Animated Solution for Mathematics - Differential Equations: Let y=y(x) be the solution of the differential equation, y+12+sinxdxdy=−cosx, y>0, y(0)=1. If y(π)=a and dxdy at x=π is b, then the ordered pair (a,b) is equal to :
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Visualized Solution
Analyze the Differential Equation
Given Differential Equation: y+12+sinxdxdy=−cosx
Initial Condition: y(0)=1
Goal: Find the ordered pair (a,b) where a=y(π) and b=dxdy at x=π
Separating the Variables
Rearrange the equation to separate y and x terms:
y+1dy=−2+sinxcosxdx
Applying Integration
Integrate both sides of the equation:
∫y+1dy=−∫2+sinxcosxdx
Solving the Integrals
Left side integral: ∫y+1dy=ln∣y+1∣
Right side substitution: Let u=2+sinx⟹du=cosxdx
Right side integral: −∫udu=−ln∣2+sinx∣+lnC
The General Solution
Equating both sides: ln∣y+1∣=−ln∣2+sinx∣+lnC
Rearranging: ln∣y+1∣+ln∣2+sinx∣=lnC
Using log properties: ln∣(y+1)(2+sinx)∣=lnC
General Solution: (y+1)(2+sinx)=C
Finding the Constant C
Apply initial condition y(0)=1:
(1+1)(2+sin0)=C
2(2+0)=C⟹C=4
The Particular Solution
Substitute C=4 back into the general solution:
Particular Solution: (y+1)(2+sinx)=4
Finding the Value of a
To find a=y(π), substitute x=π into the particular solution:
(y(π)+1)(2+sinπ)=4
(a+1)(2+sinπ)=4
Calculating a
Since sinπ=0:
(a+1)(2+0)=4
2(a+1)=4⟹a+1=2
a=1
Finding the Derivative b
From the original differential equation, isolate dxdy:
dxdy=−2+sinxcosx(y+1)
We need to evaluate this at x=π and y=a=1.
Calculating b
Substitute x=π and y=1:
b=−2+sinπcosπ(1+1)
b=−2+0(−1)(2)
b=22=1
Final Result
The value of a=1.
The value of b=1.
The ordered pair (a,b) is (1,1).
Correct Option: (4)
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The Sigma Insight: Variable Separable Method
Solution Diagram
Analyzing the Setup
The given differential equation is:
y+12+sinxdxdy=−cosx
We are provided with the initial condition y(0)=1. Our objective is to determine the value a=y(π) and the slope b=dxdyx=π.
The Art of Separation
To solve this, we must isolate the variables x and y. By rearranging the terms, we move all y components to the left and all x components to the right:
y+1dy=−2+sinxcosxdx
This separation transforms the complex relationship into two distinct, integrable parts.
The Integration Dance
We now apply the integral operator to both sides of the equation:
∫y+1dy=−∫2+sinxcosxdx
The left side integrates to ln∣y+1∣. For the right side, we use the substitution u=2+sinx, which implies du=cosxdx.
This substitution yields:
ln∣y+1∣=−ln∣2+sinx∣+lnC
The Particular Path
Using logarithmic properties, we combine the terms:
ln∣y+1∣+ln∣2+sinx∣=lnC
ln∣(y+1)(2+sinx)∣=lnC
Exponentiating both sides gives the general solution:
(y+1)(2+sinx)=C
Applying the initial condition y(0)=1:
(1+1)(2+sin0)=C⇒2(2)=C⇒C=4
Thus, the particular solution is (y+1)(2+sinx)=4.
The Final Reveal
To find a=y(π), we substitute x=π into the particular solution:
(a+1)(2+sinπ)=4
Since sinπ=0, we have 2(a+1)=4, which simplifies to a+1=2, or a=1.
To find the slope b, we rearrange the original differential equation: