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Exercise 10.5 · Q2

Q.The velocity vv, of a parachute falling vertically satisfies the equation vdvdx=g(1−v2k2)v\dfrac{dv}{dx}=g\left(1-\dfrac{v^2}{k^2}\right), where gg and kk are constants. If vv and xx are both initially zero, find vv in terms of xx.

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✓ Free question

Multiply through by k2k^2 to clear the fraction, separate variables using u=k2−v2u=k^2-v^2 (so du=−2v dvdu=-2v\,dv), integrate, and fix the constant using v=0v=0 at x=0x=0.

Step 1. Rewrite with a common denominator. vdvdx=g(k2−v2)k2 ⟹ k2v dvk2−v2=g dxv\dfrac{dv}{dx}=\dfrac{g\left(k^2-v^2\right)}{k^2}\ \Longrightarrow\ \dfrac{k^2v\,dv}{k^2-v^2}=g\,dx.

Step 2. Substitute u=k2−v2, du=−2v dvu=k^2-v^2,\ du=-2v\,dv. k2v dvu=g dx ⟹ −k22duu=g dx\dfrac{k^2v\,dv}{u}=g\,dx\ \Longrightarrow\ -\dfrac{k^2}{2}\dfrac{du}{u}=g\,dx.

Step 3. Integrate both sides. −k22ln⁡u=gx+C ⟹ −k22ln⁡(k2−v2)=gx+C-\dfrac{k^2}{2}\ln u=gx+C\ \Longrightarrow\ -\dfrac{k^2}{2}\ln\left(k^2-v^2\right)=gx+C.

Step 4. Apply v=0v=0 at x=0x=0. −k22ln⁡(k2)=C-\dfrac{k^2}{2}\ln\left(k^2\right)=C.

Step 5. Combine and solve for vv. −k22ln⁡(k2−v2)+k22ln⁡k2=gx ⟹ ln⁡k2k2−v2=2gxk2 ⟹ k2−v2=k2e−2gx/k2 ⟹ v2=k2(1−e−2gx/k2)-\dfrac{k^2}{2}\ln\left(k^2-v^2\right)+\dfrac{k^2}{2}\ln k^2=gx\ \Longrightarrow\ \ln\dfrac{k^2}{k^2-v^2}=\dfrac{2gx}{k^2}\ \Longrightarrow\ k^2-v^2=k^2e^{-2gx/k^2}\ \Longrightarrow\ v^2=k^2\left(1-e^{-2gx/k^2}\right).

✓Final answer

v=k1−e−2gx/k2v=k\sqrt{1-e^{-2gx/k^2}}

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