CUET UG Physics Booster Test - 3 Electron Dynamics and Drift
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QUESTION 1 OF 20
Which of the following statements is correct regarding the collision dynamics between conduction electrons and fixed ions?
Statements:
1. The post-collision velocity direction is completely random and independent of the incoming direction.
2. The kinetic energy of the electron changes drastically during each thermal collision with an ion.
3. The collisions only randomize the velocity vectors without drastically altering the average speed.
4. An electron emerging from a collision retains its pre-collision speed exactly.
QUESTION 2 OF 20
The macroscopic consequence of completely random post-collision velocity directions is
QUESTION 3 OF 20
If the individual thermal velocities v_i are completely random in three dimensions, evaluating the sum
1/N∑v_i
for an extremely large number of electrons N will be
QUESTION 4 OF 20
Incorrect statement regarding electron velocities in the strict absence of an electric field
QUESTION 5 OF 20
Match List I with List II
| List I | List II |
|---|---|
| 1. Negative sign in a=-eE/m | a. Electrostatic force magnitude |
| 2. Mass m | b. Rate of change of velocity |
| 3. Quantity eE | c. Indicates acceleration is antiparallel to electric field |
| 4. Variable a | d. Determines inertial resistance |
QUESTION 6 OF 20
In the conceptual setup with charged discs at the ends of a cylinder, if fresh charges are continuously supplied to the ends
QUESTION 7 OF 20
Correct statements regarding the elapsed time t_i parameter
Statements:
1. It governs the magnitude of the velocity an electron has gained from the electric field since its last collision.
2. It represents the time elapsed since the precise last collision for the i^(th)individual electron.
3. It varies randomly across the electron population at a given instant t.
4. It is perfectly identical to the relaxation time τfor all electrons simultaneously.
QUESTION 8 OF 20
By mathematically relating the resistivity ρto the macroscopic collision parameters, substituting σ=1/ρinto the conductivity formula gives the relaxation time τwhich will be
QUESTION 9 OF 20
Nature of the individual components v_i and the field-induced term
-eEt_i/m
inside the instantaneous velocity equation
V_i=v_i-eEt_i/m
is:
QUESTION 10 OF 20
If a conductive material has an internal relaxation time of 3.0×10^(-14)s and an applied steady field of 0.5 V/m, the magnitude of the drift velocity (using e/m≈1.76×10^(11)C/kg) will be
QUESTION 11 OF 20
Which of the following statements is correct regarding the steady drift speed of electrons in a conductor?
Statements:
1. Electrons continuously accelerate between collisions, but their macroscopic average remains steady.
2. The average macroscopic drift velocity vector remains independent of time.
3. The steady drift physically implies that the instantaneous acceleration of individual free electrons is zero.
4. The steady average speed is attained strictly because the kinetic energy is converted into mass.
QUESTION 12 OF 20
Incorrect statement linking drift direction to the applied electric parameters
QUESTION 13 OF 20
The core physical significance of the immense number density parameter (n, 10^(29) m^(-3))is that
QUESTION 14 OF 20
In analytically defining the net current across a planar area A via the drift velocity, the expression
-neA∣v_d∣Δt
QUESTION 15 OF 20
Match List I with List II regarding Current Density and Electric Current
| List I | List II |
|---|---|
| 1. SI Unit of current density j | a. (ne |
| 2. j×A | b. Parallel to vector E |
| 3. Magnitude ( — j 4. jvector direction | d. A/m² |
QUESTION 16 OF 20
By equating the derived microscopic equation
j=(ne^2τ/m)E
with the macroscopic Ohm's law form
j=σE
the conductivity σof a material is
QUESTION 17 OF 20
Correct statements about carrier mobility μ
Statements:
1. It is an important parameter in defining conductivity derived from mobile charge carriers.
2. It is defined as the magnitude of drift velocity per unit electric field.
3. It can be mathematically expressed as eτ/m for free electrons.
4. It is formally treated as a negative quantity for negatively charged electrons.
QUESTION 18 OF 20
If mobility is given as
4.5×10^3 cm^2/(V s)
its value in SI units is
QUESTION 19 OF 20
Incorrect statement regarding the estimation of electron density parameter in copper
QUESTION 20 OF 20
Thermal speed vs Drift speed vs Field propagation speed in a typical conductor
Test Complete!
Answer Review
1 Which of the following statements is correct regarding the collision dynamics between conduction electrons and fixed ions?
