Week 7 Β· Parallel coplanar forces: moving one force, parallel forces given as vectors, and practice with resultants and balance points Β· 3 lessons
2
Parallel forces given as i and j vectors: the resultant, and where its line crosses AB by the section formula for like and unlike forces
Applied Mathematics Sec 3 Term 1, Unit 2, Lesson 1, Part 3
GoalFind the resultant of two parallel forces given as vectors, and the point where its line cuts AB, using the section formula.
New words
force as a vector Β· a force written as a pair (a, b) = a i + b j, with i and j the unit vectors along the axessection formula Β· the point C on AB with AC : CB = m : n is (nA + mB) / (m + n)
Explanation
A force can be given by its components: F = (a, b) means a i + b j. Two forces are parallel exactly when one is a multiple of the other, Fβ = k Fβ. If k > 0 they are like forces, if k < 0 they are unlike. Their resultant is R = Fβ + Fβ = (1 + k) Fβ, which is another multiple of Fβ (if k = β1 it is zero: a couple). Where does R act? Let Fβ act at the point A and Fβ at the point B, and let the line of R cut AB at C. The forces are parallel, so the distances of C from their lines are in the same ratio as CA and CB, and the moment balance Fβ Γ (distance) = Fβ Γ (distance) gives CA : CB = |k| : 1. For like forces C is inside AB, nearer the larger force. For unlike forces C is outside AB, beyond the larger force. In both cases one formula works if k keeps its sign: C = (A + kB) / (1 + k), the average of the positions of A and B in which A counts 1 time and B counts k times. Coordinates are added one at a time: x with x, y with y.
Worked examples
In the figure, Fβ = (1, 2) acts at A(β2, 1) and Fβ = (3, 6) at B(6, 5) (forces in newtons). Find the resultant and the point C where its line cuts AB. Since (3, 6) = 3 Γ (1, 2), the forces are parallel and like, with k = 3. R = (1 + 3, 2 + 6) = (4, 8), of size β80 β 8.94 N. Then C = (A + 3B) / 4 = ((β2 + 18) / 4, (1 + 15) / 4) = (4, 4). Check: AC = (6, 3) is three quarters of AB = (8, 4), so AC : CB = 3 : 1, C is nearer the larger force. Moments about C: (β6)(2) β (β3)(1) = β9 for Fβ and (2)(6) β (1)(3) = 9 for Fβ, sum 0. (The moment about C of a force (a, b) at the point (x, y) relative to C is x b β y a.)
Fβ = (2, β1) acts at A(1, 2) and Fβ = (β4, 2) at B(4, 6). Find the resultant and the point where its line cuts the line AB. (β4, 2) = β2 Γ (2, β1), so k = β2: the forces are parallel and unlike. R = (2 β 4, β1 + 2) = (β2, 1). C = (A + kB) / (1 + k) = ((1, 2) β 2(4, 6)) / (β1) = (7, 10). C lies beyond B (B is the midpoint of AC), on the side of the larger force, with CA : CB = 2 : 1. Moments about C: (β6)(β1) β (β8)(2) = 22 for Fβ and (β3)(2) β (β4)(β4) = β22 for Fβ: the sum is 0.
Class activity
On squared paper mark A(0, 0) and B(6, 0). Draw a force of 2 squares upwards at A and a force of 4 squares upwards at B (scale: 1 square for 1 N). Predict where the resultant crosses AB using the formula with k = 2, C = (A + 2B) / 3, then check by cutting a strip of card, balancing it on a pencil with 2 coins at one end and 4 at the other (in the same ratio).
Practice
1
Fβ = (1, β3) acts at A(1, 2) and Fβ = (2, β6) at B(4, 5). Show they are parallel, and find R and the point C where its line cuts AB.
Fβ = 2Fβ, so parallel and like, k = 2. R = (3, β9). C = (A + 2B) / 3 = ((1 + 8) / 3, (2 + 10) / 3) = (3, 4) with AC : CB = 2 : 1.
2
Fβ = (4, 2) acts at A(β1, 3) and Fβ = (β2, β1) at B(5, 6). Find R and where its line cuts the line AB.
Fβ = βΒ½ Fβ, so unlike, k = β1/2. R = (2, 1). C = (A + kB) / (1 + k) = (A β B/2) / (1/2) = 2A β B = (β2 β 5, 6 β 6) = (β7, 0). C lies beyond A, on the side of the larger force Fβ.
3
Are Fβ = (2, 5) and Fβ = (6, 10) parallel? Explain.
No. 6 / 2 = 3 but 10 / 5 = 2: the two ratios differ, so Fβ is not a multiple of Fβ.
4
Fβ = (3, β2) acts at A(β2, 4) and Fβ = (β9, 6) at B(2, 0). Find R and the point where its line cuts AB.
Fβ = β3Fβ, k = β3, unlike. R = (β6, 4). C = (A β 3B) / (1 β 3) = (3B β A) / 2 = ((6 + 2) / 2, (0 β 4) / 2) = (4, β2), beyond B with CA : CB = 3 : 1.
5
What happens to the formula C = (A + kB) / (1 + k) when k = β1, that is when the two forces are equal and opposite?
The denominator is 0, and R = (1 + k)Fβ = 0: there is no resultant and no point C. The two equal opposite forces on different lines make a couple (Unit 3).