Q.If dxdf(x)=4x3−x43 such that f(2)=0. Then f(x) is (A) x4+x31+8129 (B) x3+x41+8129 (C) x4+x31−8129 (D) x3+x41−8129
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Initial Value Problem
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. …
Concept: Initial Value Problem — integrate the derivative, then use the given condition f(2)=0 to determine the constant of integration.
Step 1: Integrate
f(x)=∫(4x3−x43)dx=∫4x3dx−∫3x−4dx
=x4−3⋅−3x−3+C=x4+x31+C
Step 2: Apply f(2)=0
0=24+231+C=16+81+C …
We are given the derivative f′(x)=4x3−x43 and the initial condition f(2)=0. Integrating term by term gives f(x)=x4+x31+C, and using f(2)=0 yields C=−8129. So f(x)=x4+x31−8129, which matches option (C).
This is a classic Initial Value Problem (IVP). You are given the rate of change of a function (its derivative) and one specific value of the function itself. The idea is simple: if you know how fast something is changing and you know where it started, you can reconstruct the whole story. Here, the derivative tells us the slope of f at every x, and the point f(2)=0 anchors the curve at exactly one spot. Integrating the derivative recovers f up to an unknown constant; the initial condition pins that constant down.
Let’s walk through it.
- Integrate the derivative. We have f′(x)=4x3−x43. Rewrite x43 as 3x−4 to make the power rule clear. Then
f(x)=∫(4x3−3x−4)dx.
Integrate term by term:
- ∫4x3dx=4⋅4x4=x4,
- ∫−3x−4dx=−3⋅−3x−3=x−3=x31.
So
f(x)=x4+x31+C,
where C is the constant of integration.
A common slip is forgetting the sign when integrating x−4. The rule ∫xndx=n+1xn+1 works for n=−4: −3x−3, and then multiplying by −3 gives +x−3. Always check by differentiating: the derivative of x31 is −x43, which matches the given term.
- Use the initial condition to find C. We know f(2)=0. Substitute x=2 into the expression: …
Method: Solve an initial-value problem (integrate, then fix the constant)
Use this whenever you are given a derivative dxdf(x) plus one known value f(a), and must recover f(x). The extra condition is exactly what pins down C.
Steps
Step 1: Integrate the given derivative to get the general antiderivative.
Rewrite negative-power terms (e.g. x43=3x−4) and apply ∫xndx=n+1xn+1. This produces f(x) with an unknown constant +C.
Step 2: Substitute the given point to solve for C. …
Common Mistakes
Mistake 1: Forgetting the constant C before applying f(2)=0.
Why it's wrong: without +C there is nothing to solve for, and the condition f(2)=0 can't be used. Correct approach: integrate to x4+x31+C, then substitute.
Mistake 2: Integrating −x43 incorrectly. …
Showing the 12 most recent of 26 on this concept.
- AP EAPCET 2021Set eng-2021-08-23-AN1 markMCQQ.If f′(x)=tan2(x)+cot2(x) and f(4π)=0, then f(x)= ______ (A) tan(x)−cot(x)−x+2π (B) tan(x)−cot(x)−2x+2π (C) tan(x)+cot(x)−2x+2π (D) sec(x)−cosec(x)−2x+2π
›Reveal solutionSolution
Rewrite tan2x+cot2x using Pythagorean identities, integrate term by term, then fix the constant using f(π/4)=0.
Concept and Intuition
Whenever you see tan2x or cot2x in something you must integrate, immediately convert using tan2x=sec2x−1 and cot2x=csc2x−1 — these have known antiderivatives (tanx, −cotx), unlike the squared trig functions themselves.
Step-by-Step Solution
- Rewrite: f′(x)=(sec2x−1)+(csc2x−1)=sec2x+csc2x−2.
- Integrate: f(x)=∫(sec2x+csc2x−2)dx=tanx−cotx−2x+C.
- Apply the condition f(π/4)=0: tan(π/4)=1, cot(π/4)=1, so …
- AP EAPCET 2021Set eng-2021-08-20-AN1 markMCQQ.If f(x)=(cos2x)1+tanx1, then its anti-derivative F(x)= ______, given F(0)=4 (A) 1+tanx+4 (B) 32(1+tanx)3/2 (C) 2(1+tanx+1) (D) 1+tanx+2
›Reveal solutionSolution
A substitution-based integration followed by using the initial condition to fix the constant. The answer is 2(1+tanx+1).