Statements:
1. The post-collision velocity direction is completely random and independent of the incoming direction.
2. The kinetic energy of the electron changes drastically during each thermal collision with an ion.
3. The collisions only randomize the velocity vectors without drastically altering the average speed.
4. An electron emerging from a collision retains its pre-collision speed exactly.
�� Electron directions become randomized after collisions. �� Average thermal speed remains approximately unchanged. �� Collisions do not drastically alter electron kinetic energy.
In a metallic conductor, free electrons continuously collide with the fixed positive ions of the lattice. These collisions randomize the direction of electron motion, making the post-collision direction independent of the incoming direction. However, the collisions are primarily elastic in nature, so the speed and kinetic energy of the electrons do not change drastically. As a result, while the velocity vectors are continuously randomized, the average thermal speed remains nearly constant. Therefore, statements 1, 3, and 4 are correct. Statement 2 is incorrect because thermal collisions do not generally produce large changes in the kinetic energy of electrons.
- �� Option A → Statement 2 is incorrect.
- �� Option C → Statement 2 is incorrect.
- �� Option D → Statement 2 is incorrect.
Used – Concept Application
- Application
- Apply the microscopic collision model of free electrons in metals.
- Final Logic
- Collisions randomize direction but do not drastically change electron speed.
- Random Direction → No Preferred Motion
2 The macroscopic consequence of completely random post-collision velocity directions is
�� Random directions cancel each other. �� No preferred direction exists. �� Average velocity becomes zero.
In the absence of an external electric field, free electrons move randomly because of thermal energy. Since the post-collision directions are completely random, equal numbers of electrons move in opposite directions. Consequently, the vector sum of all electron velocities becomes zero: 1/N∑v_i=0 This implies that the average velocity of electrons is zero. Although individual electrons move at high thermal speeds, there is no net motion in any particular direction. Therefore, no macroscopic current exists in an isolated conductor. Hence, Option C is correct.
- �� Option A → Random motion does not create a net current.
- �� Option B → Electrons can accelerate when an electric field is applied.
- �� Option D → Random collisions do not synchronize electron motion.
Used – Concept Application
- Application
- Use the concept of thermal equilibrium and random motion.
- Final Logic
- Random velocities cancel statistically, giving zero average velocity.
- Zero Average → No Current
3 If the individual thermal velocities v_i are completely random in three dimensions, evaluating the sum
1/N∑v_i
for an extremely large number of electrons N will be
�� Thermal velocities are random. �� Opposite velocity components cancel. �� Average velocity becomes zero.
In thermal equilibrium, free electrons move randomly in all directions. For every electron moving in one direction, there is statistically another moving in the opposite direction. Therefore, when the vector velocities of a very large number of electrons are averaged, 1/N∑v_i=0 This does not mean electrons are stationary. Rather, their motions are equally distributed in all directions, producing complete cancellation of the vector average. Hence the correct answer is Option A.
- �� Option B → Drift velocity exists only when an electric field is applied.
- �� Option C → Average speed is not the same as average velocity.
- �� Option D → Represents thermal speed, not average velocity.
Used – Statistical Reasoning
- Application
- Use symmetry of random motion in thermal equilibrium.
- Final Logic
- Equal probability in opposite directions leads to zero average velocity.
- Average Velocity = Zero
4 Incorrect statement regarding electron velocities in the strict absence of an electric field
�� Free electrons are always moving. �� Motion is random in the absence of a field. �� Only the average velocity is zero.
Even when no electric field is present, free electrons possess thermal energy and continuously move through the conductor. Between collisions, they travel approximately in straight lines and undergo frequent collisions with lattice ions. Although individual electrons are always moving, their directions are random. Therefore, the average velocity is zero, and equal numbers cross any section in opposite directions. Statement B is incorrect because electrons are not stationary; they are in continuous thermal motion.
- �� Option A → Correct consequence of random motion.
- �� Option C → Correct description of motion between collisions.
- �� Option D → Correct statistical result.
Used – Concept Application
- Application
- Apply the free-electron model of metallic conduction.
- Final Logic
- Electrons are always moving thermally, even when no current flows.
