Physics 2 Quiz: Units And Sign Conventions In Eandm
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Units And Sign Conventions In EandmQuestion 1 of 9

An infinite line charge with linear charge density λ>0\lambda > 0 is oriented along the zz-axis. The electric field in cylindrical coordinates is:

E=λ2πϵ0ss^\mathbf{E} = \frac{\lambda}{2\pi\epsilon_0 s} \hat{s}

where ss is the perpendicular distance from the axis. A student computes the potential difference V(a)V(b)V(a) - V(b) between two points at distances aa and bb from the axis (a<ba < b) using:

V(a)V(b)=baEdl=baλ2πϵ0sdsV(a) - V(b) = -\int_b^a \mathbf{E} \cdot d\mathbf{l} = -\int_b^a \frac{\lambda}{2\pi\epsilon_0 s} ds

The student evaluates this as λ2πϵ0ln(ba)\frac{\lambda}{2\pi\epsilon_0} \ln\left(\frac{b}{a}\right) and concludes this is positive, consistent with the fact that VV decreases as you move away from a positive line charge.

Which of the following correctly identifies any errors in the student's integral setup, evaluation, or sign reasoning?

The integral setup contains a sign error: the limits of integration should run from aa to bb, not bb to aa, to match the displacement direction. With corrected limits, the result is λ2πϵ0ln(b/a)\frac{\lambda}{2\pi\epsilon_0}\ln(b/a), which is still positive for b>ab > a, so the final answer and physical reasoning are correct despite the sign error in setup.
The setup, evaluation, and reasoning are all correct. The formula V(a)V(b)=baEsdsV(a) - V(b) = -\int_b^a E_s \, ds is valid because reversing the integration limits introduces a compensating sign flip, yielding +λ2πϵ0ln(b/a)>0+\frac{\lambda}{2\pi\epsilon_0}\ln(b/a) > 0, confirming that aa (closer to the line) is at higher potential.
The evaluation is wrong because the correct antiderivative of 1/s1/s is lns+C\ln|s| + C, which must be evaluated as [lns]ba=ln(a)ln(b)=ln(a/b)[\ln s]_b^a = \ln(a) - \ln(b) = \ln(a/b), giving a negative result that contradicts the stated sign. The student's final answer has the wrong sign.
The setup is wrong because V(a)V(b)=abEdlV(a) - V(b) = -\int_a^b \mathbf{E} \cdot d\mathbf{l}, not ba-\int_b^a. The corrected integral gives λ2πϵ0ln(b/a)<0-\frac{\lambda}{2\pi\epsilon_0}\ln(b/a) < 0, implying V(a)<V(b)V(a) < V(b), which is inconsistent with a positive line charge, revealing an error in the physical premise.
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Physics 2 Quiz

Physics 2 Quiz: Units And Sign Conventions In Eandm

Practice Units And Sign Conventions In Eandm in Physics 2 with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

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This quiz focuses on Units And Sign Conventions In Eandm, giving you a quick way to practice the rules, question types, and explanations that matter most for Physics 2.

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Question 1

An infinite line charge with linear charge density λ>0\lambda > 0 is oriented along the zz-axis. The electric field in cylindrical coordinates is:

E=λ2πϵ0ss^\mathbf{E} = \frac{\lambda}{2\pi\epsilon_0 s} \hat{s}

where ss is the perpendicular distance from the axis. A student computes the potential difference V(a)V(b)V(a) - V(b) between two points at distances aa and bb from the axis (a<ba < b) using:

V(a)V(b)=baEdl=baλ2πϵ0sdsV(a) - V(b) = -\int_b^a \mathbf{E} \cdot d\mathbf{l} = -\int_b^a \frac{\lambda}{2\pi\epsilon_0 s} ds

The student evaluates this as λ2πϵ0ln(ba)\frac{\lambda}{2\pi\epsilon_0} \ln\left(\frac{b}{a}\right) and concludes this is positive, consistent with the fact that VV decreases as you move away from a positive line charge.

Which of the following correctly identifies any errors in the student's integral setup, evaluation, or sign reasoning?