Concept and Intuition
Recognizing that sec2xdx is exactly the derivative of 1+tanx lets a substitution reduce the integrand to a simple power of u, which integrates immediately.
Step-by-Step Solution
- f(x)=cos2x1+tanx1=1+tanxsec2x.
- Let u=1+tanx, so du=sec2xdx.
- F(x)=∫udu=2u+C=21+tanx+C.
- Apply F(0)=4: 21+tan0+C=21+C=2+C=4⇒C=2.
- So F(x)=21+tanx+2=2(1+tanx+1).
Common Mistakes …
- AP EAPCET 2023Set eng-2023-05-17-FN1 markMCQQ.If f′(x)=acosx+bsinx and f′(0)=4, f(0)=3, f(2π)=5, then f(x)= (A) 2cosx+4sinx+1 (B) 4cosx+2sinx+1 (C) 2cosx+3sinx+1 (D) 4cosx+sinx+1
›Reveal solutionSolution
a is pinned by f′(0), then integrating and using the two function values f(0)=3,f(π/2)=5 gives b and the constant of integration.
Concept and Intuition
Given f′(x) explicitly (up to unknown constants) and enough boundary values of f itself, integrate first (introducing a constant C), then use every given condition (there are exactly as many conditions as unknowns: a,b,C).
Step-by-Step Solution
- f′(x)=acosx+bsinx. At x=0: f′(0)=acos0+bsin0=a. Given f′(0)=4⇒a=4.
- Integrate: f(x)=∫(4cosx+bsinx)dx=4sinx−bcosx+C.
- f(0)=4(0)−b(1)+C=−b+C. Given =3: −b+C=3.
- f(π/2)=4(1)−b(0)+C=4+C. Given =5: C=1.
- From −b+1=3⇒b=−2.
- f(x)=4sinx−(−2)cosx+1=4sinx+2cosx+1, i.e. 2cosx+4sinx+1. …
- AP EAPCET 2022Set eng-2022-07-08-AN1 markMCQQ.If the solution of dxdy=xe1/y2y3cosx, y(0)=1 is y21=loge(f(x)), then f(x)= (A) 4+4sinx (B) esinx (C) 1−4sinx (D) e−4sinx
›Reveal solutionSolution
This is a separable ODE; separating variables and using the initial condition y(0)=1 gives f(x)=e−4sinx.
Concept and Intuition
The equation separates cleanly into a function of y times dy equal to a function of x times dx. Both sides then need simple substitutions (u=1/y2 and v=x) to become directly integrable exponential/trig forms.
Step-by-Step Solution
- dxdy=xe1/y2y3cosx⇒e1/y2y−3dy=xcosxdx.
- LHS: let u=1/y2⇒du=−2y−3dy⇒y−3dy=−21du. So ∫eu(−21)du=−21eu+C1=−21e1/y2+C1.
- RHS: let v=x⇒dv=2xdx⇒xdx=2dv. So ∫cosv⋅2dv=2sinv+C2=2sinx+C2.
- Combine: −21e1/y2=2sinx+C.
- Apply y(0)=1⇒1/y2=1 at x=0: −21e1=2sin0+C⇒C=−2e. …
- AP EAPCET 2026Set eng-2026-05-12-AN1 markMCQQ.If the solution of dxdy=log(x+1) when y(0)=3 is y=(x+1)log(x+1)+f(x), then f(x)= (A) 3−x (B) x−3 (C) 1−x (D) x−1
›Reveal solutionSolution
This tests integrating log(x+1) by substitution and then pinning the constant with the initial condition. The answer is f(x)=3−x.
Concept and Intuition
The differential equation dxdy=log(x+1) is already separated — y is just the antiderivative of the right-hand side. The initial condition y(0)=3 fixes the single constant of integration, and comparing the resulting expression to the given form of the solution lets us read off f(x) without guessing.
Step-by-Step Solution
- Integrate: y=∫log(x+1)dx+C.
- Substitute u=x+1, du=dx: ∫logudu=ulogu−u+C (standard result, by parts with dv=du).
- Back-substitute: y=(x+1)log(x+1)−(x+1)+C.
