Animated Solution for Mathematics - Differential Equations: Let the slope of the tangent to a curve y=f(x) at (x, y) be given by 2tanx(cosx−y). If the curve passes through the point (π/4,0), then the value of ∫0π/2ydx is equal to
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Visualized Solution
Slope of Tangent
Slope of tangent at (x,y) is dxdy
Given: dxdy=2tanx(cosx−y)
Rearranging the Equation
Expand the RHS: dxdy=2tanxcosx−2ytanx
Rearrange: dxdy+(2tanx)y=2sinx
Linear Differential Equation
Standard Form: dxdy+Py=Q
Here, P=2tanx and Q=2sinx
Integrating Factor (I.F.)
Integrating Factor (I.F.) =e∫Pdx
I.F. =e∫2tanxdx=e2ln∣secx∣=sec2x
General Solution Setup
General Solution: y⋅(I.F.)=∫Q⋅(I.F.)dx+C
Substitute values: y⋅sec2x=∫(2sinx)⋅sec2xdx
Solving the Integral
∫2sinxsec2xdx=2∫secxtanxdx
General Solution: ysec2x=2secx+C
Applying Initial Condition
Curve passes through (4π,0)
Substitute x=4π,y=0
0⋅sec2(4π)=2sec(4π)+C
Finding the Constant C
0=22+C⟹C=−22
Equation: ysec2x=2secx−22
Equation of the Curve
Divide by sec2x (or multiply by cos2x)
y=2cosx−22cos2x
Setting up the Definite Integral
Evaluate: I=∫0π/2ydx
I=∫0π/2(2cosx−22cos2x)dx
Integrating the First Part
Split the integral: I=2∫0π/2cosxdx−22∫0π/2cos2xdx
First part: 2[sinx]0π/2=2(sin2π−sin0)=2
Integrating the Second Part
Second part: 22∫0π/2cos2xdx
Using Wallis' formula: ∫0π/2cos2xdx=4π
Value: 22⋅4π=2π
Final Result
Combine parts: I=2−2π
Final Answer: 2−2π
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The Sigma Insight: Linear Differential Equations
Solution Diagram
The Art of Decoding Change
Welcome, future engineers. Today, we are not just solving a differential equation; we are uncovering the hidden geometry of a curve.
When you see a problem like this, where the slope of a tangent is defined by a relationship between x and y, do not panic. You are looking at a dynamic system.
The slope, dxdy, is the language of change. Our goal is to translate this language into a static equation of a curve, y=f(x), and then calculate the area beneath it.
Phase 1
Identifying the Hidden Structure
We start with the given expression:
dxdy=2tanx(cosx−y)
If we distribute the 2tanx, we get:
dxdy=2tanxcosx−2ytanx
Since tanx=cosxsinx, the first term simplifies beautifully: 2tanxcosx=2sinx.
Now, move the y term to the left side:
dxdy+(2tanx)y=2sinx
Suddenly, the fog clears. This is the classic standard form of a Linear Differential Equation: dxdy+P(x)y=Q(x). Identifying this form is the moment you take control of the problem.
Phase 2
The Magic of the Integrating Factor
In a linear differential equation, the Integrating Factor (I.F.) is our secret weapon. It acts as a multiplier that transforms the left side of our equation into the derivative of a product.
We calculate it as I.F.=e∫P(x)dx. Here, P(x)=2tanx.
Integrating this, we get:
∫2tanxdx=2ln∣secx∣
When we raise e to this power, e2ln∣secx∣, the logarithm and the exponential function cancel out, leaving us with sec2x. This is the elegant 'glue' that will hold our solution together.
Phase 3
The General Solution
With our I.F. in hand, the general solution is simply y⋅(I.F.)=∫Q⋅(I.F.)dx+C. Substituting our values, we get:
ysec2x=∫(2sinx)⋅sec2xdx
Do not let this integral intimidate you. Rewrite sec2x as cos2x1.
Then, the integrand becomes:
2sinx⋅cos2x1=2cosxsinx⋅cosx1=2tanxsecx
We know the integral of secxtanx is simply secx. Thus, our equation becomes ysec2x=2secx+C. We have found the family of curves that satisfy the differential condition.
Phase 4
Finding the Specific Path
We are not done yet. The problem gives us a specific point: (4π,0). This is our boundary condition.
By substituting x=4π and y=0, we find:
0=2sec(4π)+C
Since sec(4π)=2, we get 0=22+C, which means C=−22.
Now, we have the specific equation of our curve: ysec2x=2secx−22. Dividing by sec2x (or multiplying by cos2x), we get the explicit form:
y=2cosx−22cos2x
Phase 5
The Final Integration
Finally, we calculate the area:
I=∫0π/2(2cosx−22cos2x)dx
We split this into two parts. The first, ∫0π/22cosxdx, is straightforward: 2[sinx]0π/2=2(1−0)=2.
The second part, −22∫0π/2cos2xdx, is where we use Wallis' formula. The integral of cos2x from 0 to 2π is 4π.
Thus, the second term is:
−22⋅4π=−2π
Combining them, we arrive at our final answer: 2−2π. You have successfully navigated the entire process, from a differential equation to a definite integral. This is the power of calculus—modeling the world, one step at a time.