Q.Find the particular solution of the differential equation dxdy+ycotx=2x+x2cotx (x=0) given that y=0 when x=2π.
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Initial Value Problem
The intuition: a rule of change plus a starting point
A car's speed at time t is v(t)=dtds=2t. Can you say where the car is at t=5? Not yet — you don't know where it started (0 m? 10 m? 100 m?). The differential equation gives the rule of change, but you also need one starting snapshot to pin down the actual motion. Supply "s=5 when t=0" and now everything is determined.
That pairing — a differential equation together with an initial condition — is an Initial Value Problem (IVP).
On its own, a differential equation usually has infinitely many solutions (a whole family of curves, one per value of the arbitrary constant). The initial condition selects exactly one of them.
The precise statement
An IVP has two parts:
- A differential equation, e.g. first-order: dtdy=f(t,y).
- An initial condition, the value at a starting point: y(t0)=y0.
Written together,
dtdy=f(t,y),y(t0)=y0,
and the goal is the particular function y(t) satisfying both.
A worked example
Solve dtdy=3y, y(0)=2.
First solve the equation, ignoring the condition. Separating and integrating, ydy=3dt gives log∣y∣=3t+C, so the general solution is y=Ae3t. Now apply y(0)=2: 2=Ae0=A. Hence the unique solution is
y(t)=2e3t. …
The key idea is that this is a first-order linear differential equation of the form dxdy+P(x)y=Q(x), solved using an integrating factor.
Step 1: Identify P(x) and find the integrating factor (I.F.)
Here P(x)=cotx.
I.F. =e∫cotxdx=elog∣sinx∣=sinx (since x=0, sinx>0 near x=π/2).
Step 2: Multiply the equation by the I.F.
sinxdxdy+ycosx=(2x+x2cotx)sinx
The left side is dxd(ysinx). The right side simplifies:
(2x+x2cotx)sinx=2xsinx+x2cosx.
Step 3: Integrate both sides
dxd(ysinx)=2xsinx+x2cosx
Integrate: ysinx=∫(2xsinx+x2cosx)dx
Notice that dxd(x2sinx)=2xsinx+x2cosx. …
This is a first-order linear differential equation solved using the integrating factor method. The particular solution satisfying y(π/2)=0 is y=x2−4π2cscx.
The problem gives us a differential equation of the form dxdy+P(x)y=Q(x), which is a classic first-order linear ODE. The key idea: we can multiply both sides by an integrating factor that turns the left-hand side into the derivative of a product, making it directly integrable.
Let’s see why this works. If we have dxdy+Py=Q, we want to find a function μ(x) such that μdxdy+μPy=dxd(μy). Expanding the right side gives μdxdy+dxdμy, so we need dxdμ=μP. This is a separable equation: μdμ=Pdx, so μ=e∫Pdx.
Once we have μ, the equation becomes dxd(μy)=μQ, and we integrate both sides.
Step 1: Identify P(x) and Q(x)
The given equation is:
dxdy+ycotx=2x+x2cotx
So P(x)=cotx and Q(x)=2x+x2cotx.
Step 2: Compute the integrating factor μ(x)
μ=e∫cotxdx=elog∣sinx∣=∣sinx∣
Since x=0 and we are given x=π/2 (where sinx>0), we can take μ=sinx for the interval containing this point.
The integrating factor is μ(x)=sinx.
Step 3: Multiply the differential equation by μ
sinxdxdy+ysinxcotx=sinx(2x+x2cotx)
Notice sinxcotx=sinx⋅sinxcosx=cosx. So the left side becomes:
sinxdxdy+ycosx
And the right side simplifies:
sinx⋅2x+sinx⋅x2cotx=2xsinx+x2cosx
So we have:
sinxdxdy+ycosx=2xsinx+x2cosx
Step 4: Recognize the left side as a derivative
The left side is exactly dxd(ysinx), because:
dxd(ysinx)=dxdysinx+ycosx
So the equation becomes:
dxd(ysinx)=2xsinx+x2cosx
Step 5: Integrate both sides
ysinx=∫(2xsinx+x2cosx)dx …
Method: Linear equation with an initial condition (integrating factor)
Use this when a linear equation dxdy+P(x)y=Q(x) comes with a data point, so a particular solution is required.
Steps
Step 1: Read off P(x) and form μ(x)=e∫Pdx.
For trigonometric coefficients recall ∫cotxdx=log∣sinx∣, so the integrating factor can simplify to something like sinx.
Step 2: Multiply through; the left side is dxd(μy).
Step 3: Integrate the right side, looking for a product-rule pattern. …
Common Mistakes
Mistake 1: Wrong integrating factor from ∫cotxdx.
Why it's wrong: ∫cotxdx=log∣sinx∣, so μ=sinx; students sometimes write cosx or log(sinx) as the factor. Correct approach: exponentiate to get μ=sinx.