- Compare with the given form y=(x+1)log(x+1)+f(x): so f(x)=−(x+1)+C=C−1−x. …
- AP EAPCET 2023Set eng-2023-05-17-AN1 markMCQQ.g(x) is an anti derivative of f(x)=1+2xlog2 and the graph of y=g(x) passes through (−1,21). Then the curve meets the Y-axis at (A) (0, 1) (B) (0, 2) (C) (0, -2) (D) (1, 1)
›Reveal solutionSolution
Integrating f(x)=1+2xlog2 gives g(x)=x+2x+C; the given point fixes C=1, and evaluating at x=0 gives the Y-intercept (0,2).
Concept and Intuition
Since dxd2x=2xlog2, the antiderivative of 2xlog2 is simply 2x — recognizing this avoids unnecessary substitution work.
Step-by-Step Solution
- g(x)=∫(1+2xlog2)dx=x+2x+C.
- Use the given point (−1,21): g(−1)=−1+2−1+C=−1+21+C=−21+C=21⇒C=1.
- So g(x)=x+2x+1.
- Where the curve meets the Y-axis, x=0: g(0)=0+20+1=0+1+1=2. …
- AP EAPCET 2023Set eng-2023-05-16-AN1 markMCQQ.If a curve passes through (1,2) and has the slope of its tangent 1−x21 at a point (x,y), then the equation of that curve is (A) y=3x−x1 (B) y=x+x1 (C) y=2x+x1−1 (D) y=x+x2−1
›Reveal solutionSolution
Direct integration of the given slope expression, followed by using the point (1,2) to fix the constant, gives y=x+x1.
Concept and Intuition
When the slope dxdy is given purely as a function of x, the curve is found by straightforward integration (no need for separation of variables in a more complex sense) — then a known point on the curve pins down the constant of integration.
Step-by-Step Solution
- dxdy=1−x21.
- Integrate both sides: y=∫(1−x21)dx=x+x1+C.
- Apply the point (1,2): 2=1+1+C⇒C=0. …
- AP EAPCET 2021Set eng-2021-08-25-AN1 markMCQQ.Let y=Y(x) be the solution of the differential equation dxdy+ytanx=2x+x2tanx, x∈(2−π,2π), such that Y(0)=1, then ________ (A) y(4π)+Y(4−π)=2π2+2 (B) y′(4π)+Y′(4−π)=−2 (C) y(4π)−Y(4−π)=2 (D) y′(4π)−Y′(4−π)=π−2
›Reveal solutionSolution
Solving the first-order linear ODE explicitly gives Y(x)=x2+cosx; checking each option against this closed form picks out (D). Answer: π−2.
Concept and Intuition
This is a standard first-order linear ODE dxdy+P(x)y=Q(x), solved with an integrating factor. Once we have the explicit closed form for Y(x), we can just plug in and test every option directly instead of guessing.
Step-by-Step Solution
- ODE: dxdy+ytanx=2x+x2tanx. Integrating factor: μ=e∫tanxdx=e−log∣cosx∣=secx.
- Multiply through by secx: secxdxdy+ysecxtanx=2xsecx+x2secxtanx.
- LHS =dxd(ysecx). Check RHS: dxd(x2secx)=2xsecx+x2secxtanx — matches exactly!
- So dxd(ysecx)=dxd(x2secx)⇒ysecx=x2secx+C⇒y=x2+Ccosx.
- Apply Y(0)=1: 0+C(1)=1⇒C=1. So Y(x)=x2+cosx.
- Y′(x)=2x−sinx. Compute Y′(π/4)=2π−22 and Y′(−π/4)=−2π+22. …
- AP EAPCET 2023Set eng-2023-05-16-FN1 markMCQQ.If y=y(x) is the solution of dxdy=1+sinxx−ycosx, y(2π)=8π2, then y(π)= (A) 85π2 (B) 87π2 (C) 89π2 (D) 712π2
›Reveal solutionSolution
Recognise the left side of the rearranged ODE as an exact derivative dxd[y(1+sinx)], integrate directly, use the initial condition to find the constant, then evaluate at x=π.
Concept and Intuition
Many "linear-looking" first-order ODEs are secretly exact derivatives in disguise — recognising the pattern y′g(x)+yg′(x)=dxd[yg(x)] turns a substitution-heavy linear-ODE problem into direct integration.
Step-by-Step Solution
- Given: dxdy=1+sinxx−ycosx. Multiply through by (1+sinx): (1+sinx)dxdy+ycosx=x.