  1. The integral setup contains a sign error: the limits of integration should run from aa to bb, not bb to aa, to match the displacement direction. With corrected limits, the result is λ2πϵ0ln(b/a)\frac{\lambda}{2\pi\epsilon_0}\ln(b/a), which is still positive for b>ab > a, so the final answer and physical reasoning are correct despite the sign error in setup.
  2. The setup, evaluation, and reasoning are all correct. The formula V(a)V(b)=baEsdsV(a) - V(b) = -\int_b^a E_s \, ds is valid because reversing the integration limits introduces a compensating sign flip, yielding +λ2πϵ0ln(b/a)>0+\frac{\lambda}{2\pi\epsilon_0}\ln(b/a) > 0, confirming that aa (closer to the line) is at higher potential. (correct answer)
  3. The evaluation is wrong because the correct antiderivative of 1/s1/s is lns+C\ln|s| + C, which must be evaluated as [lns]ba=ln(a)ln(b)=ln(a/b)[\ln s]_b^a = \ln(a) - \ln(b) = \ln(a/b), giving a negative result that contradicts the stated sign. The student's final answer has the wrong sign.
  4. The setup is wrong because V(a)V(b)=abEdlV(a) - V(b) = -\int_a^b \mathbf{E} \cdot d\mathbf{l}, not ba-\int_b^a. The corrected integral gives λ2πϵ0ln(b/a)<0-\frac{\lambda}{2\pi\epsilon_0}\ln(b/a) < 0, implying V(a)<V(b)V(a) < V(b), which is inconsistent with a positive line charge, revealing an error in the physical premise.
Explanation: When working with potential differences, you need to track two things carefully: the definition of the line integral and what happens algebraically when you flip limits. The fundamental relation is V(a)V(b)=baEdlV(a) - V(b) = -\int_b^a \mathbf{E} \cdot d\mathbf{l}. Notice the limits run from bb to aa — this is not a typo. The definition states V(r)=refrEdlV(\mathbf{r}) = -\int_{\text{ref}}^{\mathbf{r}} \mathbf{E} \cdot d\mathbf{l}, so subtracting gives exactly this form. Plugging in the field, baλ2πϵ0sds=λ2πϵ0[lns]ba=λ2πϵ0(lnalnb)=λ2πϵ0ln ⁣(ba)-\int_b^a \frac{\lambda}{2\pi\epsilon_0 s}\,ds = -\frac{\lambda}{2\pi\epsilon_0}[\ln s]_b^a = -\frac{\lambda}{2\pi\epsilon_0}(\ln a - \ln b) = \frac{\lambda}{2\pi\epsilon_0}\ln\!\left(\frac{b}{a}\right). Since b>ab > a, this is positive — meaning the closer point aa is at higher potential, exactly right for a positive line charge. The student's setup, evaluation, and physical conclusion are all correct. B is the answer. Choice A claims there's a sign error in the limits, but the limits bab \to a are correct by definition — no error exists to fix. Choice C misapplies the antiderivative evaluation. [lns]ba=lnalnb[\ln s]_b^a = \ln a - \ln b, and after applying the leading negative sign you get +ln(b/a)+\ln(b/a), not ln(a/b)\ln(a/b). The student tracked the signs correctly. Choice D incorrectly "corrects" the limits to aba \to b, which actually introduces an error and produces the wrong sign, falsely suggesting V(a)<V(b)V(a) < V(b). Study tip: Whenever you flip integration limits, you pick up a minus sign. In the potential difference formula, those two negatives (one from the definition, one from flipping limits) cancel — so trust the algebra and always verify the physical sign against intuition.

Question 2

A student is solving for the magnetic flux through a flat circular loop of radius R=0.10 mR = 0.10 \text{ m} carrying no current, placed in an external uniform magnetic field B=B0z^\mathbf{B} = B_0 \hat{z} with B0=0.50 TB_0 = 0.50 \text{ T}. The loop lies in the xyxy-plane. The student chooses the area vector dA=dA(z^)d\mathbf{A} = dA(-\hat{z}), pointing in the z-z direction (downward), and computes:

ΦB=BA=B0(1)πR2=1.57×103 Wb\Phi_B = \mathbf{B} \cdot \mathbf{A} = B_0 (-1) \pi R^2 = -1.57 \times 10^{-3} \text{ Wb}

The student then applies Faraday's law: E=dΦB/dt\mathcal{E} = -d\Phi_B/dt. Since B0B_0 is constant, E=0\mathcal{E} = 0. The student concludes: 'My choice of area vector sign gave a negative flux, so Faraday's law will produce a positive EMF of +1.57×103+1.57 \times 10^{-3} V if the field later changes.'

Which of the following most accurately assesses the student's sign convention, flux calculation, and reasoning about Faraday's law?

