Finding the magnitude and angle of the resultant force vector

 
 
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Steps for finding the magnitude and angle of a resultant force

When we’re given two vectors with the same initial point, and they’re different lengths and pointing in different directions, we can think about each of them as a force. The longer the vector, the more force it pulls in its direction.

Oftentimes we want to be able to find the net force of the two vectors, which will be a third vector that counterbalances the force and direction of the other two. Think about the resultant vector as representing the amount of force and the direction in which you’d have to pull to cancel out the force from the other two vectors.

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In order to define this third vector, we need to find

its magnitude (its length), which will be force, in Newtons N, and

its angle, from the positive direction of the xx-axis.

To find the magnitude and angle of a resultant force, we

create vector equations for each of the given forces

add the vector equations together to get the vector equation of the resultant force

find magnitude of the resultant force using the new vector equation and the distance formula

D=(x2x1)2+(y2y1)2D=\sqrt{\left(x_2-x_1\right)^2+\left(y_2-y_1\right)^2}

find the angle of the resultant force using the new vector equation and the formula 

θR=180arctanyx\theta_R=180^\circ-\arctan{\frac{|y|}{|x|}}

 
 

Finding the magnitude and angle of a resultant force vector from two force vectors


 
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Force vectors in the first and second quadrants

Example

Find the magnitude and angle of the resultant force.

resultant force of two force vectors

We’ll use the forces and the angles to find vector equations for F1F_1 and F2F_2.

F1=150cos75 i+150sin75 jF_1=150\cos{75^\circ}\ \bold i+150\sin{75^\circ}\ \bold j

F1=38.82 i+144.89 jF_1=38.82\ \bold i+144.89\ \bold j

F1=38.82, 144.89F_1=\langle38.82,\ 144.89\rangle

and

F2=200cos15 i+200sin15 jF_2=-200\cos{15^\circ}\ \bold i+200\sin{15^\circ}\ \bold j

F2=193.19 i+51.76 jF_2=-193.19\ \bold i+51.76\ \bold j

F2=193.19, 51.76F_2=\langle-193.19,\ 51.76\rangle

Magnitude and angle of the resultant force

The longer the vector, the more force it pulls in its direction.

We’ll add our forces together to find the vector equation of the resultant force.

FR=F1+F2F_R=F_1+F_2

FR=38.82 i+144.89 j193.19 i+51.76 jF_R=38.82\ \bold i+144.89\ \bold j-193.19\ \bold i+51.76\ \bold j

FR=154.37 i+196.65 jF_R=-154.37\ \bold i+196.65\ \bold j

FR=154.37, 196.65F_R=\langle-154.37,\ 196.65\rangle

Now we can plug the vector equation into the distance formula to find the length of the resultant force vector. Because both F1F_1 and F2F_2 have their initial point at the origin, (x1, y1)(x_1,\ y_1) will be (0,0)(0,0).

DR=(x20)2+(y20)2D_R=\sqrt{\left(x_2-0\right)^2+\left(y_2-0\right)^2}

DR=(154.370)2+(196.650)2D_R=\sqrt{(-154.37-0)^2+(196.65-0)^2}

DR=23,830.10+38,671.22D_R=\sqrt{23,830.10+38,671.22}

DR=250.00D_R=250.00

To find the angle of the resultant force, we’ll use the formula

θR=180arctanyx\theta_R=180^\circ-\arctan{\frac{|y|}{|x|}}

where FR=x,yF_R=\langle{x},y\rangle. Plugging in xx and yy from the resultant force, we get

θR=180arctan196.65154.37\theta_R=180^\circ-\arctan{\frac{196.65}{154.37}}

θR=18051.73\theta_R=180^\circ-51.73^\circ

θR=128.27\theta_R=128.27^\circ

The magnitude of the resultant force is 250250 N and the angle of the resultant force is 128.27128.27^\circ.

resultant force vector

Notice how we built the vector equations for F1F_1 and F2F_2 in this last example. 

When we measure the angle of the vector, we always measure it from the horizontal axis, which means we’ll measure the angles of vectors in the first and fourth quadrants from the positive direction of the horizontal axis, but measure the angles of vectors in the second and third quadrants from the negative direction of the horizontal axis.

Because F1F_1 fell in the first quadrant, we measured its angle from the positive horizontal axis as 7575^\circ. But F2F_2 fell in the second quadrant, which means we measured its angle from the negative direction of the horizontal axis as 1515^\circ.

And we’ll always treat the angle between the vector and the horizontal axis as a positive angle. So even for vectors in the third and fourth quadrants, we’ll still measure a positive angle from the horizontal axis.

So, while we always keep the angles positive, we do need to change the signs of the coefficients on i\bold i and j\bold j, depending on the quadrant of the vector. Consider a generic vector,

FV=FVxcosθ i+FVysinθ jF_V=F_{V_x}\cos{\theta}\ \bold i+F_{V_y}\sin{\theta}\ \bold j

The signs we use for FVxF_{V_x} and FVyF_{V_y} depend on the quadrant.

In the first quadrant, FVxF_{V_x} is positive, and FVyF_{V_y} is positive

In the second quadrant, FVxF_{V_x} is negative, and FVyF_{V_y} is positive

In the third quadrant, FVxF_{V_x} is negative, and FVyF_{V_y} is negative

In the fourth quadrant, FVxF_{V_x} is positive, and FVyF_{V_y} is negative

That’s why, in the previous example, F1F_1 in the first quadrant got two positive signs, F1=150cos75 i+150sin75 jF_1=150\cos{75^\circ}\ \bold i+150\sin{75^\circ}\ \bold j, and F2F_2 in the second quadrant got a negative sign on the first term and a positive sign on the second term, F2=200cos15 i+200sin15 jF_2=-200\cos{15^\circ}\ \bold i+200\sin{15^\circ}\ \bold j.

 
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