To solve the problem of finding the relationship between the forces P and Q given that their resultant is √3Q and is inclined at an angle of 30° to the direction of P, we can use vector addition and some trigonometric principles. Let’s break this down step by step.
Understanding the Forces and Resultant
We have two concurrent forces, P and Q. The resultant R of these two forces can be expressed using the law of cosines, which states:
- R² = P² + Q² + 2PQ cos(θ)
Here, θ is the angle between the two forces. In our case, we know that R = √3Q, so we can substitute that into our equation:
- (√3Q)² = P² + Q² + 2PQ cos(θ)
This simplifies to:
- 3Q² = P² + Q² + 2PQ cos(θ)
Using the Angle Information
We also know that the resultant R is inclined at an angle of 30° to the direction of P. This means we can express the angle θ as follows:
Now, we can find cos(30°):
Substituting this value back into our equation gives:
- 3Q² = P² + Q² + 2PQ(√3/2)
This simplifies to:
Rearranging the Equation
Next, we can rearrange this equation to isolate terms involving P and Q:
Which simplifies to:
Applying the Quadratic Formula
This is a quadratic equation in terms of P. We can apply the quadratic formula, P = (-b ± √(b² - 4ac)) / 2a, where:
Substituting these values into the formula gives:
- P = (−Q√3 ± √((Q√3)² - 4(1)(-2Q²))) / 2(1)
This simplifies to:
- P = (−Q√3 ± √(3Q² + 8Q²)) / 2
Which further simplifies to:
Finding Possible Values for P
Now, we can evaluate the two possible cases for P:
- Case 1: P = (−Q√3 + √(11Q²)) / 2
- Case 2: P = (−Q√3 - √(11Q²)) / 2
However, since forces cannot be negative, we focus on Case 1. For P to be positive, we need:
This leads to:
Squaring both sides gives:
Which simplifies to:
This is always true for Q > 0. Now, we can analyze the two specific cases:
- If P = Q, then substituting gives us a valid solution.
- If P = 2Q, substituting also holds true.
Conclusion
Thus, we have shown that the relationship between the forces P and Q can indeed be either P = Q or P = 2Q, based on the conditions provided. This illustrates the beauty of vector addition and the application of trigonometric principles in solving force-related problems.