- No Field = Random Motion
5 Match List I with List II
| List I | List II |
|---|---|
| 1. Negative sign in a=-eE/m | a. Electrostatic force magnitude |
| 2. Mass m | b. Rate of change of velocity |
| 3. Quantity eE | c. Indicates acceleration is antiparallel to electric field |
| 4. Variable a | d. Determines inertial resistance |
�� Electric force acts opposite to the field on electrons. �� Mass opposes acceleration. �� Acceleration is the rate of velocity change.
For an electron in an electric field, a=-eE/m The negative sign indicates that acceleration is opposite to the electric field because electrons carry negative charge. The quantity eE represents the magnitude of the electrostatic force acting on the electron. The mass m determines the inertia of the electron and its resistance to acceleration. The variable a denotes acceleration, which is defined as the rate of change of velocity. Therefore, the correct matching is: 1-c, 2-d, 3-a, 4-b
- �� Option A → Physical meanings of acceleration and force are incorrect.
- �� Option B → Multiple quantities are incorrectly matched.
- �� Option C → Force and inertia terms are interchanged.
Used – Formula Recall
- Application
- Interpret each symbol and term appearing in
- a=-eE/m
- Final Logic
- Match every symbol with its physical significance in the acceleration equation.
- a → Velocity Change
6 In the conceptual setup with charged discs at the ends of a cylinder, if fresh charges are continuously supplied to the ends
�� Continuous charge replenishment maintains the electric field. �� The maintained field produces continuous drift. �� Continuous drift results in steady current.
When opposite charges are placed at the ends of a conductor, an electric field is established inside it. Initially, electrons drift and gradually neutralize the charge imbalance. If no further charges are supplied, the electric field disappears and the current stops. However, if an external source such as a battery continuously replenishes charges at the ends, the electric field remains constant throughout the conductor. Electrons continue to experience an electric force and acquire a steady drift velocity. Although individual electrons undergo random thermal motion and collisions, the average drift remains constant, producing a steady electric current. Therefore, a continuous supply of charges is the mechanism by which batteries maintain current in electrical circuits.
- �� Option A → Continuous replenishment prevents current from stopping.
- �� Option C → Positive ions remain fixed in the metallic lattice.
- �� Option D → Thermal motion remains random even during current flow.
Used – Concept Application
- Application
- Apply the role of a battery in maintaining an electric field.
- Final Logic
- Continuous charge replenishment maintains the field and therefore maintains steady current.
- Drift → Steady Current
7 Correct statements regarding the elapsed time t_i parameter
Statements:
1. It governs the magnitude of the velocity an electron has gained from the electric field since its last collision.
2. It represents the time elapsed since the precise last collision for the i^(th)individual electron.
3. It varies randomly across the electron population at a given instant t.
4. It is perfectly identical to the relaxation time τfor all electrons simultaneously.
�� t_i measures time since the last collision. �� Different electrons have different values of t_i. �� Larger t_i means greater field-induced velocity gain.
In the microscopic theory of conduction, t_i denotes the time elapsed since the last collision of the i^(th)electron. Because collisions occur randomly, different electrons have different elapsed times at any instant. The field-induced velocity gained by an electron is -eE/mt_i showing that the velocity acquired from the electric field depends directly on t_i. Since collisions occur at random intervals, the values of t_i vary throughout the electron population. The relaxation time τis only the average value of all such times and is not identical to every individual t_i.
- �� Option A → Statement 4 is incorrect.
- �� Option C → Statement 4 is incorrect.
- �� Option D → Statement 4 is incorrect.
Used – Concept Application
- Application
- Differentiate between individual collision times and average relaxation time.
- Final Logic
- t_i varies from electron to electron, whereas τis only the average.
- τ→ Average Time
8 By mathematically relating the resistivity ρto the macroscopic collision parameters, substituting σ=1/ρinto the conductivity formula gives the relaxation time τwhich will be
�� Conductivity and resistivity are reciprocals. �� Conductivity depends on relaxation time. �� Rearranging gives the expression for τ.
The conductivity of a conductor is σ=ne^2τ/m and resistivity is related by ρ=1/σ Substituting, 1/ρ=ne^2τ/m Rearranging, τ=m/ne^2ρ Thus the relaxation time depends directly on electron mass and inversely on electron density, electronic charge squared, and resistivity.
- �� Option B → Incorrect algebraic rearrangement.
- �� Option C → Places ρin the numerator incorrectly.
- �� Option D → Dimensionally incorrect.
Used – Formula Recall
- Application
- Use conductivity and resistivity relations.
