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If \(y(x)\) satisfies the differential equation \(y^{\prime}-y \tan x=2 x \sec x\) and \(y(0)=0\), then (A) \(y\left(\frac{\pi}{4}\right)=\frac{\pi^{2}}{8 \sqrt{2}}\) (B) \(y^{\prime}\left(\frac{\pi}{4}\right)=\frac{\pi^{2}}{18}\) (C) \(y\left(\frac{\pi}{3}\right)=\frac{\pi^{2}}{9}\) (D) \(y^{\prime}\left(\frac{\pi}{3}\right)=\frac{4 \pi}{3}+\frac{2 \pi^{2}}{3 \sqrt{3}}\)

Short Answer

Expert verified
The correct answer is (A) \(y\left(\frac{\pi}{4}\right)=\frac{\pi^2}{8\sqrt{2}}\).

Step by step solution

01

Identify the Differential Equation

Recognize that the given differential equation is a first-order linear differential equation in the form \(y^\prime - y \tan x = 2x \sec x\).
02

Find the Integrating Factor

To solve a linear first-order differential equation, use an integrating factor \(\mu(x)\) which is given by \(\mu(x) = e^{\int P(x)\,dx}\), where \(P(x)\) is the coefficient of \(y\) in the differential equation. Here, \(P(x) = -\tan x\), so \(\mu(x) = e^{-\int \tan x\,dx} = e^{-\ln|\cos x|} = \frac{1}{\cos x} = \sec x\).
03

Multiply Throughout by the Integrating Factor

Multiply the entire differential equation by the integrating factor \(\sec x\) to obtain \(\sec x y^\prime - y \sec x \tan x = 2x\).
04

Recognize the Left Side as a Derivative

Observe that the left-hand side of the equation from Step 3 is the derivative of the product of the integrating factor \(\sec x\) and \(y\). Therefore, \(\sec x y^\prime - y \sec x \tan x = (\sec x y)^\prime\).
05

Integrate Both Sides of the Equation

Integrate both sides with respect to \(x\) to find \(\sec x y = \int 2x\,dx = x^2 + C\), where \(C\) is the constant of integration.
06

Solve for y

Divide by \(\sec x\) to solve for \(y(x)\): \((y \sec x)\prime = (x^2 + C)\) gives us \((y = x^2 \cos x + C \cos x)\).
07

Apply the Initial Condition

Use the initial condition \(y(0) = 0\) to find \(C\). Plugging these values into the solution gives us \(0 = 0 + C \cos(0)\), which implies that \(C = 0\). Therefore the solution is \(y = x^2 \cos x\).
08

Evaluate y at Specific Points

Now we need to evaluate \(y\) for the given points \(x =\frac{\pi}{4}\) and \(x=\frac{\pi}{3}\) to see which options are correct.
09

Check Option (A)

Evaluating \(y\left(\frac{\pi}{4}\right) = \left(\frac{\pi}{4}\right)^2 \cos\left(\frac{\pi}{4}\right) = \frac{\pi^2}{16} \cdot \frac{\sqrt{2}}{2} = \frac{\pi^2}{16} \cdot \frac{8}{16 \sqrt{2}} = \frac{\pi^2}{8\sqrt{2}}\), which matches Option (A).
10

Differentiate y to Find y'

Differentiate \(y = x^2 \cos x\) with respect to \(x\) using the product rule to find \(y'\).
11

Evaluate y' at Specific Points

Specifically, find \(y'\left(\frac{\pi}{4}\right)\) and \(y'\left(\frac{\pi}{3}\right)\) to compare with Options (B) and (D).
12

