📚 Experimental Investigation: Determining the Resistivity of a Metal Wire | 实验探究：测定金属丝的电阻率
This article explores a core practical investigation commonly encountered in AS Physics: measuring the resistivity of a uniform metal wire. Resistivity is an intrinsic material property that quantifies how strongly a given material opposes the flow of electric current. By combining measurements of resistance, length and cross-sectional area, we can calculate resistivity and evaluate experimental uncertainties. The investigation reinforces essential skills in circuit building, data collection, graphical analysis and error propagation.
本文探讨AS物理中一个常见的核心实验探究：测量均匀金属丝的电阻率。电阻率是物质的本征属性，用于量化材料对电流阻碍作用的强弱。通过综合测量电阻、长度和横截面积，我们可以计算出电阻率并评估实验误差。这一探究有助于巩固电路搭建、数据采集、图像分析和误差传递等基本实验技能。
1. Aim and Background | 实验目的与背景
the wire diameter. By measuring R for different lengths of the same wire at constant temperature, we can determine ρ from the gradient of a suitable graph. This method assumes ohmic behaviour and minimal temperature rise.
材料的电阻率 ρ 由公式 R = ρL/A 定义，其中 R 是电阻，L 是长度，A 是横截面积。对于均匀圆柱形金属丝，A = πd²/4，d 为丝径。通过在恒定温度下测量同一金属丝不同长度对应的电阻，我们可以由合适图像的斜率确定 ρ。该方法假定元件满足欧姆定律且温升极小。
2. Equipment and Setup | 仪器与装置
A typical setup includes: a metre ruler, a micrometer screw gauge, a resistance wire (e.g., constantan or nichrome) of about 1 m, an ammeter (0–1 A), a voltmeter (0–5 V), a variable DC power supply or battery pack, connecting leads with crocodile clips, a switch, and a jockey or movable contact. The wire is mounted tautly along the ruler, with one end connected to the circuit. The jockey allows resistance measurement at exact lengths.
典型装置包括：米尺、螺旋测微器、长约1 m的电阻丝（如康铜或镍铬合金）、电流表（0–1 A）、电压表（0–5 V）、可调直流电源或电池组、带鳄鱼夹的导线、开关以及滑动触头或可移动接点。金属丝沿米尺绷紧安装，一端接入电路。滑动触头允许在精确长度处测量电阻。
3. Variables and Control | 变量与控制
lled variables: wire material (kept the same), wire diameter (measured and assumed constant along the length), temperature (minimise current to reduce heating; keep the same wire gauge), and ambient conditions. Keeping the current low (<0.5 A) prevents temperature-dependent resistance changes.
自变量：金属丝固定端与滑动触头之间的长度 L。因变量：电阻 R，由电压表和电流表读数通过 R = V/I 计算得出。控制变量：材料（保持不变）、直径（已测量并假设沿长度均匀）、温度（减小电流以降低发热，保持同一线径），以及环境条件。保持电流较小（<0.5 A）可防止因温度引起的电阻变化。
4. Experimental Procedure | 实验步骤
oltmeter in parallel across the test length, and the power supply. 3. Start with L = 1.000 itch, quickly read V and I, then open the switch to avoid heating. 4. Repeat for L = 0.900 m, 0.800 m, …, down to 0.100 m. 5. For each length, calculate R and record in a table.
1. 使用螺旋测微器在金属丝多个位置测量直径 d，记录平均值和零误差。2. 搭建电路：金属丝与电流表串联，电压表并联在被测长度两端，接入电源。3. 将滑动触头置于远端，从 L = 1.000 m 开始。闭合开关，迅速读取 V 和 I，随即断开开关以免发热。4. 对 L = 0.900 m、0.800 m……直至 0.100 m 重复实验。5. 计算每个长度对应的 R 并记录在表格中。
5. Data Collection and Table Design | 数据收集与表格设计
e to include columns for repeat V and I readings and mean values if time permits. Ensure all raw data are recorded to the precision of the instruments (e.g., ammeter to 0.01 A, voltmeter to 0.01 V). A sample table is shown below.
设计表格，列包括：长度 L (m)、电压 V (V)、电流 I (A)、电阻 R = V/I (Ω)。若时间允许，应列出 V 和 I 的重复读数及平均值。确保所有原始数据按仪器精度记录（如电流表精确至0.01 A，电压表精确至0.01 V）。下表为示例。
| L / m | V / V | I / A | R / Ω |
|---|---|---|---|
| 1.000 | 0.92 | 0.32 | 2.88 |
| 0.800 | 0.75 | 0.33 | 2.27 |
| 0.600 | 0.56 | 0.33 | 1.70 |
| 0.400 | 0.38 | 0.34 | 1.12 |
| 0.200 | 0.19 | 0.33 | 0.58 |
6. Graphical Analysis | 图像分析
tional area A is found from A = πd²/4 using the mean diameter d. For example, if d = 0.274 mm (±0.001 mm), A = π(0.274×10⁻³)²/4 = 5.90×10⁻⁸ m².
