Twenty-five fully worked problems in five batches: order/degree and verification, separable equations, homogeneous equations, linear equations, and mixed curve/model problems at miscellaneous level.
The classification ritual for every solving problem:
Is the right side a product g(x)h(y)? → separable.
Is it a function of the ratio xy (uniform degrees)? → homogeneous: y=vx.
Do y and y′ appear linearly? → linear: compute the I.F. (Check the mirror orientation too — linear in x.)
Solve generally, then apply any given condition to fix C.
Key Point: Marks are lost at classification, not at integration. Spend the first fifteen seconds of every problem naming its type — the rest is Chapter 7 machinery.
Batch 1 — Order, Degree and Verification (Easy)
Example 1: A clean third-order equation
Find the order and degree of y′′′+2y′′+y′=0.
Solution:
Order: highest derivative y′′′ — order 3.
Degree: polynomial in all derivatives, power of y′′′ is 1.
Final Answer: order 3, degree 1.
Example 2: Clear the root first
Find the order and degree of y′′=1+(y′)2.
Solution:
Clear the radical: square both sides: (y′′)2=1+(y′)2 — now polynomial in derivatives.
Read off: order 2; power of y′′ is 2.
Final Answer: order 2, degree 2.
Takeaway: Roots and fractions of derivatives must be cleared before reading the degree — but a sin(y′) can never be cleared; that stays "not defined".
Example 3: Verification with a product
Verify that y=xsin3x is a solution of dx2d2y+9y−6cos3x=0.
Example 4: A two-parameter damped-oscillation family
Verify that y=c1eaxcosbx+c2eaxsinbx (c1,c2 arbitrary) solves dx2d2y−2adxdy+(a2+b2)y=0.
Solution:
First derivative:y′=eax[(bc2+ac1)cosbx+(ac2−bc1)sinbx].
Second derivative: differentiating again multiplies in another mix of a's and b's.
Substitute and collect: the coefficients of both cosbx and sinbx cancel identically, giving L.H.S. =eax⋅0=0. ✓
Final Answer: Verified — and with two arbitrary constants matching order 2, this family is the general solution.
Example 5: Reading the constants
Without solving, state how many arbitrary constants appear in (i) the general solution of y′′−2ay′+(a2+b2)y=0, and (ii) any particular solution of it.
Solution:
(i): order 2 → general solution has 2 arbitrary constants (visible as c1,c2 in Example 4).
(ii): particular solutions have 0 arbitrary constants, by definition.
Final Answer: (i) 2; (ii) 0.
Batch 2 — Variables Separable (Easy-Medium)
Example 6: A one-line separation
Solve dxdy=(1+y2)ex.
Solution:
Separate:1+y2dy=exdx.
Integrate:tan−1y=ex+C.
Final Answer:tan−1y=ex+C.
Example 7: A logarithmic disguise
Find the particular solution of log(dxdy)=3x+4y, given y=0 when x=0.
Solution:
Exponentiate:dxdy=e3x+4y=e3xe4y — separable.
Separate and integrate:∫e−4ydy=∫e3xdx gives −4e−4y=3e3x+C, i.e. 4e3x+3e−4y+12C=0.
Apply (0,0):4+3+12C=0, so 12C=−7.
Final Answer:4e3x+3e−4y−7=0.
Example 8: Exponential of the unknown
Solve dxdy=x3e−y.
Solution:
Separate:eydy=x3dx.
Integrate:ey=4x4+C.
Final Answer:ey=4x4+C, i.e. y=log(4x4+C).
Example 9: Bacterial growth
In a culture the bacteria count is 1,00,000 and increases by 10% in 2 hours. If the growth rate is proportional to the count, in how many hours will the count reach 2,00,000?
Solution:
Model:dtdN=kN gives N=N0ekt with N0=1,00,000.
Use the 10% data:1,10,000=N0e2k, so e2k=1011, i.e. k=21log1011.
Doubling:2=ekt gives t=klog2.
Final Answer:t=log10112log2 hours.
Example 10: The inflating balloon
A spherical balloon's volume changes at a constant rate. Its radius is 3 units initially and 6 units after 3 seconds. Find the radius after t seconds.
Solution:
Model:dtdV=k with V=34πr3, so 4πr2dtdr=k.
Separate and integrate:34πr3=kt+C — i.e. r3 is linear in t: r3=at+b.
Fit the data:r(0)=3 gives b=27; r(3)=6 gives 216=3a+27, so a=63.
Takeaway: The original equation was alreadyd[y(1+x2)]=cotxdx — recognising exact left sides skips the whole I.F. computation.
Example 19: Linear in x with an inverse-trig drive
Solve (tan−1y−x)dy=(1+y2)dx.
Solution:
Reorient:dydx+1+y2x=1+y2tan−1y — linear in x with P1=1+y21.
I.F.:etan−1y.
Solve (substitute t=tan−1y in the integral): xetan−1y=∫tetdt+C=et(t−1)+C.
Divide:
Final Answer:x=(tan−1y−1)+Ce−tan−1y.
Example 20: Particular solution with matching arctangents
Solve (1+x2)dxdy+2xy=1+x21, given y=0 when x=1.
Solution:
Standardise:P=1+x22x; I.F. =1+x2.
Solve:y(1+x2)=∫1+x2dx+C=tan−1x+C.
Apply (1,0):0=4π+C, so C=−4π.
Final Answer:y(1+x2)=tan−1x−4π.
Batch 5 — Curves and Mixed Problems (Medium-Hard)
Example 21: Curve through the origin
Find the equation of the curve through the origin whose tangent slope at (x,y) equals the sum of the coordinates.
Solution:
Translate:dxdy=x+y, i.e. dxdy−y=x — linear, I.F. =e−x.
Solve:ye−x=∫xe−xdx+C=−(x+1)e−x+C, so y=−(x+1)+Cex.
Apply (0,0):0=−1+C, so C=1.
Final Answer:y=ex−x−1, i.e. x+y+1=ex.
Example 22: A worded slope condition
Find the equation of the curve through (0,2), given that the sum of the coordinates of any point exceeds the magnitude of the tangent slope there by 5.
Solution:
Translate:x+y=dxdy+5, i.e. dxdy−y=x−5 — linear, I.F. =e−x.
Solve:ye−x=∫(x−5)e−xdx+C=−(x−4)e−x+C, so y=4−x+Cex.
Apply (0,2):2=4+C, so C=−2.
Final Answer:y=4−x−2ex.
Example 23: A product-rule left side
Solve xdxdy+y=xlogx (for x>0).
Solution:
Recognise the exact form: the left side is dxd(xy).
Integrate:xy=∫xlogxdx+C — by parts: 2x2logx−4x2+C.
Takeaway: With the four-entry I.F. speed-table (tanx→secx, cotx→sinx, xa→xa, constant k→ekx), problems like this compress to three written lines — full marks, minimal ink.
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