Check Remaining Options

After computing \(y'\), plug in the specific values of \(x\) and match the results with the given options.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Integrating Factor Method
The integrating factor method is an essential tool for solving first-order linear differential equations. When a differential equation is given in the standard form \( y' + P(x)y = Q(x) \), the integrating factor \( \boldsymbol{\frac{1}{2}}\mu(x) \) will transform it into an exact equation that can be integrated directly. The integrating factor is defined as \( \boldsymbol{\frac{1}{2}}\mu(x) = e^{\boldsymbol{\frac{1}{2}}\int P(x)dx} \).To apply this method effectively:
  • First, identify the function \( P(x) \) and calculate the integrating factor.
  • Next, multiply the entire differential equation by \( \boldsymbol{\frac{1}{2}}\mu(x) \) to produce a product that can be recognized as the derivative of two functions.
  • The left-hand side simplifies into a form that can be integrated with respect to \( x \).
  • Finally, solve for \( y(x) \) and apply any initial conditions to determine the particular solution of the differential equation.
By using this process, complex differential equations can be solved systematically, providing clear steps towards the solution.
Initial Value Problem
An initial value problem (IVP) is a differential equation accompanied by a specified value, called the initial condition, which the solution must satisfy when \( x \) is at a particular point. In our exercise, the IVP is defined by the equation \( y^\boldsymbol{\frac{1}{2}} - y \tan x = 2x \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac('\), it is crucial to first determine the initial value of the function. In this case, the initial condition is \( y(0) = 0 \). Solving the IVP involves finding a function \( y(x) \) that satisfies both the differential equation and the initial condition. This often results in the introduction of a constant \( C \) after integration, which is then determined by plugging the initial condition into the general solution.
Differential Equation Solution
The solution to a differential equation represents a function or a family of functions that satisfy the equation. For first-order linear differential equations, the solution generally involves an arbitrary constant, which can be determined through initial conditions. In this context, after applying the integrating factor method, the differential equation is simplified to a point where it can be integrated to reveal the general solution.To form the complete solution, the process typically follows these steps:
  • Integrating the modified equation after applying the integrating factor.
  • Expressing the result in terms of \( y(x) \).
  • Applying any given initial condition to resolve the constant of integration.
In the given exercise, the use of the initial condition \( y(0) = 0 \) led directly to the specific solution \( y = x^2 \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{1}{2}} \boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac{\boldsymbol{\frac{\frac{\frac('\). This solution satisfies both the equation and the initial value, proving it to be the correct solution.
Product Rule Differentiation
The product rule in differentiation is a crucial technique when dealing with products of functions. It states that if \( u(x) \) and \( v(x) \) are differentiable functions of \( x \), then the derivative of their product \( uv \) is given by \( \boldsymbol{\frac{1}{2}}\frac{d}{dx}(uv) = u\boldsymbol{\frac{1}{2}}\boldsymbol{\frac{1}{2}}\boldsymbol{\frac{1}{2}}\boldsymbol{\frac{1}{2}}\boldsymbol{\frac( v(x) + v\boldsymbol{\frac( u(x) \). The product rule is essential in finding the derivative of a product without having to expand the product first.For example, when differentiating the function \( y = x^2 \boldsymbol{\frac{1}{2}} \boldsymbol{\frac( x \), the product rule helps us find \( y' \) efficiently:
  • Take \( u(x) = x^2 \) and \( v(x) = \boldsymbol{\frac( x \) as the two parts of the product.
  • Apply the product rule to find \( y' = u'v + uv' \).
  • Substitute the derivatives \( u' = 2x \) and \( v' = -\boldsymbol{\frac( x \) into the formula.
This produces the derivative of the function \( y \), which is needed to solve the differential equation or evaluate the function at specific points, as seen in the provided exercise.

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Most popular questions from this chapter

Young's double slit experiment is carried out by using green, red and blue light, one color at a time. The fringe widths recorded are \(\beta_{G}, \beta_{R}\) and \(\beta_{B}\), respectively. Then, (A) \(\beta_{G}>\beta_{B}>\beta_{R}\) (B) \(\beta_{B}>\beta_{G}>\beta_{R}\) (C) \(\beta_{R}>\beta_{B}>\beta_{G}\) (D) \(\beta_{R}>\beta_{G}>\beta_{B}\)

In the determination of Young's modulus \(\left(Y=\frac{4 M L \mathrm{~g}}{\pi l d^{2}}\right)\) by using Searle's method, a wire of length \(L=2 \mathrm{~m}\) and diameter \(d=0.5 \mathrm{~mm}\) is used. For a load \(M=2.5 \mathrm{~kg}\), an extension \(l=0.25 \mathrm{~mm}\) in the length of the wire is observed. Quantities \(d\) and \(l\) are measured using a screw gauge and a micrometer, respectively. They have the same pitch of \(0.5 \mathrm{~mm}\). The number of divisions on their circular scale is 100 . The contributions to the maximum probable error of the \(Y\) measurement (A) due to the errors in the measurements of \(d\) and \(l\) are the same. (B) due to the error in the measurement of \(d\) is twice that due to the error in the measurement of \(l\). (C) due to the error in the measurement of \(l\) is twice that due to the error in the measurement of \(d\). (D) due to the error in the measurement of \(d\) is four times that due to the error in the measurement of \(l\).

Let \(z\) be a complex number such that the imaginary part of \(z\) is nonzero and \(a=z^{2}+z+1\) is real. Then \(a\) cannot take the value (A) \(-1\) (B) \(\frac{1}{3}\) (C) \(\frac{1}{2}\) (D) \(\frac{3}{4}\)

The point \(P\) is the intersection of the straight line joining the points \(Q(2,3,5)\) and \(R(1,-1,4)\) with the plane \(5 x-4 y-z=1\). If \(S\) is the foot of the perpendicular drawn from the point \(T(2,1,4)\) to \(Q R\), then the length of the line segment \(P S\) is (A) \(\frac{1}{\sqrt{2}}\) (B) \(\sqrt{2}\) (C) 2 (D) \(2 \sqrt{2}\)

The ellipse \(E_{1}: \frac{x^{2}}{9}+\frac{y^{2}}{4}=1\) is inscribed in a rectangle \(R\) whose sides are parallel to the coordinate axes. Another ellipse \(E_{2}\) passing through the point \((0,4)\) circumscribes the rectangle \(R\). The eccentricity of the ellipse \(E_{2}\) is (A) \(\frac{\sqrt{2}}{2}\) (B) \(\frac{\sqrt{3}}{2}\) (C) \(\frac{1}{2}\) (D) \(\frac{3}{4}\)

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