Q.If y(t) is a solution of (1+t)dtdy−ty=1 and y(0)=−1, then show that y(1)=−21.
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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. …
The key idea is to solve the Initial Value Problem (IVP) by rewriting the differential equation in standard linear form and using an integrating factor.
Step 1: Write the equation in standard linear form:
dtdy−1+tty=1+t1,t=−1.
Step 2: The integrating factor is
μ(t)=e∫−1+ttdt.
Compute ∫1+ttdt=∫(1−1+t1)dt=t−log∣1+t∣, so
μ(t)=e−(t−log∣1+t∣)=e−t(1+t).
Step 3: Multiply through by μ(t):
dtd[e−t(1+t)y]=e−t.
Integrate both sides from 0 to t: …
This is a first-order linear ODE solved using an integrating factor. The solution satisfying y(0)=−1 gives y(1)=−21.
The problem gives us a differential equation and an initial condition — that’s an Initial Value Problem (IVP). The goal is to find the specific function y(t) that satisfies both the equation and the starting value, then evaluate it at t=1.
The equation is:
(1+t)dtdy−ty=1,y(0)=−1
This is a first-order linear ODE in y. The standard form is dtdy+P(t)y=Q(t). Let’s rewrite it.
- Rewrite in standard linear form
Divide through by (1+t) (valid for t=−1, and we only care about t=0 to t=1, so fine):
dtdy−1+tty=1+t1
So P(t)=−1+tt and Q(t)=1+t1.
- Find the integrating factor
The integrating factor is μ(t)=e∫P(t)dt.
Compute ∫P(t)dt=∫−1+ttdt.
Simplify the integrand: −1+tt=−(1−1+t1)=−1+1+t1.
So:
∫P(t)dt=∫(−1+1+t1)dt=−t+log∣1+t∣+C
We only need one antiderivative, so take C=0. Then:
μ(t)=e−t+log∣1+t∣=e−t⋅elog∣1+t∣=(1+t)e−t
Since t>−1 in our domain, 1+t>0, so absolute values drop.
The integrating factor is μ(t)=(1+t)e−t.
- Multiply the ODE by μ(t)
Multiply the standard form by μ(t):
(1+t)e−tdtdy−(1+t)e−t⋅1+tty=(1+t)e−t⋅1+t1
Simplify the second term: (1+t)e−t⋅1+tt=te−t. The right side becomes e−t.
So we have:
(1+t)e−tdtdy−te−ty=e−t
Notice the left side is exactly dtd[(1+t)e−ty]. Check by differentiating:
dtd[(1+t)e−ty]=(1+t)e−tdtdy+[e−t−(1+t)e−t]y=(1+t)e−tdtdy−te−ty
Yes, matches.
So the equation becomes:
dtd[(1+t)e−ty]=e−t
- Integrate both sides
Integrate from 0 to t (or indefinitely and then use initial condition):
∫0tdsd[(1+s)e−sy(s)]ds=∫0te−sds …
Method: Linear IVP via integrating factor, then verifying a value
Use this for a linear first-order equation with an initial condition, where you must confirm a specific value of the solution.
Steps
Step 1: Standard linear form
Divide to get dtdy+P(t)y=Q(t) and read off P(t), Q(t).
Step 2: Integrating factor
IF=e∫P(t)dt. …
Common Mistakes
Mistake 1: Mis-evaluating ∫1+ttdt
Why it's wrong: it equals t−log∣1+t∣ (split 1+tt=1−1+t1), not log∣1+t∣. Correct approach: do the algebraic split first.
Mistake 2: Getting the integrating factor sign wrong
Why it's wrong: with P=−1+tt, IF=e−(t−log∣1+t∣)=e−t(1+t). Correct approach: track the minus sign carefully. …
Showing the 12 most recent of 26 on this concept.
- AP EAPCET 2022Set eng-2022-07-05-FN1 markMCQQ.If the general solution of the differential equation cos2xdxdy+y=tanx is y=tanx−1+Ce−tanx satisfies y(π/4)=1, then C= (A) e (B) 1 (C) −1 (D) 1/e
›Reveal solutionSolution
This tests applying an initial condition to a given general solution of a linear first-order DE to find the arbitrary constant.
Concept and Intuition
Once a general solution y=y(x,C) is known, an initial condition (initial value) pins down C by substituting the given point directly — no need to re-derive the DE.
Step-by-Step Solution
- General solution: y=tanx−1+Ce−tanx.
- At x=π/4: tan(π/4)=1.
- So y(π/4)=1−1+Ce−1=Ce−1. …
- 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 2023Set eng-2023-05-18-AN1 markMCQQ.If f(x) is a function such that f′(x)=f2(x)−1 and f(0)=1, then f(1)= (A) 2ee−2+1 (B) 2ee2+1 (C) 2ee2−1 (D) 2ee−2−1
›Reveal solutionSolution
This is a separable differential equation whose natural substitution is the hyperbolic identity cosh2u−sinh2u=1; the answer is f(1)=cosh1=2ee2+1.
Concept and Intuition
Whenever you see f′(x)=f2(x)−1, the structure f2−1 screams hyperbolic substitution, because cosh2u−1=sinh2u. Setting f=coshu turns the messy square root into the clean function sinhu, and the chain rule collapses the whole ODE to u′=1 — a straight line in disguise.