- Final Logic
- σ=ne^2τ/mandσ=1/ρ
- lead directly to
- τ=m/ne^2ρ
- Resistivity Up → Relaxation Time Down
9 Nature of the individual components v_i and the field-induced term
-eEt_i/m
inside the instantaneous velocity equation
V_i=v_i-eEt_i/m
is:
�� v_i is the random thermal velocity after the last collision. �� -eEt_i/m is produced by the electric field. �� The field-induced term has a definite direction.
The instantaneous velocity of the i^(th)electron is given by V_i=v_i-eEt_i/m Here, v_i represents the random thermal velocity of the electron immediately after its last collision with a positive ion. Because collisions occur randomly, both the magnitude and direction of v_i are random. The term -eEt_i/m represents the velocity gained due to acceleration by the applied electric field during the time interval t_i. Since the electric field has a fixed direction, this contribution is directional. The negative sign indicates that the electron velocity gained due to the field is opposite to the direction of the electric field. Therefore, v_i is random while -eEt_i/m is directional.
- �� Option A → The thermal velocity component is random.
- �� Option B → Reverses the nature of the two terms.
- �� Option C → The field-induced term is not random.
Used – Concept Application
- Application
- Identify the physical meaning of each term in the instantaneous velocity equation.
- Final Logic
- Thermal motion is random, whereas the electric field produces a directed velocity component.
- eEt_i/m→ Electric Field → Directional
10 If a conductive material has an internal relaxation time of 3.0×10^(-14)s and an applied steady field of 0.5 V/m, the magnitude of the drift velocity (using e/m≈1.76×10^(11)C/kg) will be
�� Drift velocity depends on E and τ. �� Use v_d=eEτ/m. �� Substitute the given values.
The magnitude of drift velocity is v_d=eEτ/m Substituting the given values, v_d=(1.76×10^(11))(0.5)(3.0×10^(-14))v_d=2.64×10^(-3) m/s Thus the electrons drift with a very small average speed even though their thermal speeds are much larger.
- �� Option B → Arithmetic error.
- �� Option C → Incorrect power of ten.
- �� Option D → Incorrect multiplication.
Used – Substitution
- Application
- Substitute the given values into the drift velocity formula.
- Final Logic
- v_d=eEτ/m=(1.76×10^(11))(0.5)(3×10^(-14))=2.64×10^(-3) m/s
- Stronger Field → Larger Drift
11 Which of the following statements is correct regarding the steady drift speed of electrons in a conductor?
Statements:
1. Electrons continuously accelerate between collisions, but their macroscopic average remains steady.
2. The average macroscopic drift velocity vector remains independent of time.
3. The steady drift physically implies that the instantaneous acceleration of individual free electrons is zero.
4. The steady average speed is attained strictly because the kinetic energy is converted into mass.
�� Individual electrons accelerate between collisions. �� Frequent collisions maintain a constant average drift speed. �� Steady drift does not imply zero acceleration.
When an electric field is applied, electrons experience a force and accelerate between successive collisions. However, collisions repeatedly randomize their motion, preventing indefinite acceleration. As a result, the average drift velocity reaches a constant value known as the steady drift velocity. The macroscopic drift velocity remains constant with time for a steady current even though individual electrons continuously accelerate between collisions. Therefore, statements 1 and 2 are correct. Statement 3 is incorrect because electrons do accelerate between collisions. Statement 4 is incorrect because steady drift has nothing to do with conversion of kinetic energy into mass.
- �� Option A → Statement 4 is incorrect.
- �� Option C → Statements 3 and 4 are incorrect.
- �� Option D → Statement 3 is incorrect.
Used – Concept Application
- Application
- Distinguish between microscopic electron motion and macroscopic current behavior.
- Final Logic
- Individual electrons accelerate, but the average drift velocity remains constant.
- Average Drift → Constant
12 Incorrect statement linking drift direction to the applied electric parameters
�� Electrons are negatively charged. �� Drift velocity is opposite to the electric field. �� Current density is parallel to the electric field.
The drift velocity of electrons is given by v_d=-eτ/mE The negative sign indicates that electrons drift opposite to the electric field direction. Therefore, statement C is incorrect. Since conventional current is defined in the direction of positive charge flow, the current density vector is parallel to the electric field. Electrons move from lower potential to higher potential because they carry negative charge. Thus statements A, B, and D are correct while statement C is incorrect.
