java file转换muli,如何从绝对文件路径制作CommonsMultipartFile?

博客围绕应用程序API开发展开,在基于GUI浏览器的应用中,文件通过表单提交上传,而API提供文件的绝对路径字符串。为不改变应用底层方法,需将绝对路径文件转换为CommonsMultipartFile对象,文中给出了具体实现步骤和代码示例。

I'm creating an API for my application. In the GUI browser based application the file is uploaded via a form submission. So I simply do CommonsMultipartFile file = request.getFile(myfile). However, the API will provide an absolute path to the file as a string rather than uploading the file. My application will have access to this absolute path.

So that I don't have to change the underlying methods of my application (which accept the common interface MultiPartFile For API purposes, I would like to read the file from this absolute path and create a CommonsMultipartFile object which can be passed around to the methods that I am already using for GUI browser based application.

How can I do this? Constructor to CommonsMultipartFile accepts a FileItem

解决方案

This is API-specific code. i.e. not the usual file upload code.

Usual steps would be to:

construct FileItemFactory

construct ServletFileUpload, passing it the factory

call ServletFileUpload.parseRequest(request)

This answer replaces 2 & 3 with logic independent of servlets - it avoids using ServletFileUpload (servlet-specific) and its ancestor FileUpload (so as to control the file location with an absolute path name). Note: (3) usually examines HTTP request parameters to determine lower-level parameters that are passed to FileItemFactory.createItem - these parameters are instead provided manually, and then only used as informational metadata. Replacement for 2 & 3:

construct FileItem (via FileItemFactory.createItem - need to manually provide lower-level parameters, usually determined via ServletFileUpload.upload())

write to a specific file, with an absolute path

upload the file via MultipartFile

Requested code provided below. At the end it invokes common code - shared with Servlet upload.

// Initialise Apache Commons FileItemFactory for API use only

FileItemFactory fif = new DiskFileItemFactory(sizeThreshold, repositoryBaseDirFile);

// Create Apache Commons FileItem & write file at fullFilePathString into it

FileItem fi = fif.createItem(fieldName, contentType, isFormField, fileName);

fi.write(new java.io.File(new java.net.URI(fullFilePathString));

// Convert FileItem to Spring wrapper: CommonsMultipartFile

org.springframework.web.multipart.MultipartFile mf = new CommonsMultipartFile(fi);

// From here, reuse the same code as the servlet upload. Operate only upon

// Spring MultipartFile, but not ServletFileUpload, FileItemFactory etc...

Parameters:

fullFilePathString: absolute path (as String) where file will be uploaded

fieldName: name of field on the form

(Because ServletFileUpload & FileUpload are avoided, the following become metadata fields only, and are not used to control processing)

sizeThreshhold: memory size threshold in bytes (usually files smaller are uploaded using memory only and files larger are uploaded via disk - but this logic has files always uploaded via disk). Default = DiskFileItemFactory.DEFAULT_SIZE_THRESHOLD.

repositoryBaseDireFile: usually the file upload 'temp' directory (as a File type), but this logic uses an absolute path to upload file

contentType: content type (MIME type) of field on the form (null if not multi-part form field)

isFormField: if plain form field, 'true', else false if multi-part field.

fileName: the name of the file - usually specified via form / client.

### 验证戴维南定理的实现或仿真方法 #### 使用MATLAB验证戴维南定理 可以通过编写MATLAB脚本来模拟电路行为,从而验证戴维南定理。以下是具体的方法: 1. **定义电路参数** 定义电路中的各个元件值,例如电阻、电压源和电流源。这些值可以根据实际实验设定。 2. **计算开路电压 (Uoc)** 开路电压是指当负载断开时,有源二端网络两端的电压。可以利用基尔霍夫定律或其他电路分析方法计算得到[^1]。 3. **计算等效电阻 (Req)** 将所有独立电源置零(理想电压源视为短路,理想电流源视为开路),然后计算此时的等效电阻[^2]。 4. **绘制外部特性曲线** 改变负载电阻的值,记录对应的电流和电压变化情况,并绘制成曲线。 以下是一个简单的MATLAB代码示例用于验证戴维南定理: ```matlab % MATLAB Code to Verify Thevenin's Theorem % Define circuit parameters R1 = 330; % Ohms R2 = 510; % Ohms Rs = 10; % Series resistance with current source, Ohms Is = 10e-3; % Current Source value, Amps Vs = 12; % Voltage Source value, Volts % Step 1: Calculate Open Circuit Voltage (Uoc) Uoc = ((Is * R2) / (R1 + Rs + R2)) - ((Is * Rs) / (R1 + Rs + R2)) + Vs; disp(['Open Circuit Voltage (Uoc): ', num2str(Uoc), ' V']); % Step 2: Calculate Equivalent Resistance (Req) Req = (((R1 + R2) * Rs) / (R1 + R2 + Rs)) + R2; disp(['Equivalent Resistance (Req): ', num2str(Req), ' Ohms']); % Step 3: Simulate Load Behavior and Plot External Characteristics RL_values = linspace(1, 1000, 100); % Range of load resistances from 1 ohm to 1k ohm IL_values = zeros(size(RL_values)); for i = 1:length(RL_values) RL = RL_values(i); IL_values(i) = Uoc / (Req + RL); end figure; plot(RL_values, IL_values, '-b'); xlabel('Load Resistance (\Omega)'); ylabel('Current through Load (A)'); title('External Characteristic Curve'); grid on; ``` --- #### 使用Python与SymPy库验证戴维南定理 除了MATLAB外,还可以使用Python及其科学计算库SymPy来进行符号化推导和数值计算。 ```python from sympy import symbols, Eq, solve # Define symbolic variables R1, R2, Rs, Is, Vs, Req, Uoc, RL = symbols('R1 R2 Rs Is Vs Req Uoc RL') # Assign values to components R1_val = 330 # Ohms R2_val = 510 # Ohms Rs_val = 10 # Ohms Is_val = 10e-3 # Amperes Vs_val = 12 # Volts # Equation for open-circuit voltage (Uoc) eq_Uoc = Eq(Uoc, ((Is*R2)/(R1+Rs+R2)) - ((Is*Rs)/(R1+Rs+R2)) + Vs) # Solve for Uoc solution_Uoc = eq_Uoc.subs({R1: R1_val, R2: R2_val, Rs: Rs_val, Is: Is_val, Vs: Vs_val}) Uoc_value = solve(solution_Uoc, Uoc)[0] print(f"Open-Circuit Voltage (Uoc): {Uoc_value} V") # Equation for equivalent resistance (Req) eq_Req = Eq(Req, ((((R1 + R2)*Rs)/(R1 + R2 + Rs)) + R2)) # Solve for Req solution_Req = eq_Req.subs({R1: R1_val, R2: R2_val, Rs: Rs_val}) Req_value = solve(solution_Req, Req)[0] print(f"Equivalent Resistance (Req): {Req_value} Ω") ``` --- #### 使用SPICE仿真软件验证戴维南定理 SPICE是一种广泛使用的电子电路仿真工具,能够精确地模拟复杂电路的行为。以下是基于LTspice的一个简单流程: 1. 构建原始电路模型,包括所有的电压源、电流源以及电阻。 2. 设置两个测试条件:一是测量开路电压;二是测量短路电流以间接获得等效电阻。 3. 替换原电路为一个单一的电压源和串联电阻组合,再次运行仿真并与之前的测试结果对比。 --- ### 总结 无论是采用编程语言还是专用仿真工具,都可以有效验证戴维南定理的核心概念——即任何线性含源网络都能被简化成一个单电源加串联回路的形式表示出来。
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