绘制电阻 R（y轴）与长度 L（x轴）的关系图。根据 R = (ρ/A)L，图像应为一条通过原点的直线，斜率 m = ρ/A。由最佳拟合线计算斜率，然后由 ρ = m × A 求 ρ。横截面积 A 由平均直径 d 通过 A = πd²/4 求得。例如，若 d = 0.274 mm（±0.001 mm），则 A = π(0.274×10⁻³)²/4 = 5.90×10⁻⁸ m²。
7. Calculations and Result | 计算与结果
Suppose the gradient from the R–L graph is 2.87 Ω m⁻¹. Then ρ = 2.87 Ω m⁻¹ × 5.90×10⁻⁸ m² = 1.69×10⁻⁷ Ω m. This is consistent with the resistivity of nichrome (around 1.10–1.50×10⁻⁶ Ω m? wait, careful: typical nichrome is ~1.0×10⁻⁶, constantan ~4.9×10⁻⁷, so 1.69×10⁻⁷ seems low; adjust numbers to be realistic. I'll use constantan. Let's set gradient = 7.8 Ω m⁻¹, A = 6.0×10⁻⁸ m² gives ρ = 4.68×10⁻⁷ Ω m, near constantan. I'll use that.) So: gradient m = 7.80 Ω m⁻¹, A = 6.03×10⁻⁸ m², yielding ρ = 4.70×10⁻⁷ Ω m. The accepted value for constantan is about 4.9×10⁻⁷ Ω m. The result is reasonable.
设 R–L 图的斜率为 7.80 Ω m⁻¹，横截面积 A = 6.03×10⁻⁸ m²，则 ρ = 7.80 × 6.03×10⁻⁸ = 4.70×10⁻⁷ Ω m。康铜电阻率的公认值约为 4.9×10⁻⁷ Ω m，实验值与此相符。
ρ = m × A = 7.80 Ω m⁻¹ × 6.03×10⁻⁸ m² = 4.70×10⁻⁷ Ω m
8. Uncertainty Analysis | 不确定度分析
l sources contribute to uncertainty: the precision of the length measurement (typically ±1 d jockey positioning), the precision of the diameter measurement (micrometer reads to 0.01 om graph) and area. The area uncertainty is twice the percentage uncertainty in d, since A ∝ d². A full error propagation can be carried out using worst-case lines on the graph.
多种因素引入不确定度：长度测量的精度（通常由米尺和滑动触头定位产生 ±1 mm 的不确定度），直径测量的精度（螺旋测微器可读至0.01 mm，但丝径不均匀可能增加不确定度），以及电压表、电流表读数的随机误差。ρ 的百分不确定度近似等于斜率（来自图像）和面积的百分不确定度之和。面积的百分不确定度是直径百分不确定度的两倍，因为 A ∝ d²。可通过在图像上绘制最差情况直线进行完整的误差传递分析。
9. Common Sources of Error | 常见误差来源
Heating effect: even with low current, the wire may heat up, increasing resistance and causing the R–L graph to deviate from a straight line near long lengths where current is highest if voltage is constant. Contact resistance between crocodile clips and wire can add a constant offset, making the graph not pass through the origin. Zero error in the micrometer or voltmeter/ammeter can introduce systematic errors. Parallax when reading the ruler or analogue meters is also a factor.
热效应：即使电流较小，金属丝也可能升温，导致电阻增大，使 R–L 图在电压恒定时较长段电阻偏高，偏离直线。鳄鱼夹与金属丝之间的接触电阻可能增加一个常量偏移，使图像不通过原点。螺旋测微器或电压/电流表的零误差会引入系统误差。读数时的视差也是一个因素。
10. Improvements and Refinements | 改进与优化
Use a constant current source to eliminate voltage variation. Keep the wire in a water bath to maintain constant temperature. Apply the jockey with a sharp point to minimise contact resistance, or solder connections at fixed lengths. Take multiple diameter measurements along the wire and use the average; reject obvious outliers. Use a digital ohmmeter directly if permitted, but the method of varying length remains essential for gradient analysis. For more accurate length measurement, use a travelling microscope to position the jockey.
使用恒流源以消除电压波动。将金属丝置于水浴中以保持恒温。使用尖头滑动触头以减小接触电阻，或在固定长度处焊接。沿金属丝多次测量直径并取平均值，剔除明显异常值。若允许，可直接使用数字欧姆表，但变长度法对于斜率分析仍必不可少。为更精确地测量长度，可用读数显微镜来定位滑动触头。
11. Extensions and Further Investigation | 拓展与深入探究
Investigate how resistivity changes with temperature by immersing the wire in a hot water bath and measuring resistance at different temperatures. Explore the resistivity of other materials (copper, iron, graphite) and compare. Determine the temperature coefficient of resistance α from the graph of R vs temperature. Alternatively, use a Wheatstone bridge circuit for more precise resistance measurement.
通过将金属丝浸入热水浴中测量不同温度下的电阻，探究电阻率如何随温度变化。研究其他材料（铜、铁、石墨）的电阻率并加以比较。通过 R–T 图确定电阻温度系数 α。也可使用惠斯通电桥进行更精确的电阻测量。
12. Conclusion | 结论
es, precise measurement of diameter, and graphical analysis minimised uncertainties. The investigation demonstrates the practical application of Ohm’s law and provides a solid foundation for understanding material properties and experimental design in AS Physics.
通过控制实验，在误差范围内成功测定了金属丝的电阻率。R 与 L 的线性关系验证了理论模型 ρ = RA/L。细致的变量控制、精确的直径测量和图像分析减小了不确定度。本次探究展示了欧姆定律的实际应用，并为AS物理中理解材料属性和实验设计奠定了坚实基础。
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