- �� Option A → Correct relation for current density.
- �� Option B → Correct direction of electron drift.
- �� Option D → Correct interpretation of the negative sign.
Used – Formula Recall
- Application
- Use the drift velocity equation and sign convention.
- Final Logic
- Negative charge causes electron drift opposite to the electric field.
- Current Follows Field
13 The core physical significance of the immense number density parameter (n, 10^(29) m^(-3))is that
�� Electron density is extremely large. �� Drift speed is very small. �� Large numbers of carriers produce large current.
For a conductor, I=neA∣v_d∣ where n is the number density of free electrons. In metals, n is typically of the order of 10^(28)–10^(29) m^(-3). Although the drift velocity v_d is very small (often around 10^(-4)to 10^(-3) m/s), the enormous number of free electrons ensures that a large amount of charge crosses any cross-section every second. This results in measurable macroscopic currents. Therefore, the significance of large n is that it compensates for the tiny drift speed.
- �� Option A → Thermal speed is not determined by number density.
- �� Option B → Electrons can still accelerate under electric fields.
- �� Option D → Ohm's law is not restricted to insulators.
Used – Concept Application
- Application
- Analyze the microscopic current equation.
- Final Logic
- Large carrier density × Small drift speed = Significant current.
- Tiny Drift × Huge Number = Big Current
14 In analytically defining the net current across a planar area A via the drift velocity, the expression
-neA∣v_d∣Δt
�� Expression represents transported electron charge. �� Negative sign arises from electron charge. �� Current direction is opposite to electron motion.
During a small interval Δt, electrons drift a distance ∣v_d∣Δt. The number of electrons crossing area A is nA∣v_d∣Δt Since each electron carries charge -e, ΔQ=-neA∣v_d∣Δt This expression represents the charge transported by electrons. Because electrons move opposite to the electric field, the corresponding conventional current is along the electric field direction. Hence Option B is correct.
- �� Option A → Drift current is not cancelled by thermal motion.
- �� Option C → Expression refers to electron charge, not positive charges.
- �� Option D → No such restriction exists.
Used – Concept Application
- Application
- Apply the microscopic definition of current.
- Final Logic
- Charge transported equals number of carriers × charge per carrier.
- Electron Charge → Negative Sign
15 Match List I with List II regarding Current Density and Electric Current
| List I | List II |
|---|---|
| 1. SI Unit of current density j | a. (ne |
| 2. j×A | b. Parallel to vector E |
| 3. Magnitude ( — j 4. jvector direction | d. A/m² |
�� Current density is current per unit area. �� Its magnitude depends on carrier density and drift velocity. �� Current density is directed along the electric field.
Current density is defined as j=I/A where I is the electric current and A is the cross-sectional area. The magnitude of current density is ∣j∣=ne∣v_d∣ where n is the number density of free charge carriers, e is the electronic charge, and v_d is the drift velocity. The SI unit of current density is A/m^2 For a conductor obeying Ohm's law, the current density vector is parallel to the electric field vector E. Also, I=jA Therefore, the correct matching is: 1-d, 2-c, 3-a, 4-b
- �� Option A → Magnitude and unit are interchanged.
- �� Option B → Unit and current relations are mismatched.
- �� Option D → Direction and unit are incorrectly matched.
Used – Formula Recall
- Application
- Recall the standard definitions of current density, drift velocity, and electric current.
- Final Logic
- j=I/A,∣j∣=ne∣v_d∣,I=jA
- and the SI unit of j is A/m².
- j follows E
16 By equating the derived microscopic equation
j=(ne^2τ/m)E
with the macroscopic Ohm's law form
j=σE
the conductivity σof a material is
�� Current density is proportional to electric field. �� Conductivity is the proportionality constant. �� Compare microscopic and macroscopic forms of Ohm's law.
The microscopic form of Ohm's law is j=(ne^2τ/m)E where n is the number density of free electrons, e is the electronic charge, τis the relaxation time, and m is the mass of an electron. The macroscopic form of Ohm's law is j=σE Comparing the coefficients of E, σ=ne^2τ/m Thus conductivity increases with carrier density and relaxation time and decreases with electron mass.
- �� Option A → Represents resistivity-related form.
- �� Option C → Missing one factor of e.
- �� Option D → Relaxation time incorrectly placed in denominator.
Used – Formula Recall
- Application
- Compare microscopic and macroscopic forms of Ohm's law.