  1. The flux calculation and zero-EMF result are correct, and the student's final claim is also correct: a negative flux that becomes more negative as B0B_0 increases gives dΦB/dt<0d\Phi_B/dt < 0, so E=dΦB/dt>0\mathcal{E} = -d\Phi_B/dt > 0 regardless of the rate of change.
  2. The flux calculation is correct and the EMF for constant BB is correctly zero, but the student's area vector choice is physically invalid. By convention, the area vector of a loop in the xyxy-plane must point in the +z+z direction, so choosing z^-\hat{z} violates the standard sign convention for flux.
  3. The flux calculation is wrong because magnetic flux must always be positive. The correct flux is +1.57×103 Wb+1.57 \times 10^{-3} \text{ Wb}, and the resulting EMF from Faraday's law would be negative for an increasing B0B_0.
  4. The flux calculation and the zero-EMF result for constant BB are both correct. However, the student's final claim is wrong: the sign of the induced EMF depends on whether B0B_0 increases or decreases, not on the sign of ΦB\Phi_B alone. The student's statement is only valid for increasing B0B_0. (correct answer)
Explanation: Whenever you see a question involving Faraday's law and sign conventions, your job is to separately evaluate three things: the flux calculation, the EMF result, and any reasoning about hypothetical future scenarios. Here, the student's flux calculation is legitimate. Choosing dA=dA(z^)d\mathbf{A} = dA(-\hat{z}) is a perfectly valid convention — the sign of the area vector is a free choice, and the resulting ΦB=B0πR2=1.57×103\Phi_B = -B_0\pi R^2 = -1.57 \times 10^{-3} Wb is internally consistent. Since B0B_0 is constant, dΦB/dt=0d\Phi_B/dt = 0, so E=0\mathcal{E} = 0 is also correct. The problem lies in the student's final claim. The student asserts that a negative flux automatically produces a positive EMF if the field changes — but that's incomplete. If B0B_0 increases, then ΦB\Phi_B becomes more negative, giving dΦB/dt<0d\Phi_B/dt < 0, so E=dΦB/dt>0\mathcal{E} = -d\Phi_B/dt > 0. But if B0B_0 decreases, dΦB/dt>0d\Phi_B/dt > 0, making E<0\mathcal{E} < 0. The sign of the induced EMF depends on the rate of change of flux, not on the sign of ΦB\Phi_B alone. That's exactly what answer D captures. Answer A is wrong because it claims the positive EMF result holds "regardless of the rate of change" — this ignores the possibility of a decreasing field. Answer B is wrong because it invents a rule that doesn't exist: there is no requirement that the area vector point in +z^+\hat{z}; both orientations are valid. Answer C is wrong because magnetic flux is absolutely allowed to be negative — the sign is physically meaningful and convention-dependent. Your takeaway: never conflate the sign of flux with the sign of EMF. Faraday's law responds to how flux changes, so always ask whether the field is increasing or decreasing before drawing conclusions about the induced EMF's direction.

Question 3

A student is computing the electric potential energy of a system of two point charges. She writes:

U=kq1q2rU = k \frac{q_1 q_2}{r}

where k=8.99×109 Nm2/C2k = 8.99 \times 10^9 \text{ N}\cdot\text{m}^2/\text{C}^2, q1=+3μCq_1 = +3 \, \mu\text{C}, q2=5μCq_2 = -5 \, \mu\text{C}, and r=0.12 mr = 0.12 \text{ m}. She obtains U1.12 JU \approx -1.12 \text{ J}. She then claims: 'Because U is negative, work must be done on the system to separate these charges to infinity, and the magnitude of that work equals 1.12 J.'

Which of the following correctly evaluates the student's unit analysis and physical interpretation?

  1. Both the unit analysis and the interpretation are correct. The units of kq1q2/rk q_1 q_2 / r reduce to joules, and a negative potential energy means an attractive configuration requires positive external work equal to U|U| to separate the charges. (correct answer)
  2. The unit analysis is correct, but the interpretation is wrong. A negative UU means the system is in a repulsive configuration, so the external agent receives energy rather than supplies it when separating the charges.
  3. The unit analysis is correct, but the interpretation is wrong. A negative UU means the system is bound, so energy must be removed from the system—not added—to separate the charges, meaning the external agent does negative work.
  4. The unit analysis is wrong because μC\mu\text{C} values must be converted to nanocoulombs before the formula applies, and the interpretation is wrong because the sign of UU alone cannot determine the direction of work without knowing the sign of the force.
Explanation: When tackling a question like this, you need to evaluate two separate claims independently: dimensional consistency and physical interpretation of sign. For the unit analysis, check that kq1q2/rk q_1 q_2 / r yields joules. Since kk carries units of Nm2/C2\text{N}\cdot\text{m}^2/\text{C}^2, multiplying by two charges in coulombs gives Nm2\text{N}\cdot\text{m}^2, and dividing by meters gives Nm=J\text{N}\cdot\text{m} = \text{J}. This works regardless of whether the charges are expressed in microcoulombs or any other prefix, as long as you convert to base SI units (C) before computing — which the student implicitly did, since she arrived at a numerically correct result of 1.12 J-1.12 \text{ J}. For the physical interpretation, a negative UU means the charges are in a bound, attractive configuration (opposite signs attract). To pull them apart to infinity — where U=0U = 0 by convention — you must increase the potential energy from 1.12 J-1.12 \text{ J} to 00. That requires an external agent to do positive work of exactly U=1.12 J|U| = 1.12 \text{ J}. The student's claim is correct, making A the right answer. B is wrong because it reverses the physics: negative UU signals attraction, not repulsion. Opposite charges attract, which is precisely why UU is negative here. C is wrong in the opposite direction — it confuses "bound system" with needing to remove energy. Separating bound charges requires energy input, not removal. D is wrong on both counts: unit prefixes like μC\mu\text{C} are perfectly valid as long as you convert properly, and the sign of UU absolutely does determine the direction of work for a two-charge system at a known separation. Study tip: Always evaluate unit analysis and physical interpretation as two separate questions — exams frequently make one correct and one wrong to catch students who conflate them.

