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IB DP Physics Mock Exam SL Paper 1B Set 4 - 2025 Syllabus

IB DP Physics Mock Exam SL Paper 1B Set 4

Prepare for the IB DP Physics Mock Exam SL Paper 1B Set 4 with our comprehensive mock exam set 4. Test your knowledge and understanding of key concepts with challenging questions covering all essential topics. Identify areas for improvement and boost your confidence for the real exam

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Question 

A student investigates the resistivity \(\rho\) of a cylindrical metal wire. The following measurements are obtained:
Wire length \(L = (462 \pm 2)\,mm\)
Diameter \(d\) measurements taken at several positions along the wire:
Reading123456
\(d / mm\)\(0.18\)\(0.20\)\(0.21\)\(0.22\)\(0.26\)\(0.18\)
Wire resistance \(R = 13.7\,\Omega \pm 1.5\%\)
(a) Explain why measurements of \(d\) were taken at different positions along the wire.
(b) Recommend appropriate instruments for measuring:
(i) \(L\)
(ii) \(d\)
(c) (i) Show that the average diameter of the wire is approximately \(0.2\,mm\).
(ii) Determine the fractional uncertainty in the diameter of the wire.
(iii) Determine the fractional uncertainty in the length of the wire.
(d) The resistivity of the wire is calculated using \(\rho = \frac{RA}{L}\), where \(A\) is the cross-sectional area. Calculate \(\rho\) and its absolute uncertainty. Give your answers to a suitable number of significant figures.
▶️ Answer/Explanation
Detailed solution

(a)
Measurements are taken at different places to check for uniformity (such as variations in diameter or thickness) or to minimize the impact of random uncertainties by calculating an average .

(b)
(i) A metre ruler or a measuring tape with millimeter graduations is suitable, provided it is at least \(50\,cm\) long .
(ii) A micrometer screw gauge or a Vernier caliper should be used .

(c)
(i) The reading of \(0.26\,mm\) is considered an outlier and should be discarded. The mean of the remaining five readings is:
\(\frac{0.18 + 0.20 + 0.21 + 0.22 + 0.18}{5} = \frac{0.99}{5} = 0.198\,mm \approx 0.2\,mm\).
(ii) The range of the valid data is \(0.22 – 0.18 = 0.04\,mm\). The absolute uncertainty is half the range: \(\frac{0.04}{2} = 0.02\,mm\) .
The fractional uncertainty is:
\(\frac{0.02}{0.20} = 0.1 \text{ (or } 10\% \text{)}\) .
(iii) The fractional uncertainty in length is:
\(\frac{2}{462} \approx 0.004 \text{ (or } 0.4\% \text{)}\).

(d)
First, calculate the resistivity \(\rho\). Using the mean diameter \(d = 0.20\,mm = 2.0 \times 10^{-4}\,m\), the cross-sectional area is \(A = \pi (\frac{d}{2})^2\).
\(\rho = \frac{RA}{L} = \frac{13.7 \times \pi \times (1.0 \times 10^{-4})^2}{0.462} \approx 9.3 \times 10^{-7}\,\Omega m\) .

Determine the total fractional uncertainty in \(\rho\):
\(\frac{\Delta \rho}{\rho} = \frac{\Delta R}{R} + \frac{\Delta L}{L} + 2\left( \frac{\Delta d}{d} \right)\)
\(\frac{\Delta \rho}{\rho} = 0.015 + 0.004 + 2(0.1) = 0.219\) (or approx \(0.22\)) .
Calculate the absolute uncertainty \(\Delta \rho\):
\(\Delta \rho = 0.22 \times 9.3 \times 10^{-7} \approx 2.0 \times 10^{-7}\,\Omega m\) .

Final Answer:
\(\rho = (9 \pm 2) \times 10^{-7}\,\Omega m\).

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