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Exercise 5.7 · Q14

Q.If y=Aemx+Benxy = Ae^{mx} + Be^{nx}, show that d2ydx2−(m+n)dydx+mny=0\frac{d^2 y}{dx^2} - (m+n)\frac{dy}{dx} + mny = 0.

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The given function y=Aemx+Benxy = Ae^{mx} + Be^{nx} is a linear combination of two exponentials. Differentiating twice and substituting into the differential equation shows that the expression simplifies to zero because the exponentials are eigenfunctions of the derivative operator, and the coefficients (m+n)(m+n) and mnmn are chosen to cancel the terms.

Why This Works: The Concept

This problem is about linear differential equations with constant coefficients. When you have a function like y=Aemx+Benxy = Ae^{mx} + Be^{nx}, each exponential term emxe^{mx} has a special property: differentiating it just multiplies it by mm. So emxe^{mx} is an eigenfunction of the derivative operator.

The differential equation d2ydx2−(m+n)dydx+mny=0\frac{d^2 y}{dx^2} - (m+n)\frac{dy}{dx} + mny = 0 is designed so that when you plug in emxe^{mx} or enxe^{nx}, the result is zero. Think of it as a "characteristic equation" (r−m)(r−n)=0(r - m)(r - n) = 0 in disguise — the numbers mm and nn are precisely the roots of r2−(m+n)r+mn=0r^2 - (m+n)r + mn = 0.

Since the differential equation is linear (no products of yy with its derivatives), if each exponential satisfies it individually, then any linear combination Aemx+BenxAe^{mx} + Be^{nx} also satisfies it. That's the core idea.

Step-by-Step Verification

1. Write down the given function and find the first derivative.

We have y=Aemx+Benxy = Ae^{mx} + Be^{nx}.

Differentiating term by term:

  • The derivative of AemxAe^{mx} is A⋅memx=AmemxA \cdot m e^{mx} = Am e^{mx}.
  • The derivative of BenxBe^{nx} is B⋅nenx=BnenxB \cdot n e^{nx} = Bn e^{nx}.

So:

dydx=Amemx+Bnenx\frac{dy}{dx} = Am e^{mx} + Bn e^{nx}

2. Find the second derivative.

Differentiate dydx\frac{dy}{dx}:

  • The derivative of AmemxAm e^{mx} is Am⋅memx=Am2emxAm \cdot m e^{mx} = Am^2 e^{mx}.
  • The derivative of BnenxBn e^{nx} is Bn⋅nenx=Bn2enxBn \cdot n e^{nx} = Bn^2 e^{nx}.

So:

d2ydx2=Am2emx+Bn2enx\frac{d^2 y}{dx^2} = Am^2 e^{mx} + Bn^2 e^{nx}

3. Build the expression we need to check.

We want to verify that:

d2ydx2−(m+n)dydx+mny=0\frac{d^2 y}{dx^2} - (m+n)\frac{dy}{dx} + mny = 0

Substitute each piece:

  • First term: d2ydx2=Am2emx+Bn2enx\frac{d^2 y}{dx^2} = Am^2 e^{mx} + Bn^2 e^{nx}
  • Second term: −(m+n)dydx=−(m+n)(Amemx+Bnenx)-(m+n)\frac{dy}{dx} = -(m+n)(Am e^{mx} + Bn e^{nx})
  • Third term: +mny=mn(Aemx+Benx)+ mny = mn(Ae^{mx} + Be^{nx})

4. Group terms by the exponential factor.

Collect all terms with emxe^{mx}:

Am2emx−(m+n)Amemx+mnAemxAm^2 e^{mx} - (m+n)Am e^{mx} + mnA e^{mx}

Factor out AemxA e^{mx}:

Aemx[m2−(m+n)m+mn]A e^{mx} \left[ m^2 - (m+n)m + mn \right]

Now simplify the bracket:

m2−(m+n)m+mn=m2−m2−mn+mn=0m^2 - (m+n)m + mn = m^2 - m^2 - mn + mn = 0

So the emxe^{mx} part contributes Aemx⋅0=0A e^{mx} \cdot 0 = 0.

5. Do the same for the enxe^{nx} terms.

Collect terms with enxe^{nx}: …

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