{ "cells": [ { "cell_type": "code", "execution_count": 1, "id": "wheatstone-bridge-000", "metadata": { "execution": { "iopub.execute_input": "2026-10-16T00:33:14.961382Z", "iopub.status.busy": "2026-10-16T00:33:14.961227Z", "iopub.status.idle": "2026-10-16T00:33:15.647848Z", "shell.execute_reply": "2026-10-16T00:33:15.647174Z" }, "jupyter": { "source_hidden": true }, "tags": [ "setup" ] }, "outputs": [ { "data": { "text/html": [ "" ], "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "from pathlib import Path\n", "import sys\n", "ROOT=next(p for p in (Path.cwd(),*Path.cwd().parents) if (p/'pyproject.toml').exists())\n", "sys.path.insert(0,str(ROOT/'src'))\n", "import numpy as np\n", "import pandas as pd\n", "import matplotlib.pyplot as plt\n", "from IPython.display import display,Markdown,HTML\n", "from physicslab.common.theme import EXPORT_CSS\n", "from physicslab.common.manuscripts import table_display,metrics_display,display_plotly,series_plot\n", "from physicslab.experiments import wheatstone_bridge as adapter\n", "EXP=ROOT/'experiments/course-03/wheatstone-bridge'\n", "result=adapter.analyze(EXP)\n", "import json\n", "labels=json.loads((EXP/'authoring.json').read_text(encoding='utf-8')).get('metric_labels',{})\n", "for key,value in result['metrics'].items():value.setdefault('label',labels.get(key,key))\n", "display(HTML(EXPORT_CSS))\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-001", "metadata": {}, "source": [ "# 单臂电桥测电阻\n", "\n", "淮南师范学院实验报告\n", "\n", "学院:电子工程学院 专业:物理学 班级:24 物理 1 班\n", "\n", "姓名:缪雨轩 学号:2414050120 实验日期:2025 年 11 月 5 日\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-002", "metadata": {}, "source": [ "## 一、实验名称\n", "\n", "单臂电桥测电阻。\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-003", "metadata": {}, "source": [ "## 二、实验目的\n", "\n", "1. 理解惠斯通电桥比较法测量电阻的原理。\n", "2. 掌握 QJ47 型直流单臂电桥的使用。\n", "3. 计算平衡电阻并依据适用量程和仪器规格分析结果。\n", "\n" ] }, { "attachments": { "bridge.svg": { "image/svg+xml": [ "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" ] } }, "cell_type": "markdown", "id": "wheatstone-bridge-004", "metadata": {}, "source": [ "## 三、实验原理\n", "\n", "四臂为 $R_a,R_b,R_x,R$,电源接 A、C,检流计接 B、D。\n", "\n", "![惠斯通电桥连接关系](attachment:bridge.svg)\n", "\n", "\n", "\n", "图 1 惠斯通电桥节点与四臂连接示意\n", "\n", "\n", "\n", "平衡时 $V_B=V_D$、检流计电流为零,左右支路电流分别为 $I_1,I_2$,有\n", "\n", "$$\n", "I_1R_a=I_2R_x,\\qquad I_1R_b=I_2R.\n", "$$\n", "\n", "消去电流:\n", "\n", "$$\n", "\\frac{R_a}{R_b}=\\frac{R_x}{R},\\qquad M=\\frac{R_a}{R_b},\\qquad R_x=MR.\n", "$$\n", "\n", "不平衡时,在开路检流端、理想电源模型下\n", "\n", "$$\n", "\\frac{V_B-V_D}{E}=\\frac{R_b}{R_a+R_b}-\\frac{R}{R_x+R}.\n", "$$\n", "\n", "该电压可解释调节比较臂寻找零点的过程,实际检流计加载会改变不平衡电压,平衡条件保持不变。\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-005", "metadata": {}, "source": [ "#### 平衡附近的桥电压灵敏度\n", "\n", "令比较臂 $R=1$、比率臂 $R_b=1,R_a=M$(归一化模型),扫描 $R_x/(MR)$。