Animated Solution for Mathematics - Differential Equations: If y=y(x) is the solution curve of the differential equation dxdy+ytanx=xsecx,0≤x≤3π,y(0)=1, then y(6π) is equal to
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Visualized Solution
Identify the Differential Equation
Given equation: dxdy+ytanx=xsecx
Standard form: dxdy+P(x)y=Q(x)
Comparing, we get P(x)=tanx and Q(x)=xsecx
Calculate the Integrating Factor
Integrating Factor formula: I.F.=e∫P(x)dx
Substitute P(x): I.F.=e∫tanxdx
Since ∫tanxdx=ln∣secx∣, I.F.=eln∣secx∣=secx
Formulate the General Solution
General solution formula: y⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C
Substitute values: y⋅secx=∫(xsecx)⋅secxdx+C
Simplify the Integrand
Multiply the terms inside the integral: (xsecx)⋅secx=xsec2x
Simplified equation: ysecx=∫xsec2xdx+C
Integrate using Integration by Parts
Use ILATE rule for ∫xsec2xdx
Let u=x (algebraic) and dv=sec2xdx (trigonometric)
Apply formula ∫udv=uv−∫vdu
Result: xtanx−∫1⋅tanxdx
Complete the Integration
Integrate the remaining term: ∫tanxdx=ln∣secx∣
General solution: ysecx=xtanx−ln∣secx∣+C
Apply Initial Condition
Given initial condition: y(0)=1
Substitute x=0 and y=1 into the general solution
1⋅sec(0)=0⋅tan(0)−ln∣sec(0)∣+C
Since sec(0)=1 and ln(1)=0, we get 1=0−0+C⟹C=1
Write the Particular Solution
Substitute C=1 back into the general solution
Particular solution: ysecx=xtanx−ln∣secx∣+1
Evaluate at x=6π
Substitute x=6π into the particular solution
ysec(6π)=6πtan(6π)−lnsec(6π)+1
Using sec(6π)=32 and tan(6π)=31
y(32)=6π(31)−ln(32)+1
Final Answer
Multiply the entire equation by 23 to isolate y
y=12π−23ln(32)+23
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The Sigma Insight: Linear Differential Equations
Solution Diagram
Analyzing the Setup
The given differential equation is:
dxdy+ytanx=xsecx
This is a first-order linear differential equation of the standard form:
dxdy+P(x)y=Q(x)
Here, we identify P(x)=tanx and Q(x)=xsecx.
The Magic of the Integrating Factor
Our first mission is to find the Integrating Factor (I.F.). We define it as:
I.F.=e∫P(x)dx
Substituting P(x)=tanx, we calculate the integral:
∫tanxdx=ln∣secx∣
Thus, the integrating factor simplifies beautifully:
I.F.=eln∣secx∣=secx
The Dance of Integration by Parts
Multiplying the entire original equation by the I.F.=secx, the left side becomes the derivative of a product, and the right side becomes xsec2x:
dxd(ysecx)=xsec2x
Integrating both sides with respect to x:
ysecx=∫xsec2xdx+C
To solve ∫xsec2xdx, we apply the ILATE rule for integration by parts, setting u=x and dv=sec2xdx:
ysecx=xtanx−∫tanxdx+C
ysecx=xtanx−ln∣secx∣+C
Pinning the Curve
We are given the boundary condition y(0)=1. Substituting x=0 and y=1 into our general solution:
1⋅sec(0)=0⋅tan(0)−ln∣sec(0)∣+C
Since sec(0)=1 and ln(1)=0, the equation simplifies to:
1=0−0+C⇒C=1
The unique curve is defined by:
ysecx=xtanx−ln∣secx∣+1
The Final Reveal
To find y at x=6π, we substitute the value into our specific solution:
ysec(6π)=6πtan(6π)−lnsec(6π)+1
Using the trigonometric values sec(6π)=32 and tan(6π)=31:
y(32)=6π(31)−ln(32)+1
Multiplying by 23 to isolate y, we obtain the final answer: