Analyzing the Setup
Welcome, future engineer! Today, we are going to peel back the layers of a trigonometric problem that, at first glance, might look like a standard identity exercise.
The equation
2sin2x+5sinx−3=0
is a classic example of a 'wolf in sheep's clothing.' It is a quadratic equation masquerading as trigonometry.
When you see a squared term and a linear term of the same function, your first instinct should always be to simplify. Let us define a new variable, t=sinx.
Suddenly, the complexity vanishes, and we are left with the familiar:
2t2+5t−3=0
The Art of Factorization
Now, we enter the realm of algebra. We need to split the middle term to factorize this quadratic.
We are looking for two numbers that multiply to 2×(−3)=−6 and add to 5. Those numbers are 6 and −1.
So, we rewrite the equation as:
2t2+6t−t−3=0
By grouping terms, we get
2t(t+3)−1(t+3)=0, which leads us to the beautiful factorization:
(2t−1)(t+3)=0
This gives us two potential roots: t=21 and t=−3.
The Reality Check
Here is where many students stumble. We must ask ourselves: does t=−3 make sense?
Since t=sinx, and we know the range of the sine function is strictly [−1,1], the value −3 is impossible. It is a 'ghost root'—a mathematical artifact that has no place in the physical world of angles.
We discard it immediately. We are left with the elegant, singular requirement:
sinx=21
Visualizing the Journey
Now, let us step into the shoes of an observer watching the sine wave oscillate. We are restricted to the interval [0,3π].
Imagine the graph of y=sinx starting at 0, rising to 1 at 2π, falling back to 0 at π, dipping to −1 at 23π, and returning to 0 at 2π. That is one full cycle.
But we are not done! We must continue for another half-cycle, from 2π to 3π.
We draw a horizontal line at y=21. Where does it cut the wave?
In the first cycle [0,2π], the line intersects the curve twice: once in the first quadrant at x=6π and once in the second quadrant at x=π−6π=65π.
Extending the Horizon
But wait, the interval goes up to 3π. Because the sine function is periodic with a period of 2π, we can simply add 2π to our previous solutions to find the intersections in the next cycle.
Thus, x=2π+6π=613π and x=2π+65π=617π.
We check our boundaries: is 617π less than 3π? Since 3π=618π, yes, it is!
We have successfully captured all four solutions:
6π,65π,613π, and 617π
The Final Victory
Counting them up, we find exactly 4 values of x that satisfy the equation.
The beauty of this problem lies not just in the algebra, but in the synthesis of algebraic constraints and geometric visualization. You didn't just solve an equation; you mapped the behavior of a wave across a specific domain.
Keep this mindset—always look for the constraint, always visualize the graph, and never let a 'ghost root' distract you from the truth. You are doing great!