默认 $M=1$;不把归一化阻值当成本次实际桥臂内阻。" ] }, { "cell_type": "code", "execution_count": 2, "id": "wheatstone-bridge-006", "metadata": { "execution": { "iopub.execute_input": "2026-10-16T00:33:15.649587Z", "iopub.status.busy": "2026-10-16T00:33:15.649338Z", "iopub.status.idle": "2026-10-16T00:33:15.914171Z", "shell.execute_reply": "2026-10-16T00:33:15.913294Z" }, "jupyter": { "source_hidden": true } }, "outputs": [ { "data": { "text/html": [ "
\n", "
" ], "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "import physicslab.common.manuscripts as _presentation\n", "_presentation._table_captioned=False\n", "display_plotly(adapter.explore(\"balance\",result))" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-007", "metadata": {}, "source": [ "图 2 理想开路桥电压与比率臂灵敏度" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-008", "metadata": {}, "source": [ "## 四、主要仪器设备\n", "\n", "QJ47 型直流单双臂电桥、五个待测电阻(标称 $3,47,200,2000,20000\\,\\Omega$)及导线。仪器总体标称 0.05 级,但说明书按测量区间另有等级条件,不可对所有结果统一应用。\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-009", "metadata": {}, "source": [ "## 五、实验步骤\n", "\n", "1. 熟悉比率盘、比较臂十进盘、粗调/细调、电源和指零仪开关。\n", "2. 指零仪内接并调零,按估计阻值选比率 $M$,尽量使用比较臂高位。\n", "3. 待测电阻接入,先粗调再细调,从高位到低位寻找平衡。\n", "4. 松开按钮后读取 $M$ 和比较臂总示值 $R$,计算 $R_x=MR$。\n", "5. 更换电阻重复,核查说明书有效范围、基准值及环境条件后再评价允许误差。\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-010", "metadata": {}, "source": [ "## 六、原始数据记录\n", "\n", "\n", "\n", "表 1 比率设定、比较臂与源处理结果\n", "\n", "\n", "\n", "| 标称 / Ω | 比率设定 | 比较臂 / Ω | 源处理结果 / Ω |\n", "| --- | --- | --- | --- |\n", "| 3 | 0.1 | 30.66 | 3.066 |\n", "| 47 | 0.1 | 465.94 | 46.594 |\n", "| 200 | 100/100 | 200.2 | 200.2 |\n", "| 2000 | 10 | 197.97 | 1979.7 |\n", "| 20000 | 100 | 204.21 | 20421 |\n", "\n", "$100/100$ 是比率盘设定标识,实际乘数为 1;没有将其作为两次独立读数。\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-011", "metadata": {}, "source": [ "## 七、数据处理\n", "\n", "### 1. 平衡值及标称比较\n", "\n", "$$\n", "D=\\frac{R_x-R_{\\mathrm{nom}}}{R_{\\mathrm{nom}}}\\times100\\%.\n", "$$\n", "\n", "\n", "\n", "表 2 平衡电阻复算及量程条件\n", "\n", "\n", "\n", "| 标称 / Ω | $M$ | 重算电阻 / Ω | 标称偏差 / % | 说明书等级条件 |\n", "| --- | --- | --- | --- | --- |\n", "| 3 | 0.1 | 3.066 | 2.2 | <10 Ω,超单桥有效范围 |\n", "| 47 | 0.1 | 46.594 | -0.86383 | $0.05\\%$(参考条件下) |\n", "| 200 | 1 | 200.2 | 0.1 | $0.05\\%$(参考条件下) |\n", "| 2000 | 10 | 1979.7 | -1.015 | $0.05\\%$(参考条件下) |\n", "| 20000 | 100 | 20421 | 2.105 | $0.1\\%$(参考条件下) |\n", "\n", "标称偏差只比较标称与读数,不等于仪器校准误差。\n", "\n", "### 2. 允许误差与适用性\n", "\n", "说明书单电桥有效范围下限为 $10\\,\\Omega$;$10$–$10^4\\,\\Omega$ 的等级指数为 $0.05\\%$,$10^4$–$10^5\\,\\Omega$ 为 $0.1\\%$,更高区间另有规定,参考温度为 $20\\pm2\\,^{\\circ}\\mathrm C$。\n", "\n", "其允许误差表达采用\n", "\n", "$$\n", "E_{\\mathrm{lim}}=\\pm c\\left(\\frac{R_N}{10}+X\\right),\n", "$$\n", "\n", "$c$ 为等级指数的无量纲数值,$R_N$ 为基准,$X$ 在说明书中定义为标度盘示值。源示例将 $c=0.0005,R_N=100,X=3.066$ 代入得 $0.006533\\,\\Omega$,算术可复算,但不能据此确认 $3\\,\\Omega$ 结果适用该单桥规格。\n", "\n", "\n", "\n", "表 3 源报告给出的限差表达(适用条件待核,非新认定结果)\n", "\n", "\n", "\n", "| 标称 / Ω | 源报告限差表达(待核适用条件) |\n", "| --- | --- |\n", "| 3 | $(3.066\\pm0.007)\\,\\Omega$ |\n", "| 47 | $(46.59\\pm0.03)\\,\\Omega$ |\n", "| 200 | $(200.2\\pm0.2)\\,\\Omega$ |\n", "| 2000 | $(1980\\pm2)\\,\\Omega$ |\n", "| 20000 | $(20420\\pm30)\\,\\Omega$ |\n", "\n", "本次各档基准和温度条件未完整记录,且 $3\\,\\Omega$ 在有效范围以下,故不将这些允许误差极限改称标准不确定度。若未来确认半宽为 $a$ 的均匀误差模型,才可据模型取 $u_B=a/\\sqrt3$ 并与其他分量合成。\n", "\n" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-012", "metadata": {}, "source": [ "#### 平衡结果与规格分开核验\n", "\n", "复算全部乘积,检查3Ω的量程边界和20kΩ等级区间。限差条件不足时不输出伪确定的不确定度。" ] }, { "cell_type": "code", "execution_count": 3, "id": "wheatstone-bridge-013", "metadata": { "execution": { "iopub.execute_input": "2026-10-16T00:33:15.957473Z", "iopub.status.busy": "2026-10-16T00:33:15.957246Z", "iopub.status.idle": "2026-10-16T00:33:15.961685Z", "shell.execute_reply": "2026-10-16T00:33:15.960901Z" }, "jupyter": { "source_hidden": true } }, "outputs": [ { "data": { "text/markdown": [ "表 计算结果\n", "\n", "| 标称 / Ω | $M$ | 重算电阻 / Ω | 标称偏差 / % | 说明书等级条件 |\n", "| --- | --- | --- | --- | --- |\n", "| 3 | 0.1 | 3.066 | 2.2 | <10 Ω,超单桥有效范围 |\n", "| 47 | 0.1 | 46.594 | -0.86383 | $0.05\\%$(参考条件下) |\n", "| 200 | 1 | 200.2 | 0.1 | $0.05\\%$(参考条件下) |\n", "| 2000 | 10 | 1979.7 | -1.015 | $0.05\\%$(参考条件下) |\n", "| 20000 | 100 | 20421 | 2.105 | $0.1\\%$(参考条件下) |" ], "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "import physicslab.common.manuscripts as _presentation\n", "_presentation._table_captioned=False\n", "table_display(result[\"tables\"][\"results\"])" ] }, { "cell_type": "markdown", "id": "wheatstone-bridge-014", "metadata": {}, "source": [ "## 八、实验结果与讨论\n", "\n", "1. 五个平衡结果为 $3.066,46.594,200.20,1979.7,20421\\,\\Omega$,由实际比率和比较臂示值计算,保留未修约值用于复算。\n", "2. $3\\,\\Omega$ 低于说明书单桥有效范围下限,比较臂 $30.66\\,\\Omega$ 也未充分使用建议高位,不能按标称 0.05 级保证其准确度;低阻宜选择适用量程或四端测量。\n", "3. $20\\,\\mathrm{k}\\Omega$ 属于 $0.1\\%$ 等级区间,不可统一套用 $0.05\\%$。各档基准、环境条件及重复性缺失,未给出已经核定的完整不确定度。\n", "4. 比较法减少了对电源幅度和检流计绝对标定的依赖,但仍受比较臂、比率臂、接触和零点灵敏度影响。按平衡公式计算本身不构成对该公式的独立实验验证。\n" ] } ], "metadata": { "kernelspec": { "display_name": "Python 3", "language": "python", "name": "python3" }, "language_info": { "codemirror_mode": { "name": "ipython", "version": 3 }, "file_extension": ".py", "mimetype": "text/x-python", "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython3", "version": "3.14.7" }, "physicslab": { "chinese_font": "SimSun", "experiment_id": "course-03/wheatstone-bridge", "latin_font": "Times New Roman" } }, "nbformat": 4, "nbformat_minor": 5 }