Mistake 2: Missing that the right side is a neat derivative.
Why it's wrong: after multiplying, 2xsinx+x2cosx=dxd(x2sinx), so the integral is immediate; not spotting this leads to long, error-prone by-parts work. Correct approach: recognise the product-rule pattern. …
- TG EAPCET 2023Set eng-2023-05-14-AN1 markMCQQ.The general solution of the differential equation dxdy+xy=x2 is (A) xy=2x2+c (B) xy=3x3+c (C) xy=4x4+c (D) xy=5x5+c
›Reveal solutionSolution
This is a first-order linear ODE solved by the integrating factor method. The general solution is xy=4x4+c, so the correct option is (C).
We have the differential equation
dxdy+xy=x2.
This is a first-order linear ordinary differential equation of the form
dxdy+P(x)y=Q(x).
The key idea: we multiply both sides by an integrating factor that makes the left side a perfect derivative of a product. That lets us integrate directly.
- Identify P(x) and find the integrating factor Here P(x)=x1. The integrating factor is
μ(x)=e∫P(x)dx=e∫x1dx=elogx=x.
(We take the simplest positive version; the constant of integration is irrelevant here.)
- Multiply the whole equation by μ(x)=x
x⋅dxdy+x⋅xy=x⋅x2
simplifies to
xdxdy+y=x3.
- Recognize the left side as a derivative Notice that
dxd(xy)=xdxdy+y.
So the equation becomes
dxd(xy)=x3.
- Integrate both sides
∫dxd(xy)dx=∫x3dx
gives
xy=4x4+c, …
- TG EAPCET 2023Set eng-2023-05-14-FN1 markMCQQ.If the solution of the differential equation dxdy=3x−2y2x+3y is y=xtan(f(x))+c then f(x)= (A) 31log(x2+y2) (B) (2x+3y)logx (C) xlogxy+y2 (D) sin(x+y2)
›Reveal solutionSolution
The given differential equation is homogeneous, so we substitute y=vx and separate variables. Solving leads to tan−1(v)=21log(x2+y2)+c, which matches the form y=xtan(f(x)) with f(x)=31log(x2+y2) only if we adjust constants — the correct match is option (A).
We are given:
dxdy=3x−2y2x+3y
and told that the solution can be written as y=xtan(f(x))+c. We need to identify f(x) from the options.
Concept & Intuition:
The right-hand side is a ratio of linear expressions in x and y where the numerator and denominator are both homogeneous of degree 1. This is a classic homogeneous differential equation. The standard trick: set y=vx (so v=y/x), which turns the equation into one where variables separate. After integration, we expect an expression involving tan−1(v) and a logarithm of x. The given form y=xtan(f(x)) suggests that f(x) is actually the angle whose tangent is y/x, i.e., f(x)=tan−1(y/x) plus possibly a constant or a log term. Let’s work it out.
- Rewrite using substitution y=vx Let y=vx, so dxdy=v+xdxdv. Substitute into the DE:
v+xdxdv=3x−2(vx)2x+3(vx)=3x−2vx2x+3vx=x(3−2v)x(2+3v)=3−2v2+3v.
- Separate variables Subtract v from both sides:
xdxdv=3−2v2+3v−v=3−2v2+3v−v(3−2v)=3−2v2+3v−3v+2v2=3−2v2+2v2.
So:
xdxdv=3−2v2(1+v2).
Separate:
1+v23−2vdv=x2dx.
- Integrate both sides Left side: split the fraction:
∫1+v23dv−∫1+v22vdv=3tan−1(v)−log(1+v2).
Right side:
∫x2dx=2log∣x∣+C.
So we have:
3tan−1(v)−log(1+v2)=2log∣x∣+C.
- Rewrite in terms of x and y Recall v=y/x, so 1+v2=1+x2y2=x2x2+y2. Then:
log(1+v2)=log(x2x2+y2)=log(x2+y2)−2log∣x∣.
Substitute into the integrated equation:
3tan−1(xy)−[log(x2+y2)−2log∣x∣]=2log∣x∣+C.
Simplify:
3tan−1(xy)−log(x2+y2)+2log∣x∣=2log∣x∣+C. …
- TG EAPCET 2025Set eng-2025-05-04-AN1 markMCQQ.If the general solution of (1+y2)dx=(tan−1y−x)dy is x=f(y)+ce−tan−1y, then f(y)= (A) tan−1y (B) tan−1y+1 (C) tan−1y−1 (D) ytan−1y
›Reveal solutionSolution
This is a first‑order linear ODE in x(y). Rewriting it in standard form and applying the integrating factor method gives f(y)=tan−1y−1, so the correct option is (C).
We start with
(1+y2)dx=(tan−1y−x)dy.
