Problem 53
Question
Equilibrium of Forces The forces \(\mathbf{F}_{1}, \mathbf{F}_{2}, \ldots, \mathbf{F}_{n}\) acting at the same point \(P\) are said to be in equilibrium if the resultant force is zero, that is, if \(\mathbf{F}_{1}+\mathbf{F}_{2}+\cdots+\mathbf{F}_{n}=0 .\) Find (a) the resultant forces acting at \(P,\) and (b) the additional force required (if any) for the forces to be in equilibrium. $$ \begin{array}{l}{\mathbf{F}_{1}=4 \mathbf{i}-\mathbf{j}, \quad \mathbf{F}_{2}=3 \mathbf{i}-7 \mathbf{j}, \quad \mathbf{F}_{3}=-8 \mathbf{i}+3 \mathbf{j}} \\ {\mathbf{F}_{4}=\mathbf{i}+\mathbf{j}}\end{array} $$
Step-by-Step Solution
Verified Answer
Resultant force is \(-4\mathbf{j}\). Additional force needed is \(4\mathbf{j}\).
1Step 1: Calculate the Resultant Force
To find the resultant force, we sum up all the given forces: \( \mathbf{F}_{R} = \mathbf{F}_{1} + \mathbf{F}_{2} + \mathbf{F}_{3} + \mathbf{F}_{4} \). \[ \mathbf{F}_{R} = (4\mathbf{i} - \mathbf{j}) + (3\mathbf{i} - 7\mathbf{j}) + (-8\mathbf{i} + 3\mathbf{j}) + (\mathbf{i} + \mathbf{j}) \]Combine like terms:\[ \mathbf{F}_{R} = (4 + 3 - 8 + 1)\mathbf{i} + (-1 - 7 + 3 + 1)\mathbf{j} \]Simplify:\[ \mathbf{F}_{R} = 0\mathbf{i} - 4\mathbf{j} \]Thus, the resultant force is \( \mathbf{F}_{R} = -4\mathbf{j} \).
2Step 2: Determine the Additional Force Required for Equilibrium
For the forces to be in equilibrium, the resultant force must be zero. Currently, \( \mathbf{F}_{R} = -4\mathbf{j} \). We need an additional force \( \mathbf{F}_{A} \) such that:\[ \mathbf{F}_{R} + \mathbf{F}_{A} = 0 \]This means:\[ -4\mathbf{j} + \mathbf{F}_{A} = 0 \]Thus, \( \mathbf{F}_{A} = 4\mathbf{j} \).The additional force required to achieve equilibrium is \( 4\mathbf{j} \).
Key Concepts
Resultant ForceVector AdditionForce EquilibriumAdditional Force
Resultant Force
The resultant force is like the sum of all individual forces acting at a specific point. Imagine you have several people pushing a sled from different directions; the resultant force tells you which way the sled will move if all these forces are combined. In our exercise, we calculated the resultant force at point \( P \) by adding up the given forces \( \mathbf{F}_{1}, \mathbf{F}_{2}, \mathbf{F}_{3}, \) and \( \mathbf{F}_{4} \). By combining their components in the \( \mathbf{i} \) and \( \mathbf{j} \) directions, we found that the resultant force is \( \mathbf{F}_{R} = -4\mathbf{j} \). In simpler terms, this resultant force means there is a net force acting downwards (negative \( \mathbf{j} \)-direction) once all forces have been accounted for.
Vector Addition
Vector addition is a method used to combine multiple force vectors to find the resultant or total force. Vectors have both magnitude and direction, and just like arrows, they can be broken down into components (like \( \mathbf{i} \) for horizontal and \( \mathbf{j} \) for vertical movement).
To add vectors, align them by their components, summing up all like terms in each direction.
To add vectors, align them by their components, summing up all like terms in each direction.
- Combine all \( \mathbf{i} \)-components together.
- Combine all \( \mathbf{j} \)-components together.
Force Equilibrium
Force equilibrium occurs when all forces acting on an object are perfectly balanced, resulting in no movement. At this point, the resultant force equals zero. In the exercise, we noticed the forces were not in equilibrium since the resultant was \( -4\mathbf{j} \). In practical terms, one can imagine a perfectly balanced see-saw - it won't tip over as long as weights on both sides are evenly distributed.
When forces are balanced, it means:
When forces are balanced, it means:
- The sum of all force vectors equals zero.
- There is no net motion in any direction.
Additional Force
An additional force is a force needed to bring the system back into force equilibrium. This is often necessary when the calculated resultant force is not zero, indicating that some directional force remains. In our exercise, the existing forces left an unbalanced \( -4\mathbf{j} \) (downwards).
To counter this, we needed an additional upwards force of \( 4\mathbf{j} \) to achieve balance. By adding \( 4\mathbf{j} \) to the resultant, we bring the system to equilibrium:
To counter this, we needed an additional upwards force of \( 4\mathbf{j} \) to achieve balance. By adding \( 4\mathbf{j} \) to the resultant, we bring the system to equilibrium:
- The net force becomes zero.
- The object stops moving or stays at rest.
Other exercises in this chapter
Problem 52
\(49-56\) me product \(z_{1} z_{2}\) and the quotient \(z_{1} / z_{2}\) . Express your answer in polar form. $$ z_{1}=7\left(\cos \frac{9 \pi}{8}+i \sin \frac{9
View solution Problem 52
(a) Graph the polar equation \(r=\tan \theta \sec \theta\) in the viewing rectangle \([-3,3]\) by \([-1,9] .\) (b) Note that your graph in part (a) looks like a
View solution Problem 53
Convert the polar equation to rectangular coordinates. $$ r=\frac{1}{\sin \theta-\cos \theta} $$
View solution Problem 53
\(49-56\) me product \(z_{1} z_{2}\) and the quotient \(z_{1} / z_{2}\) . Express your answer in polar form. $$ \begin{array}{l}{z_{1}=4\left(\cos 120^{\circ}+i
View solution