Question 4

A student is computing the force on a charge q=2μCq = -2 \, \mu\text{C} moving with velocity v=3×105x^ m/s\mathbf{v} = 3 \times 10^5 \hat{x} \text{ m/s} through a magnetic field B=0.4z^ T\mathbf{B} = 0.4 \hat{z} \text{ T}. Using the Lorentz force law F=qv×B\mathbf{F} = q\mathbf{v} \times \mathbf{B}, the student evaluates the cross product as x^×z^=y^\hat{x} \times \hat{z} = -\hat{y} and writes:

F=(2×106)(3×105)(0.4)(y^)=+0.24y^ N\mathbf{F} = (-2 \times 10^{-6})(3 \times 10^5)(0.4)(-\hat{y}) = +0.24 \hat{y} \text{ N}

The student claims: 'The force is in the +y^+\hat{y} direction because the negative charge reverses the direction from the cross product result.'

Which of the following correctly evaluates the student's cross product, sign handling, and final force direction?

  1. The cross product is wrong: x^×z^=y^\hat{x} \times \hat{z} = -\hat{y} is correct, but the final force is 0.24y^ N-0.24\hat{y}\text{ N}, not +0.24y^ N+0.24\hat{y}\text{ N}. The student made a sign error by applying the negative charge's sign twice—once in the magnitude factor and once in the 'reversal' claim.
  2. The cross product is correct (x^×z^=y^\hat{x} \times \hat{z} = -\hat{y}), the sign handling is correct (negative qq reverses direction), and the final result +0.24y^ N+0.24\hat{y}\text{ N} is correct. The student's full calculation contains no errors. (correct answer)
  3. The cross product is wrong: x^×z^=+y^\hat{x} \times \hat{z} = +\hat{y}, not y^-\hat{y}. With the correct cross product, the force on the negative charge becomes 0.24y^ N-0.24\hat{y}\text{ N}, pointing in the y^-\hat{y} direction.
  4. The cross product is wrong: x^×z^=+y^\hat{x} \times \hat{z} = +\hat{y}, not y^-\hat{y}. With the correct cross product and the sign of the negative charge, the force is +0.24y^ N+0.24\hat{y}\text{ N}, which agrees with the student's final answer even though the intermediate step was wrong.
Explanation: When applying the Lorentz force law F=qv×B\mathbf{F} = q\mathbf{v} \times \mathbf{B}, you must handle the cross product and the charge's sign as one unified algebraic calculation — not as separate conceptual "reversals." The student's calculation is actually correct. First, verify the cross product: using the right-hand rule and the cyclic identity x^×y^=z^\hat{x} \times \hat{y} = \hat{z}, we get x^×z^=y^\hat{x} \times \hat{z} = -\hat{y}. This is right. Then, plugging everything in: F=(2×106)(3×105)(0.4)(y^)\mathbf{F} = (-2 \times 10^{-6})(3 \times 10^5)(0.4)(-\hat{y}) The scalar part gives (2×106)(3×105)(0.4)=0.24(-2 \times 10^{-6})(3 \times 10^5)(0.4) = -0.24, and multiplying by y^-\hat{y} yields +0.24y^ N+0.24\hat{y} \text{ N}. The student's arithmetic is clean, and the explanation — that the negative charge reverses the cross-product direction — is a valid conceptual shortcut, not a double-counted sign. Answer B is correct. Answer A claims the student applied the negative sign twice, but that's not what happened. The single factor of q=2×106q = -2\times10^{-6} is already included in the numerical product; saying "negative charge reverses direction" is just a verbal restatement of that same mathematics, not an additional operation. Answer C incorrectly states x^×z^=+y^\hat{x} \times \hat{z} = +\hat{y}, which reverses the cross product's sign — a right-hand rule error. Answer D also gets the cross product wrong (same error as C) and only accidentally recovers the right final answer through compensating mistakes. Study tip: Always treat qv×Bq\mathbf{v}\times\mathbf{B} as a single algebraic expression. Don't apply the charge sign separately after deciding a direction — let the math handle it all at once to avoid double-counting errors.