- Note dxd[y(1+sinx)]=y′(1+sinx)+ycosx — exactly the left side above.
- So dxd[y(1+sinx)]=x. Integrate: y(1+sinx)=2x2+C.
- Apply y(π/2)=8π2: 1+sin(π/2)=2, so LHS =8π2×2=4π2.
- RHS at x=π/2: 2(π/2)2+C=8π2+C.
- Equate: 4π2=8π2+C⇒C=8π2.
- General solution: y(1+sinx)=2x2+8π2. …
- AP EAPCET 2023Set eng-2023-05-16-FN1 markMCQQ.If limx→∞y(x)=2π, then the solution of x3sinydxdy=2 is cosy= (A) x23 (B) x1 (C) x21 (D) x32
›Reveal solutionSolution
This is a separable ODE; integrate directly and use the given limiting condition at infinity to pin down the constant of integration.
Concept and Intuition
x3sinydy/dx=2 separates cleanly into a function of y times dy equals a function of x times dx. The unusual boundary condition (a limit as x→∞, rather than a value at a finite point) still fixes the constant because both sides of the solution tend to definite limits.
Step-by-Step Solution
- Rewrite: x3sinydxdy=2⇒sinydy=x32dx.
- Integrate both sides: ∫sinydy=∫2x−3dx⇒−cosy=−x−2+C0.
- Rearranged: cosy=x−2−C0=x21−C (renaming the constant). …
- AP EAPCET 2025Set eng-2025-05-24-FN1 markMCQQ.The solution of the differential equation x2(y+1)dxdy+y2(x+1)2=0, when y(1)=2, is (A) log∣x2y∣=x2+y1+x−1 (B) log41x2y=x1+y2+x−1 (C) log21x2y=x1+y1−x−21 (D) log31x2y=x1+y1−x+21
›Reveal solutionSolution
This is a separable ODE; separating and integrating gives an implicit relation, and the initial condition y(1)=2 pins the constant to match option (C).
Concept and Intuition
x2(y+1)dy=−y2(x+1)2dx separates cleanly because all the y-terms can be gathered on one side (as y2y+1) and all x-terms on the other (as x2(x+1)2). Both sides then reduce to standard integrals: y1+y21 integrates via power rule and log, and x2(x+1)2=1+x2+x21 likewise.
Step-by-Step Solution
- Rearranging: x2(y+1)dy=−y2(x+1)2dx⇒y2y+1dy=−x2(x+1)2dx.
- LHS: y2y+1=y1+y21, so ∫(y1+y21)dy=log∣y∣−y1+C1.
- RHS: x2(x+1)2=x2x2+2x+1=1+x2+x21, so −∫(1+x2+x21)dx=−x−2log∣x∣+x1+C2.
- Equate: log∣y∣−y1=−x−2log∣x∣+x1+C.
- Rearranged: log∣y∣+2log∣x∣=x1+y1−x+C⇒log(x2y)=x1+y1−x+C.
- Apply y(1)=2: log(1⋅2)=1+21−1+C⇒ln2=21+C⇒C=ln2−21.
- Substitute back: log(x2y)=x1+y1−x+ln2−21, i.e. log(x2y)−ln2=x1+y1−x−21.
- log(x2y)−ln2=log(2x2y)=log21x2y, so finally …
- AP EAPCET 2026Set eng-2026-05-13-FN1 markMCQQ.If y=f(x) is a solution of dxdy=(y−Kx)2+K when x=0 and y=1, then f(2)= (A) 2K+1 (B) 2K−1 (C) 2K+5 (D) 2K−5
›Reveal solutionSolution
A shift substitution v=y−Kx turns the equation into the separable dv/dx=v2; solving and evaluating at x=2 gives f(2)=2K−1.
Concept and Intuition
The right side (y−Kx)2+K is not separable in y directly, but the combination y−Kx appears squared — this is the signal to substitute v=y−Kx, which typically removes the extra additive constant K from the derivative and leaves a clean separable equation in v.
Step-by-Step Solution
- Let v=y−Kx. Then dxdv=dxdy−K.
- Given dxdy=(y−Kx)2+K=v2+K, so dxdv=v2+K−K=v2.
- Separate variables: v2dv=dx⇒−v1=x+c.
- Initial condition: at x=0, y=1⇒v=y−K⋅0=1. So −1=0+c⇒c=−1.
- Thus −v1=x−1⇒v=1−x1. …
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