 \times 10^{-14}\) N.
First, we use the relation derived from force balance at terminal velocity to find the radius of the oil drop.
This formula relates viscosity, terminal velocity, density difference, and gravity to the radius.
Substituting the given values carefully gives the radius.
Next, using Stokes' law, the viscous force is calculated as proportional to radius, viscosity, and velocity.
This stepwise calculation helps understand how physical quantities relate in the experiment.
Zener voltage, \(V_Z = 5.6 \, V\)
Depletion layer width, \(d = 100 \, nm = 100 \times 10^{-9} \, m = 1 \times 10^{-7} \, m\)
Electric field strength, \(E = \frac{V_Z}{d} = \frac{5.6}{1 \times 10^{-7}} = 5.6 \times 10^{7} \, V/m\)
Therefore, the electric field strength across the depletion layer is \(5.6 \times 10^{7} \, V/m\).
The electric field strength is the voltage divided by the distance over which the voltage is applied.
Here, the voltage is the Zener voltage and the distance is the depletion layer width.
Convert the width from nanometers to meters for consistent units.
Divide the voltage by the width to get the electric field strength in volts per meter.
This calculation shows the very strong electric field present in the depletion region during Zener breakdown.
To solve a circuit using Kirchhoff’s rules, the first step is to assign directions to the currents in each branch.
Next, apply Kirchhoff’s current rule (junction rule) at the junctions to write current equations.
Then, apply Kirchhoff’s voltage rule (loop rule) to write voltage equations for independent loops.
Finally, solve the simultaneous equations obtained from the junction and loop equations to find the unknown currents.
This sequence ensures systematic and correct analysis of the circuit.
Initial force: \( F = k \frac{q_1 q_2}{r^2} \)
New charges: \( q_1' = \frac{q_1}{2} \), \( q_2' = \frac{q_2}{2} \)
New distance: \( r' = 2r \)
New force:
\[ F' = k \frac{q_1' q_2'}{r'^2} = k \frac{(q_1/2)(q_2/2)}{(2r)^2} = k \frac{q_1 q_2}{4} \times \frac{1}{4 r^2} = \frac{k q_1 q_2}{16 r^2} = \frac{F}{16} \]
Therefore, the new force is \( \frac{F}{16} \).
The electrostatic force depends on the product of the charges and inversely on the square of the distance. When both charges are halved, their product becomes one-fourth. When the distance is doubled, the denominator becomes four times larger (since distance squared). Multiplying these effects, the force reduces by a factor of 16. This problem helps students apply the formula and understand how changes in charge and distance affect the force.
The Wheatstone bridge is balanced when \( \frac{P}{Q} = \frac{R}{S} \), and no current flows through the galvanometer. Here, since the ratios are not equal, the bridge is unbalanced, and current flows through the galvanometer. To find this current, Kirchhoff’s current and voltage laws are applied to the circuit. By writing equations for currents at junctions and voltages around loops, a system of equations is formed. Solving these equations gives the galvanometer current. The calculation involves algebraic manipulation and understanding of circuit laws. Approximations such as neglecting galvanometer resistance simplify the problem. This example illustrates how Kirchhoff’s laws help analyze complex circuits with multiple branches.