Question 5

A student uses the standard sign convention for circuits: current is defined as the flow of positive charge, and the potential drops in the direction of conventional current through a resistor. She sets up a loop equation for a single-loop circuit containing an EMF source E\mathcal{E} (ideal, 12 V), a resistor R1=4ΩR_1 = 4 \, \Omega, and a resistor R2=8ΩR_2 = 8 \, \Omega, traversing the loop clockwise. She assigns clockwise current I>0I > 0 and writes:

EIR1IR2=0\mathcal{E} - I R_1 - I R_2 = 0

She obtains I=1 AI = 1 \text{ A}. She then states: 'The terminal voltage across R2R_2 is +8 V+8 \text{ V}, with the left terminal of R2R_2 being at higher potential if current enters from the left.'

Assuming the traversal and sign convention are applied consistently, which statement best evaluates the student's loop equation, her current result, and her terminal-voltage claim?

  1. The loop equation is correct, I=1 AI = 1 \text{ A} is correct, and the terminal-voltage claim is correct: conventional current entering a resistor from one side means that side is at higher potential, consistent with V=IR=8 VV = IR = 8 \text{ V}. (correct answer)
  2. The loop equation is correct and I=1 AI = 1 \text{ A} is correct, but the terminal-voltage claim is wrong: the side where current exits a resistor is at higher potential, so the right terminal of R2R_2 is at higher potential.
  3. The loop equation has a sign error because the EMF term should be negative when traversed in the direction of conventional current inside the source, giving I=1 AI = -1 \text{ A}, which means the actual current is counterclockwise and the terminal-voltage claim is reversed.
  4. The loop equation is correct and I=1 AI = 1 \text{ A} is correct, but the terminal-voltage claim is ambiguous without knowing the internal resistance of the source, because the terminal voltage of R2R_2 depends on the voltage drop across the source's internal resistance as well.
Explanation: Kirchhoff's Voltage Law (KVL) questions test two things simultaneously: your ability to write a correct loop equation and your understanding of what that equation physically means for individual components. Keep both in mind as you evaluate each part of the student's work. The student's loop equation EIR1IR2=0\mathcal{E} - IR_1 - IR_2 = 0 is textbook KVL: traversing clockwise, you gain potential across the EMF source and lose potential across each resistor. Solving gives I=124+8=1 AI = \frac{12}{4+8} = 1 \text{ A}, which is correct. Her terminal-voltage claim is also correct — in a resistor, conventional current flows from higher potential to lower potential, meaning the side where current enters is at higher potential. With I=1 AI = 1 \text{ A} through R2=8ΩR_2 = 8\,\Omega, the voltage across it is V=IR2=8 VV = IR_2 = 8\text{ V}, and the entering (left) terminal is indeed at higher potential. Answer A correctly validates all three parts. Answer B reverses the potential rule for resistors — current flows from high to low potential through a resistor, so the entry side is higher, not the exit side. This is a common misconception worth eliminating now. Answer C misapplies the sign convention for EMF sources. When you traverse a battery from − to + (in the direction the source drives current), you gain potential, so the EMF term is positive. There is no sign error here. Answer D introduces a red herring. The problem explicitly states the source is ideal, meaning zero internal resistance. Terminal voltage of R2R_2 is simply IR2IR_2, with no ambiguity. Study tip: Always pair KVL with the physical rule — current in a resistor runs from high to low potential. Memorizing this eliminates the trap in B every time.

Question 6

The Biot–Savart law in SI units is dB=μ04πIdl×r^r2d\mathbf{B} = \frac{\mu_0}{4\pi} \frac{I \, d\mathbf{l} \times \hat{r}}{r^2}. A student claims that the units of μ0\mu_0 must be T·m/A (equivalently H/m) so that the expression yields tesla for dBd\mathbf{B}. A second student claims that the factor μ0/(4π)\mu_0/(4\pi) taken together has units of T·m/A (not μ0\mu_0 alone). Which of the following correctly adjudicates this dispute and performs the necessary dimensional analysis?