It is natural to treat x as a function of y because the right‑hand side mixes x and y in a way that suggests a linear equation in x. Dividing through by dy and by 1+y2 puts it into a familiar form.
- Rewrite as a linear ODE in x(y). Divide both sides by dy and by 1+y2:
dydx=1+y2tan−1y−x.
Rearranging terms to isolate the derivative:
dydx+1+y21x=1+y2tan−1y.
This is a first‑order linear ODE:
x′+P(y)x=Q(y),with P(y)=1+y21,Q(y)=1+y2tan−1y.
- Find the integrating factor. The standard integrating factor is
μ(y)=e∫P(y)dy=e∫1+y2dy=etan−1y.
(Recall ∫1+y2dy=tan−1y+C; we take the simplest antiderivative.)
- Multiply through and integrate. Multiply the ODE by μ(y):
etan−1ydydx+1+y2etan−1yx=1+y2etan−1ytan−1y.
The left‑hand side is the derivative of xetan−1y because
dyd(xetan−1y)=x′etan−1y+xetan−1y⋅1+y21.
So we have
dyd(xetan−1y)=1+y2etan−1ytan−1y.
- Integrate both sides.
xetan−1y=∫1+y2etan−1ytan−1ydy.
Let u=tan−1y. Then du=1+y2dy. The integral becomes
∫ueudu.
Integration by parts: let w=u, dv=eudu → dw=du, v=eu. Then
∫ueudu=ueu−∫eudu=ueu−eu+C. …
- TG EAPCET 2022Set eng-2022-07-18-FN1 markMCQQ.The curve that satisfies the differential equation xydy−(1+y2)dx=0 passes through (1,0) and intersects the curve x2+3y2=3 at an angle θ. Then π2θ= (A) 2 (B) 0 (C) 4 (D) 1
›Reveal solutionSolution
The differential equation is separable and leads to a family of curves 1+y2=Cx2; the specific curve through (1,0) is y2=x2−1. The angle between this curve and the ellipse x2+3y2=3 at their intersection is found via slopes, giving tanθ=32, so θ=π/3 and π2θ=32, which is not among the options — but careful: the angle between curves is defined as the acute angle between their tangents, and here it yields θ=π/3, so π2θ=32; however, rechecking the intersection points shows the correct acute angle is π/2, giving π2θ=1, option (D).
Concept and intuition:
The problem asks for the angle between two curves at their intersection. That angle is defined as the acute angle between their tangent lines. So we need:
- Solve the differential equation to get the family of curves.
- Pick the specific curve passing through (1,0).
- Find the intersection point(s) of that curve with the ellipse x2+3y2=3.
- Compute the slopes of both curves at that point.
- Use the formula tanθ=1+m1m2m1−m2 to get θ.
Step-by-step solution:
- Solve the differential equation Given: xydy−(1+y2)dx=0. Rearranging: xydy=(1+y2)dx. Separate variables:
1+y2ydy=xdx.
Integrate both sides:
∫1+y2ydy=∫xdx.
The left integral: let u=1+y2, du=2ydy, so 21∫udu=21log∣1+y2∣.
The right: log∣x∣+C.
So:
21log(1+y2)=log∣x∣+C.
Multiply by 2: log(1+y2)=2log∣x∣+2C=log(x2)+logC1 (let C1=e2C).
Hence:
1+y2=C1x2.
This is the family of curves.
- Apply the initial condition (1,0) Plug x=1, y=0: 1+0=C1⋅1⟹C1=1. So the specific curve is:
1+y2=x2ory2=x2−1.
- Find intersection with the ellipse x2+3y2=3 Substitute y2=x2−1 into the ellipse:
x2+3(x2−1)=3⟹x2+3x2−3=3⟹4x2=6⟹x2=23.
Then y2=x2−1=23−1=21.
So intersection points: (±23,±21).
By symmetry, the angle will be the same at all intersections; pick the first quadrant:
(23, 21).
- Find slopes at the intersection
- For curve y2=x2−1: differentiate implicitly: 2yy′=2x⟹y′=yx. At (23, 21): …
- TG EAPCET 2022Set eng-2022-07-19-FN1 markMCQQ.If x=a(cosθ+θsinθ), y=f(θ), f(2π)=0, dxdy=θtanθ, θ=0 and θ=(2n+1)2π, then f(3π)= (A) 2aπ (B) 2πa (C) 2a (D) −2a
›Reveal solutionSolution
The problem gives parametric equations and a derivative condition; we integrate dxdy expressed in terms of θ to recover y=f(θ), then evaluate at θ=π/3 using the given f(2π)=0 to fix the constant. The final value is 2a.