Step-by-Step Solution
- Separate variables: f2−1df=dx.
- Let f=coshu, so df=sinhudu and f2−1=sinhu (taking u≥0 since f≥1 near x=0).
- The equation becomes sinhusinhudu=dx⇒du=dx⇒u=x+C. …
- AP EAPCET 2022Set eng-2022-07-04-FN1 markMCQQ.If the solution of dxdy−yloge0.5=0, y(0)=1, and y(x)→k, as x→∞ then k= (A) ∞ (B) −1 (C) 1 (D) 0
›Reveal solutionSolution
A linear first-order ODE dy/dx=ky with k=loge0.5<0 describes exponential decay, so y→0 as x→∞; k=0.
Concept and Intuition
dxdy=cy always solves to y=y0ecx. The sign of c decides growth (c>0) or decay (c<0) as x→∞. Here c=loge(0.5)=−loge2<0, so the solution decays to zero.
Step-by-Step Solution
- Rewrite: dxdy=yloge(0.5), i.e. ydy=loge(0.5)dx.
- Integrate: logey=xloge(0.5)+C1, so y=Cexloge(0.5)=C(0.5)x.
- Apply y(0)=1: 1=C(0.5)0=C, so C=1. Hence y(x)=(0.5)x. …
- AP EAPCET 2021Set eng-2021-08-24-AN1 markMCQQ.The equation of a curve passing through the point (0,1), given that the slope of the tangent to the curve at any point (x,y) is equal to the sum of the x-coordinate, and the product of x and y coordinates at that point, is ________ (A) y=1−2e(x2/2) (B) y=−1+2e(x2/2) (C) y=−1−2e(x2/2) (D) y=1+2e(x2/2)
›Reveal solutionSolution
Translate the word problem into a separable differential equation dxdy=x(1+y), solve it, and apply the initial point (0,1) to fix the constant — giving y=−1+2ex2/2.
Concept and Intuition
"Slope of the tangent" always means dxdy. The sentence describing the slope translates directly into an algebraic expression in x and y; recognizing that it factors as x(1+y) makes the equation separable, which is the easiest class of ODE to solve.
Step-by-Step Solution
- Translate: slope = (x-coordinate) + (product of x and y) ⇒dxdy=x+xy=x(1+y).
- Separate variables: 1+ydy=xdx.
- Integrate both sides: log∣1+y∣=2x2+C.
- Apply the point (0,1): log∣1+1∣=0+C⇒C=log2. …
- AP EAPCET 2025Set eng-2025-05-24-FN1 markMCQQ.If xlogxdxdy+y=logx2 and y(e)=0, then y(e2)= (A) 0 (B) 1 (C) 21 (D) 23
›Reveal solutionSolution
This is a first-order linear ODE in y; finding the integrating factor logx and applying y(e)=0 gives y(e2)=23.
Concept and Intuition
Dividing the given equation by xlogx puts it in the standard linear form dxdy+P(x)y=Q(x), which is always solvable via an integrating factor μ=e∫Pdx. Recognizing log(x2)=2logx also simplifies the RHS immediately.
Step-by-Step Solution
- Given: xlogxdxdy+y=log(x2)=2logx.
- Divide throughout by xlogx: dxdy+xlogxy=x2.
- This is linear with P(x)=xlogx1. Integrating factor:
μ=e∫xlogx1dx.
Let u=logx, du=dx/x, so ∫xlogxdx=∫udu=log∣u∣=log∣logx∣. Hence μ=elog∣logx∣=logx (positive since x>1 in this problem).
4. Multiply the linear ODE by μ=logx:
logx⋅dxdy+xy=x2logx.
- The LHS is exactly dxd(ylogx) (product rule check: y′logx+y⋅x1 — matches).
- Integrate both sides: ylogx=∫x2logxdx. With u=logx: ∫2udu=u2=(logx)2. So ylogx=(logx)2+C. …
- 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-2023-05-17-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 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 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 2022Set eng-2022-07-06-FN1 markMCQQ.The solution of (1+y2)dx−xydy=0, y(1)=0 represents a conic. Its eccentricity is (A) 2 (B) 1/e (C) 1 (D) 2
›Reveal solutionSolution
Solving the separable ODE with the given initial condition yields the rectangular hyperbola x2−y2=1, whose eccentricity is 2.
Concept and Intuition
Separate the variables in the ODE, integrate, apply the initial condition to fix the constant, and identify the resulting conic. A rectangular hyperbola (a=b) always has eccentricity 2 — a fact worth recognising instantly once the conic's form is found.
Step-by-Step Solution
- Given (1+y2)dx−xydy=0⇒(1+y2)dx=xydy⇒xdx=1+y2ydy.
- Integrate both sides: logx=21log(1+y2)+C.
- Exponentiate: x=k1+y2 for some constant k>0, i.e. x2=k2(1+y2), or x2−k2y2=k2.
- Apply y(1)=0: at x=1,y=0: 1=k2(1+0)⇒k2=1⇒k=1.
- So the curve is x2−y2=1, a rectangular hyperbola with a2=1, b2=1. …
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