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EXERCISE 1.5 · Q192

Q.x=cos⁡tx=\cos t, y=emty=e^{mt}, show that (1−x2)d2ydx2−xdydx−m2y=0(1-x^2)\dfrac{d^2y}{dx^2}-x\dfrac{dy}{dx}-m^2y=0

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Given x=cos⁡tx=\cos t, y=emty=e^{mt}.

Step 1: dxdt=−sin⁡t\dfrac{dx}{dt}=-\sin t, dydt=memt\dfrac{dy}{dt}=me^{mt}, so y1=dydx=memt−sin⁡t=−memtsin⁡ty_1=\dfrac{dy}{dx}=\dfrac{me^{mt}}{-\sin t}=-\dfrac{me^{mt}}{\sin t}.

Step 2 — differentiate y1y_1 w.r.t. tt using the quotient rule: ddt(y1)=−m⋅memtsin⁡t−emtcos⁡tsin⁡2t=−memt(msin⁡t−cos⁡t)sin⁡2t\dfrac{d}{dt}(y_1)=-m\cdot\dfrac{me^{mt}\sin t-e^{mt}\cos t}{\sin^2t}=-\dfrac{me^{mt}(m\sin t-\cos t)}{\sin^2t}.

Step 3 — divide by dx/dt=−sin⁡tdx/dt=-\sin t to get y2y_2: y2=memt(msin⁡t−cos⁡t)sin⁡3ty_2=\dfrac{me^{mt}(m\sin t-\cos t)}{\sin^3t}.

Step 4 — substitute into the target, using x=cos⁡tx=\cos t so 1−x2=sin⁡2t1-x^2=\sin^2t:

(1−x2)y2=sin⁡2t⋅memt(msin⁡t−cos⁡t)sin⁡3t=memt(msin⁡t−cos⁡t)sin⁡t(1-x^2)y_2=\sin^2t\cdot\dfrac{me^{mt}(m\sin t-\cos t)}{\sin^3t}=\dfrac{me^{mt}(m\sin t-\cos t)}{\sin t} …

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