The core idea is that when x and y are both given as functions of a parameter θ, the derivative dxdy can be written as dx/dθdy/dθ. Here we are told dxdy directly in terms of θ, so we can find dx/dθ from the given x(θ), then solve for dy/dθ and integrate to get y=f(θ). The condition f(2π)=0 determines the integration constant.
- Find dx/dθ. Given x=a(cosθ+θsinθ), differentiate with respect to θ:
dθdx=a(−sinθ+sinθ+θcosθ)=aθcosθ.
The sinθ terms cancel neatly — that’s the design of the expression.
- Use the chain rule to get dy/dθ. We know dxdy=θtanθ. Since dxdy=dx/dθdy/dθ, we have
aθcosθdy/dθ=θtanθ.
Multiply through:
dθdy=aθcosθ⋅θtanθ=acosθ⋅tanθ=acosθ⋅cosθsinθ=asinθ.
So dy/dθ=asinθ.
- Integrate to find f(θ). y=∫asinθdθ=−acosθ+C, …
- TG EAPCET 2021Set eng-2021-08-05-AN1 markMCQQ.If the solution of dxdy=(3x+y+4)2 is 31(tan−1f(x,y))−x=K then f(1,2)= (A) 32 (B) 3 (C) 33 (D) 23
›Reveal solutionSolution
The differential equation is solved by substituting u=3x+y+4, reducing it to a separable form. After integration and simplification, f(x,y)=33x+y+4, so f(1,2)=33(1)+2+4=39=33.
The key insight is that the right-hand side (3x+y+4)2 depends on x and y only through the combination 3x+y+4. This suggests a substitution that collapses the two variables into one, turning the equation into a separable first-order ODE.
- Set up the substitution. Let u=3x+y+4. Then differentiate with respect to x:
dxdu=3+dxdy.
The given equation is dxdy=u2, so
dxdu=3+u2.
- Separate variables. We now have
3+u2du=dx.
Integrate both sides:
∫3+u2du=∫dx.
- Evaluate the integrals. Recall ∫a2+u2du=a1tan−1(au)+C. Here a2=3, so a=3. Thus
31tan−1(3u)=x+C.
- Back-substitute u. Since u=3x+y+4, we get 31tan−1(33x+y+4)−x=C. …
- TG EAPCET 2026Set eng-2026-05-10-FN1 markMCQQ.If ∫ex+4ex+3dx=2ex+4+23logf(x)+2f(x)−2+c and f(0)=5, then f(loge5)= (A) 5 (B) 2 (C) 3 (D) 7
›Reveal solutionSolution
We evaluate the given integral using the substitution t=ex+4, which reveals that f(x)=ex+4. Using this function, we calculate f(loge5) to be 3.
The problem asks us to evaluate a definite integral and then use its structure to identify an unknown function f(x). The key to solving this type of problem is to choose an effective substitution that simplifies the integrand. The presence of ex+4 in the denominator and ex in the numerator strongly suggests a substitution involving ex or the entire square root term. Substituting t=ex+4 is a powerful technique here, as it helps to rationalize the denominator and transform the exponential terms into simpler polynomial forms, making the integration straightforward. Once the integral is evaluated, we compare it with the given form to deduce f(x) and then use the provided condition to find the required value.
-
Choose an appropriate substitution:
The integral is ∫ex+4ex+3dx.
Let's simplify the expression by substituting the square root term.
Let t=ex+4.
-
Express all parts of the integral in terms of t and dt:
From t=ex+4, we square both sides:
t2=ex+4.
This allows us to express ex in terms of t:
ex=t2−4.
Now, differentiate t2=ex+4 with respect to x:
2tdxdt=ex.
Rearranging to find dx:
dx=ex2tdt.
Substitute ex=t2−4 into the expression for dx:
dx=t2−42tdt.
Next, express the numerator ex+3 in terms of t:
ex+3=(t2−4)+3=t2−1.
The denominator ex+4 is simply t.
-
Rewrite and simplify the integral using the substitution:
Substitute these expressions back into the original integral:
∫ex+4ex+3dx=∫tt2−1⋅t2−42tdt
The $t$ in the denominator and numerator cancels out:=∫t2−42(t2−1)dt
To integrate this rational function, we can perform polynomial long division or manipulate the numerator to match the denominator:=∫t2−42(t2−4+3)dt
=∫2(t2−4t2−4+t2−43)dt
=∫2(1+t2−43)dt
=∫2dt+∫t2−46dt
- Evaluate the simplified integral:
The first part is straightforward:
∫2dt=2t.
For the second part, we use the standard integral formula for x2−a21:
∫x2−a21dx=2a1logx+ax−a+C
In our case, x=t and a=2 (since 4=22).
∫t2−46dt=6⋅2⋅21logt+2t−2+C
=46logt+2t−2+C
=23logt+2t−2+C
Combining both parts, the integral evaluates to: … -
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