  1. The first student is correct. Since 4π4\pi is dimensionless, it does not contribute units, so μ0\mu_0 itself carries T·m/A. Dimensional analysis confirms: (Tm/A)(A)(m)/(m2)=T(\text{T}\cdot\text{m/A})(\text{A})(\text{m})/(\text{m}^2) = \text{T}. (correct answer)
  2. The second student is correct. Because 4π4\pi appears in the denominator, dimensional analysis must treat μ0/(4π)\mu_0/(4\pi) as a single combined constant; assigning units to μ0\mu_0 alone is physically meaningless in SI.
  3. Neither student is correct. The Biot–Savart formula yields units of Wb/m (webers per meter), not tesla, because the cross product dl×r^d\mathbf{l} \times \hat{r} introduces an extra factor of meters that prevents the result from reducing to tesla.
  4. The first student is correct in the unit assignment but wrong about the equivalence: the SI unit T·m/A cannot be rewritten as N/A² or H/m, because those alternative forms apply only in Gaussian units and introduce a factor of 4π4\pi when converted to SI.
Explanation: Whenever you encounter a dimensional analysis question involving physical constants, the key principle to remember is that pure numbers are dimensionless — they scale a quantity but never contribute or remove units. This question tests whether you understand that 4π4\pi is simply a dimensionless geometric factor. Because 4π4\pi carries no units, μ0\mu_0 and μ0/(4π)\mu_0/(4\pi) must have identical units. To find them, work backward from the Biot–Savart law. You need dBdB in tesla (T), and the remaining factors contribute Am/m2=A/m\text{A} \cdot \text{m} / \text{m}^2 = \text{A/m}. So μ0\mu_0 must supply the missing T·m/A to make the product equal T: (TmA)Amm2=T\left(\frac{\text{T}\cdot\text{m}}{\text{A}}\right) \cdot \frac{\text{A} \cdot \text{m}}{\text{m}^2} = \text{T} \checkmark This confirms Answer A is correct: μ0\mu_0 itself has units of T·m/A, and the dimensional check closes perfectly. Answer B is wrong because it introduces a false claim — that 4π4\pi being in the denominator forces you to treat μ0/(4π)\mu_0/(4\pi) as an inseparable unit-bearing object. Dimensionless numbers never affect units, period. Answer C is wrong because the cross product dl×r^d\mathbf{l} \times \hat{r} involves a unit vector r^\hat{r}, which is dimensionless. So the cross product contributes only meters (from dld\mathbf{l}), not an extra factor — the result is indeed tesla, not Wb/m. Answer D is wrong because T·m/A, N/A², and H/m are all equivalent SI units for μ0\mu_0. These are not Gaussian-specific forms; the equivalence holds entirely within SI. Study tip: Always check whether a number in a formula is dimensionless before letting it influence your unit analysis — and verify unit equivalences (T·m/A = N/A² = H/m) by expanding each into base SI units: kg·m·s⁻²·A⁻².

Question 7

Maxwell's displacement current density is defined as Jd=ϵ0Et\mathbf{J}_d = \epsilon_0 \frac{\partial \mathbf{E}}{\partial t}. A student checks units: [ϵ0][E/t]=(C2/(Nm2))(V/(ms))[\epsilon_0][\partial E/\partial t] = (\text{C}^2/(\text{N}\cdot\text{m}^2))(\text{V/(m}\cdot\text{s)}). She simplifies V=Nm/C\text{V} = \text{N}\cdot\text{m/C} and claims the result is A/m2\text{A/m}^2, which she identifies as the correct SI unit for current density. Which of the following correctly evaluates her unit analysis?

  1. Her analysis is wrong in the intermediate step: C2/(Nm2)\text{C}^2/(\text{N}\cdot\text{m}^2) times Nm/(Cms)\text{N}\cdot\text{m/(C}\cdot\text{m}\cdot\text{s)} yields C/(Nms)\text{C/(N}\cdot\text{m}\cdot\text{s)}, not C/(m2s)\text{C/(m}^2\cdot\text{s)}, because the Newton units do not fully cancel, and the result is not dimensionally equivalent to current density.
  2. Her analysis is wrong because she should use [ϵ0]=F/m[\epsilon_0] = \text{F/m} and [E]=V/m[E] = \text{V/m}, giving FmVms=FVm2s=Cm2s\frac{\text{F}}{\text{m}} \cdot \frac{\text{V}}{\text{m}\cdot\text{s}} = \frac{\text{F}\cdot\text{V}}{\text{m}^2\cdot\text{s}} = \frac{\text{C}}{\text{m}^2\cdot\text{s}}, which simplifies to A/m2\text{A/m}^2. Her method gives the right answer but uses a non-standard form of [ϵ0][\epsilon_0] that introduces an error of a factor of 4π4\pi in SI.
  3. Her analysis is wrong because she identified the final unit as A/m2\text{A/m}^2 when the correct unit of current density is A/m\text{A/m} (amperes per meter), which describes surface current density, not volume current density, and the displacement current is inherently a surface phenomenon.
  4. Her analysis is correct. Substituting V=Nm/C\text{V} = \text{N}\cdot\text{m/C} gives C2Nm2NmCms=Cm2s=A/m2\frac{\text{C}^2}{\text{N}\cdot\text{m}^2} \cdot \frac{\text{N}\cdot\text{m}}{\text{C}\cdot\text{m}\cdot\text{s}} = \frac{\text{C}}{\text{m}^2 \cdot \text{s}} = \text{A/m}^2, which is indeed the SI unit of current density. (correct answer)
Explanation: When checking units in electromagnetism, your goal is to systematically substitute known equivalences and track cancellations — treat it like algebraic simplification where units are variables. The student's approach is sound. Starting with C2Nm2Vms\frac{\text{C}^2}{\text{N}\cdot\text{m}^2} \cdot \frac{\text{V}}{\text{m}\cdot\text{s}}, she substitutes V=Nm/C\text{V} = \text{N}\cdot\text{m/C}, giving C2Nm2NmCms\frac{\text{C}^2}{\text{N}\cdot\text{m}^2} \cdot \frac{\text{N}\cdot\text{m}}{\text{C}\cdot\text{m}\cdot\text{s}}. Now cancel: one factor of N cancels, one factor of m cancels, and one factor of C cancels, leaving Cm2s\frac{\text{C}}{\text{m}^2 \cdot \text{s}}. Since C/s=A\text{C/s} = \text{A}, the result is A/m2\text{A/m}^2 — exactly the SI unit for volume current density. Answer D is correct. Answer A claims the Newton units don't fully cancel, but if you carefully count the powers — N¹ in the numerator and N¹ in the denominator — they cancel completely. This is simply an arithmetic error in tracking the algebra. Answer B introduces a false claim that using [ϵ0]=C2/(Nm2)[\epsilon_0] = \text{C}^2/(\text{N}\cdot\text{m}^2) introduces a factor of 4π4\pi error. This is entirely fabricated — C2/(Nm2)\text{C}^2/(\text{N}\cdot\text{m}^2) is a perfectly valid SI expression for [ϵ0][\epsilon_0], equivalent to F/m. The alternative route through F/m also yields A/m2\text{A/m}^2, confirming both paths agree. Answer C confuses volume current density (A/m2\text{A/m}^2) with surface (linear) current density (A/m\text{A/m}). Displacement current density is indeed a volume quantity, so A/m2\text{A/m}^2 is correct. Study tip: When verifying units, write every substitution explicitly and tally exponents for each base unit — most unit errors come from losing track of a single power of a variable.

