Step 1: Substitute x=−1 to find the initial value of siny.
Step 2: Differentiate the equation implicitly with respect to x.
Step 3: Substitute x=−1 and siny into the derivative to find dxdy.
Substituting x=−1
Substitute x=−1 into the original equation:
(siny)sin(−2π)+23sec−1(−2)+2−1tan(ln1)=0
Evaluating the Terms
Recall standard values:
sin(−2π)=−1
sec−1(−2)=32π
ln1=0⟹tan(0)=0
Solving for siny
The equation simplifies to:
(siny)−1+23(32π)+0=0
siny1+3π=0
⟹siny=−π3
Differentiating T1: Setup
Let T1=(siny)sin(2πx)
This is of the form uv. We use logarithmic differentiation or the formula:
dxd(uv)=uv[uvdxdu+lnudxdv]
Differentiating T1: Execution
Here, u=siny and v=sin(2πx)
At x=−1: v=−1 and dxdv=2πcos(−2π)=0
dxdu=cosy⋅dxdy
Differentiating T1: Result
Substituting into the formula:
dxdT1=(siny)−1[siny−1(cosydxdy)+ln(siny)⋅0]
dxdT1=−sin2ycosydxdy
Differentiating T2
Let T2=23sec−1(2x)
dxdT2=23⋅∣2x∣(2x)2−12
At x=−1: ∣2(−1)∣=2 and 4(−1)2−1=3
dxdT2=23⋅232=21
Differentiating T3
Let T3=2xtan(ln(x+2))
Use the Product Rule: dxd(f⋅g)=f′g+fg′
dxdT3=(2xln2)tan(ln(x+2))+2xsec2(ln(x+2))⋅x+21
Evaluating dxdT3 at x=−1
Substitute x=−1:
ln(−1+2)=ln1=0
tan(0)=0 (First part vanishes)
sec2(0)=1
dxdT3=0+2−1⋅1⋅11=21
Combining the Derivatives
Sum of all derivatives equals the derivative of 0 (which is 0).
dxdT1+dxdT2+dxdT3=0
−sin2ycosydxdy+21+21=0
−sin2ycosydxdy+1=0
Solving for dxdy
Rearrange the equation to isolate dxdy:
sin2ycosydxdy=1
dxdy=cosysin2y
Final Evaluation
We know siny=−π3
cosy=±1−sin2y=±1−π23=±ππ2−3
dxdy=±ππ2−3(−π3)2=±ππ2−33
*Note: The reference solution states dxdy=0 due to specific problem constraints not fully detailed here, but mathematically, this is the exact value.*
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The Sigma Insight: Techniques of Differentiation
The Anatomy of an Implicit Challenge
Welcome, future engineer. Today, we are going to dismantle a problem that, at first glance, looks like a chaotic mess of transcendental functions. We have an implicit equation:
(siny)sin(2πx)+23sec−1(2x)+2xtan(ln(x+2))=0
Your goal is to find dxdy at x=−1. Take a deep breath; in the world of JEE Advanced, intimidation is the first trap. We will break this down into a sequence of elegant, manageable steps.
Phase 1
The Pre-Game Evaluation
Before we touch the derivative, we need to understand the state of our system at the specific point of interest, x=−1. Implicit differentiation often leaves us with terms involving y that we must evaluate first.
Substituting x=−1 into our equation:
1. The first term becomes (siny)sin(−2π)=(siny)−1.
2. The second term involves sec−1(−2)=32π.
3. The third term involves tan(ln(−1+2))=tan(0)=0, causing the entire term to vanish.
We are left with the simplified relation:
siny1+23⋅32π=0⟹siny=−π3
Keep this value safe; it is our key to the final answer.
Phase 2
The Differentiation Battlefield
Now, we differentiate term by term. Let T1=(siny)sin(2πx). Using the logarithmic differentiation formula dxd(uv)=uv[uvdxdu+ln(u)dxdv], we evaluate at x=−1.
Since the derivative of the exponent v=sin(2πx) involves cos(2πx), which is 0 at x=−1, the expression simplifies significantly. The derivative of T1 at x=−1 becomes:
dxdT1=−sin2ycosydxdy
Next, consider T2=23sec−1(2x). Using the derivative rule dxdsec−1(u)=∣u∣u2−1u′, we get:
dxdT2=23⋅∣2x∣4x2−12
At x=−1, this evaluates to 21. Finally, for T3=2xtan(ln(x+2)), the product rule at x=−1 leaves us with 2−1⋅sec2(0)⋅0+11=21.
Phase 3
The Grand Assembly
We have arrived at the final assembly. The sum of our derivatives must be zero:
−sin2ycosydxdy+21+21=0⟹−sin2ycosydxdy+1=0
Rearranging for the derivative, we find:
dxdy=cosysin2y
Given siny=−π3, we use cosy=±1−sin2y=±1−π23=±ππ2−3. Substituting these into our expression, the final result is:
dxdy=±ππ2−33
You have successfully navigated the complexity and arrived at the truth. This is the essence of mathematics—finding order in the apparent disorder.