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Question: A ball is thrown vertically upwards. It was observed at a height $h$ twice with a time interval $\De...

A ball is thrown vertically upwards. It was observed at a height hh twice with a time interval Δt\Delta t. The initial velocity of the ball is

A

8gh+g2(Δt)2\sqrt{8gh+g^2(\Delta t)^2}

B

8gh+(gΔt2)2\sqrt{8gh+(\frac{g\Delta t}{2})^2}

C

128gh+g2(Δt)2\frac{1}{2}\sqrt{8gh+g^2(\Delta t)^2}

D

8gh+4g2(Δt)2\sqrt{8gh+4g^2(\Delta t)^2}

Answer

(C) 128gh+g2(Δt)2\frac{1}{2}\sqrt{8gh+g^2(\Delta t)^2}

Explanation

Solution

The motion of a ball thrown vertically upwards is governed by the equation of motion under constant acceleration due to gravity. Let the initial velocity of the ball be uu, the height be hh, and the acceleration due to gravity be gg. We take the upward direction as positive, so the acceleration is g-g.

The equation relating displacement (hh), initial velocity (uu), time (tt), and acceleration (g-g) is:

h=ut12gt2h = ut - \frac{1}{2}gt^2

Rearrange this equation into a standard quadratic form in terms of time tt:

12gt2ut+h=0\frac{1}{2}gt^2 - ut + h = 0

Multiply by 2 to clear the fraction:

gt22ut+2h=0gt^2 - 2ut + 2h = 0

Let t1t_1 and t2t_2 be the two instants of time when the ball is at height hh. These are the two roots of the quadratic equation. According to Vieta's formulas for a quadratic equation at2+bt+c=0at^2 + bt + c = 0, the sum of the roots (t1+t2t_1 + t_2) and the product of the roots (t1t2t_1 t_2) are given by:

Sum of roots: t1+t2=(2u)g=2ugt_1 + t_2 = -\frac{(-2u)}{g} = \frac{2u}{g}

Product of roots: t1t2=2hgt_1 t_2 = \frac{2h}{g}

We are given that the time interval between the two observations at height hh is Δt\Delta t. Assuming t2>t1t_2 > t_1, we have:

t2t1=Δtt_2 - t_1 = \Delta t

Now we use the algebraic identity that relates the sum, difference, and product of two numbers:

(t2+t1)2(t2t1)2=4t1t2(t_2 + t_1)^2 - (t_2 - t_1)^2 = 4t_1 t_2

Substitute the expressions for the sum, difference, and product of t1t_1 and t2t_2 into this identity:

(2ug)2(Δt)2=4(2hg)(\frac{2u}{g})^2 - (\Delta t)^2 = 4(\frac{2h}{g})

4u2g2(Δt)2=8hg\frac{4u^2}{g^2} - (\Delta t)^2 = \frac{8h}{g}

Now, we need to solve for uu:

4u2g2=8hg+(Δt)2\frac{4u^2}{g^2} = \frac{8h}{g} + (\Delta t)^2

To isolate u2u^2, multiply both sides by g2g^2:

4u2=g2(8hg+(Δt)2)4u^2 = g^2(\frac{8h}{g} + (\Delta t)^2)

4u2=8hg+g2(Δt)24u^2 = 8hg + g^2(\Delta t)^2

Divide by 4:

u2=8hg+g2(Δt)24u^2 = \frac{8hg + g^2(\Delta t)^2}{4}

u2=14(8hg+g2(Δt)2)u^2 = \frac{1}{4}(8hg + g^2(\Delta t)^2)

Take the square root of both sides to find uu:

u=14(8hg+g2(Δt)2)u = \sqrt{\frac{1}{4}(8hg + g^2(\Delta t)^2)}

u=128hg+g2(Δt)2u = \frac{1}{2}\sqrt{8hg + g^2(\Delta t)^2}

Comparing this result with the given options, it matches option (C).