Question 8

In the context of a parallel-plate capacitor with plate separation dd, area AA, and permittivity ϵ0\epsilon_0, the energy stored is U=Q2/(2C)U = Q^2/(2C) where C=ϵ0A/dC = \epsilon_0 A/d. A student argues: 'Since U=Q2d/(2ϵ0A)U = Q^2 d / (2\epsilon_0 A), increasing plate separation dd at fixed charge QQ increases the stored energy. But energy is conserved, so the extra energy must come from the work done by the electric field as the plates attract each other—meaning the electric force between the plates is repulsive, not attractive.' Which of the following correctly identifies the error in the student's reasoning about signs and energy bookkeeping?

  1. The student correctly identifies that UU increases with dd and correctly concludes the force is attractive, since a system naturally moves to minimize energy, and attraction would decrease dd, reducing UU. The error is only in stating that the 'electric field does work'—it is the external agent, not the field, that transfers energy.
  2. The student's energy formula is correct, but the conclusion that UU increases with dd is wrong at fixed QQ. Because CC decreases with dd and U=Q2/(2C)U = Q^2/(2C), increasing dd actually decreases UU, so the electric force must be repulsive to push the plates apart and do negative work on the system.
  3. The student's energy formula and the conclusion that UU increases with dd are correct, but the sign reasoning is inverted. If an external agent must do positive work to separate the plates against an attractive force, the energy input from the external agent accounts for the increase in UU. The electric force is attractive, not repulsive, consistent with opposite charges on the plates. (correct answer)
  4. The student's energy formula contains a unit error: Q2d/(2ϵ0A)Q^2 d/(2\epsilon_0 A) has units of C2m/(C2/(Nm2)m2)=Nm3/m=Nm2\text{C}^2 \cdot \text{m} / (\text{C}^2/(\text{N}\cdot\text{m}^2) \cdot \text{m}^2) = \text{N}\cdot\text{m}^3/\text{m} = \text{N}\cdot\text{m}^2, not joules, so the entire analysis is dimensionally invalid before any physical reasoning is applied.
Explanation: When analyzing energy storage in capacitors, the key skill is tracking where energy comes from and what sign the forces have — two separate questions that must not be conflated. The student gets the math right: substituting C=ϵ0A/dC = \epsilon_0 A/d into U=Q2/(2C)U = Q^2/(2C) gives U=Q2d/(2ϵ0A)U = Q^2 d/(2\epsilon_0 A), which genuinely increases as dd increases at fixed QQ. So far, so good. The fatal mistake is in the energy bookkeeping. When you pull the plates apart against an attractive force, you — the external agent — must do positive work. That work is the source of the additional stored energy. The electric force does negative work (it opposes the separation), which is exactly what you expect from an attractive force. The student confused "the system gains energy" with "the electric field must have done positive work," inverting the sign logic entirely. Answer C correctly pinpoints this: the increase in UU is funded by the external agent, and the electric force remains attractive, as it must be between opposite charges. Answer A is wrong on two counts: it claims the student's force conclusion is correct (it isn't — the student said repulsive), and its distinction between "field work" and "external agent work" doesn't address the actual error. Answer B is factually incorrect — U=Q2/(2C)U = Q^2/(2C) absolutely increases when CC decreases, so the premise that UU decreases is simply false. Answer D invents a dimensional error that doesn't exist; the units of Q2d/(2ϵ0A)Q^2 d/(2\epsilon_0 A) do work out to joules correctly. Study tip: Whenever stored energy increases, always ask who supplied that energy — the external agent or the field — before drawing conclusions about force direction. Getting the sign right requires tracking the full energy budget.

