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Thread Torque To Force Calculator

Thread Torque To Force Formula:

\[ F = \frac{T}{K \times D} \]

Nm
dimensionless
m

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1. What is the Thread Torque To Force Formula?

The Thread Torque To Force formula calculates the axial force generated from applied torque in threaded fasteners. This relationship is essential in mechanical engineering for determining clamping force in bolted joints and other threaded connections.

2. How Does the Calculator Work?

The calculator uses the formula:

\[ F = \frac{T}{K \times D} \]

Where:

Explanation: The formula converts rotational torque into linear force, accounting for the mechanical advantage provided by the thread geometry and friction characteristics.

3. Importance of Force Calculation

Details: Accurate force calculation is crucial for ensuring proper joint integrity, preventing bolt failure, maintaining seal integrity, and optimizing mechanical designs in various engineering applications.

4. Using the Calculator

Tips: Enter thread torque in Nm, coefficient value (typically 0.2 for standard bolts), and diameter in meters. All values must be positive numbers.

5. Frequently Asked Questions (FAQ)

Q1: What is the typical value for coefficient K?
A: For standard bolts, K is typically around 0.2, but it varies based on thread type, lubrication, and material properties.

Q2: Why is diameter important in this calculation?
A: Diameter determines the lever arm for torque conversion - larger diameters require more torque to achieve the same force.

Q3: Can this formula be used for all thread types?
A: While the basic principle applies, specific thread profiles (metric, unified, acme, etc.) may require adjusted coefficients.

Q4: How does lubrication affect the calculation?
A: Lubrication reduces friction, which decreases the K coefficient, meaning less torque is needed to achieve the same clamping force.

Q5: What are common applications of this calculation?
A: Bolted joint design, automotive assembly, machinery construction, pressure vessel sealing, and structural connections.

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