- Final Logic
- j=(ne^2τ/m)E=σE
- Therefore,
- σ=ne^2τ/m
- Conductivity = Carriers × Charge² × Relaxation Time ÷ Mass
17 Correct statements about carrier mobility μ
Statements:
1. It is an important parameter in defining conductivity derived from mobile charge carriers.
2. It is defined as the magnitude of drift velocity per unit electric field.
3. It can be mathematically expressed as eτ/m for free electrons.
4. It is formally treated as a negative quantity for negatively charged electrons.
�� Mobility measures ease of carrier motion. �� Mobility relates drift velocity and electric field. �� Mobility contributes directly to conductivity.
Carrier mobility is defined as μ=∣v_d∣/E which represents the drift velocity acquired per unit electric field. Using the drift velocity relation v_d=eEτ/m we obtain μ=eτ/m for free electrons. Conductivity can also be written as σ=neμ showing the direct role of mobility in electrical conduction. Mobility is treated as a positive physical parameter representing magnitude. Therefore statement 4 is incorrect.
- �� Option A → Statement 4 is incorrect.
- �� Option B → Statement 4 is incorrect.
- �� Option C → Statement 4 is incorrect.
Used – Concept Application
- Application
- Use the definitions of drift velocity, mobility, and conductivity.
- Final Logic
- μ=∣v_d∣/E=eτ/m
- and
- σ=neμ
- Conductivity = Carrier Density × Charge × Mobility
18 If mobility is given as
4.5×10^3 cm^2/(V s)
its value in SI units is
�� 1 cm^2=10^(-4) m^2 �� Convert area units carefully. �� Multiply by 10^(-4).
Given, μ=4.5×10^3 cm^2/(V s) Since 1 cm^2=10^(-4) m^2 we get μ=(4.5×10^3)(10^(-4))μ=4.5×10^(-1)μ=0.45 m^2/(V s) Therefore Option A is correct.
- �� Option B → Incorrect power of ten.
- �� Option C → Conversion factor applied incorrectly.
- �� Option D → Unit conversion error.
Used – Unit Conversion
- Application
- Convert square centimetres into square metres.
- Final Logic
- 4.5×10^3×10^(-4)=0.45
- cm² → m² ⇒ Multiply by 10^(-4)
19 Incorrect statement regarding the estimation of electron density parameter in copper
�� Most copper atoms contribute conduction electrons. �� Electron density in copper is extremely large. �� Drift speed is small despite many free electrons.
Copper is an excellent conductor because a large number of its atoms contribute free electrons for conduction. The electron number density is of the order of 10^(29) m^(-3) and not a tiny fraction as stated in Option C. The commonly used values in estimating electron density are: • Density of copper ≈ 9.0×10^3 kg/m^3 • Atomic mass ≈ 63.5 g/mol • Avogadro number ≈ 6.0×10^(23) These values allow calculation of the number of atoms and hence the number of free electrons per unit volume.
- �� Option A → Correct numerical value.
- �� Option B → Correct density approximation.
- �� Option D → Correct Avogadro relation.
Used – Concept Application
- Application
- Use the free-electron model of metallic conduction.
- Final Logic
- Copper contains an enormous density of conduction electrons.
- Huge Density + Tiny Drift = Large Current
20 Thermal speed vs Drift speed vs Field propagation speed in a typical conductor
�� Thermal speed is very large. �� Drift speed is extremely small. �� Electrical signals propagate nearly at light speed.
Free electrons inside a conductor possess large random thermal speeds, typically hundreds of metres per second or more. However, when an electric field is applied, the resulting drift speed is extremely small, usually of the order of 10^(-4) to 10^(-3) m/s Despite this small drift velocity, electrical effects appear almost instantaneously because the electric field propagates through the conductor at a speed close to 3×10^8 m/s which is approximately the speed of light. Therefore, the correct order is: Thermal Speed → High Drift Speed → Extremely Low Field Propagation Speed → Speed of Light
- �� Option B → Thermal and drift speeds reversed.
- �� Option C → Field propagation is not limited to the speed of sound.
- �� Option D → Thermal speed is not equal to light speed.
Used – NCERT Recall
- Application
- Recall the characteristic orders of magnitude of important speeds in conductors.
- Final Logic
- Thermal Speed ≫ Drift Speed, while Field Propagation ≈ Speed of Light.
- Field → Light Speed