Question 9

Consider the continuity equation for charge: J=ρt\nabla \cdot \mathbf{J} = -\frac{\partial \rho}{\partial t}, where J\mathbf{J} is the free current density (A/m²) and ρ\rho is the free charge density (C/m³). A student checks this equation dimensionally and writes:

[J]=A/m2m=Am3[\nabla \cdot \mathbf{J}] = \frac{\text{A/m}^2}{\text{m}} = \frac{\text{A}}{\text{m}^3}

[ρt]=C/m3s=Cm3s\left[\frac{\partial \rho}{\partial t}\right] = \frac{\text{C/m}^3}{\text{s}} = \frac{\text{C}}{\text{m}^3 \cdot \text{s}}

The student concludes: 'These have different units—A/m³ versus C/(m³·s)—so the continuity equation is dimensionally inconsistent unless a conversion factor is included.'

Which of the following correctly identifies the flaw in the student's dimensional analysis?

  1. The student applied the divergence operator incorrectly. The correct result is [J]=A/m2[\nabla \cdot \mathbf{J}] = \text{A/m}^2 (not A/m³), because \nabla \cdot acts on the vector components without reducing the overall dimension by one power of length.
  2. The student's error is in the divergence step: \nabla \cdot does not divide by meters but by seconds, because spatial derivatives in Maxwell's equations carry implicit time dependence. Correcting this gives [J]=C/(m2s2)[\nabla \cdot \mathbf{J}] = \text{C/(m}^2\cdot\text{s}^2), which still differs from [ρ/t][\partial\rho/\partial t].
  3. The student overlooks that 1 A=1 C/s1 \text{ A} = 1 \text{ C/s} by definition, so A/m3=C/(m3s)\text{A/m}^3 = \text{C/(m}^3\cdot\text{s)}. Both sides carry identical dimensions, and the continuity equation is dimensionally consistent without any conversion factor. (correct answer)
  4. The student's definition of ρ\rho is wrong. In the continuity equation, ρ\rho represents charge per unit volume per unit time, with units C/(m³·s), so [ρ/t]=C/(m3s2)[\partial\rho/\partial t] = \text{C/(m}^3\cdot\text{s}^2). This corrected form makes both sides dimensionally consistent.
Explanation: Dimensional analysis in electromagnetism often trips students up when they forget the fundamental definitions linking electrical units. When you see a question like this, your first instinct should be to check whether the units involved have hidden relationships — especially between amperes, coulombs, and seconds. The student's arithmetic is actually correct: [J]=A/m3[\nabla \cdot \mathbf{J}] = \text{A/m}^3 and [ρ/t]=C/(m3s)[\partial\rho/\partial t] = \text{C/(m}^3\cdot\text{s)}. The mistake is concluding these differ. By definition, the ampere is exactly one coulomb per second: 1 A=1 C/s1\text{ A} = 1\text{ C/s}. Substituting this into the left side gives A/m3=C/(sm3)\text{A/m}^3 = \text{C/(s}\cdot\text{m}^3), which is identical to the right side. No conversion factor is needed — the continuity equation is perfectly consistent. Answer C correctly identifies this oversight. A is wrong because the divergence operator does divide by length — applying \nabla\cdot to a quantity in A/m² genuinely yields A/m³. The student's divergence step was fine; the error came afterward. B is a fabricated rule. The \nabla operator involves spatial derivatives (dividing by meters), not temporal ones. There is no principle in Maxwell's equations that makes spatial derivatives "carry seconds." This answer invents a correction that produces a dimensionally inconsistent result anyway. D is wrong because ρ\rho is defined as charge per unit volume, C/m³ — not charge per unit volume per unit time. Redefining it to fix a perceived inconsistency that doesn't actually exist is unnecessary and incorrect. Study tip: Memorize the base-unit definitions of common electrical quantities — especially 1 A=1 C/s1\text{ A} = 1\text{ C/s} and 1 V=1 J/C1\text{ V} = 1\text{ J/C}. Many "inconsistencies" in dimensional checks dissolve the moment you expand derived units into their SI base components.