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Rectangular Components of a Force in 2D

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H4M Team
H4M Team

“Write a force by its x and y components, in scalar and Cartesian vector form, and get its magnitude and direction back.”

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Resolving a force along two perpendicular axes, \(x\) and \(y\), gives its rectangular components. They turn vector addition into ordinary addition of numbers, which is why almost every statics problem uses them.

1. Rectangular components

Rectangular components of a force
Rectangular components of a force

On perpendicular axes, the parallelogram of the components becomes a rectangle (Figure 1). If \(\theta\) is the angle between \(\mathbf{F}\) and the \(x\) axis, the components follow from the right triangle:

 
$$ F_x = F\cos\theta, \qquad F_y = F\sin\theta $$

The axes do not have to be horizontal and vertical. On an incline, axes along and across the slope often make the components simpler; Equation 1 still holds with \(\theta\) measured from the new \(x\) axis.

2. Signs of the components

In scalar notation, \(F_x\) and \(F_y\) are numbers with signs: positive when the component points along \(+x\) or \(+y\), negative otherwise. The same force turned into each of the four quadrants gives four sign pairs (Figure 2).

Signs of the components in the four quadrants
Signs of the components in the four quadrants
 

Use the acute angle. Take the acute angle between the force and the nearest axis, compute the magnitudes of the components with sine and cosine, and give each one its sign from the sketch. This is safer than working with angles over 90°.

3. Cartesian vector notation

The unit vectors \(\mathbf{i}\) and \(\mathbf{j}\) have magnitude 1, no unit, and point along \(+x\) and \(+y\). Any force in the plane can be written with them:

 
$$ \mathbf{F} = F_x\,\mathbf{i} + F_y\,\mathbf{j} $$

The signs of the components go into the expression. A force of 200 N directed 30° below the \(-x\) axis is \(\mathbf{F} = \{-173\,\mathbf{i} - 100\,\mathbf{j}\}\,\text{N}\). Scalar and Cartesian notation carry the same information; the Cartesian form is the one that extends to three dimensions.

4. Components from a slope

Components of a 260 N force from a 5-12-13 slope triangle
Components of a 260 N force from a 5-12-13 slope triangle

Drawings often give a direction as a small slope triangle, or as the coordinates of two points, instead of an angle. The components are then in the same ratio as the sides of the triangle:

 
$$ F_x = F\,\frac{\Delta x}{L}, \qquad F_y = F\,\frac{\Delta y}{L}, \qquad L = \sqrt{\Delta x^2 + \Delta y^2} $$

For a 260 N force along a 5-12-13 slope (Figure 3), \(F_x = 260 \cdot 12/13 = 240\,\text{N}\) and \(F_y = 260 \cdot 5/13 = 100\,\text{N}\). No angle is needed.

5. Back from components to the force

When the components are known, the magnitude and the direction are:

 
$$ F = \sqrt{F_x^2 + F_y^2}, \qquad \theta = \tan^{-1}\left|\frac{F_y}{F_x}\right| $$

Equation 4 gives the acute angle from the \(x\) axis; the signs of \(F_x\) and \(F_y\) tell the quadrant.

 

Check the quadrant. A calculator's \(\tan^{-1}\) returns angles between \(-90^\circ\) and \(90^\circ\) only. For \(F_x = -40\,\text{N}\) and \(F_y = 30\,\text{N}\), \(F = 50\,\text{N}\) and the acute angle is \(36.9^\circ\), but the force points up and to the left: \(36.9^\circ\) above the \(-x\) axis, or \(143.1^\circ\) from \(+x\).

Summary

  • Rectangular components: \(F_x = F\cos\theta\), \(F_y = F\sin\theta\), with \(\theta\) from the \(x\) axis.
  • Components carry signs; take magnitudes from the acute angle and signs from the sketch.
  • Cartesian form: \(\mathbf{F} = F_x\mathbf{i} + F_y\mathbf{j}\).
  • With a slope triangle, the components are in the ratio of its sides.
  • \(F = \sqrt{F_x^2 + F_y^2}\); always check the quadrant of the angle.

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