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Question: A particle of mass m is dropped from a height h above the ground. At the same time another particle ...

A particle of mass m is dropped from a height h above the ground. At the same time another particle of the same mass is thrown vertically upwards from the ground with a speed of 2gh\sqrt{2gh}. If they collide head-on completely inelastically, the time taken for the combined mass to reach the ground, in units of hg\sqrt{\frac{h}{g}} is:

A

12\frac{1}{2}

B

12\frac{1}{\sqrt{2}}

C

43\sqrt{\frac{4}{3}}

D

23\sqrt{\frac{2}{3}}

Answer

None of the options are correct. The calculated value is 32\sqrt{\frac{3}{2}}

Explanation

Solution

To solve this problem, we need to follow these steps:

  1. Determine the time and position of the collision.
  2. Calculate the velocities of both particles just before the collision.
  3. Apply the principle of conservation of momentum to find the velocity of the combined mass immediately after the inelastic collision.
  4. Calculate the time taken for the combined mass to reach the ground from the collision point.

Let's set up a coordinate system with the ground as the origin (y=0y=0) and the upward direction as positive. The acceleration due to gravity is a=ga = -g.

Step 1: Time and position of collision

  • Particle 1 (dropped from height h):
    Initial position y1,0=hy_{1,0} = h
    Initial velocity u1=0u_1 = 0
    Position at time tt: y1(t)=h12gt2y_1(t) = h - \frac{1}{2}gt^2

  • Particle 2 (thrown vertically upwards from ground):
    Initial position y2,0=0y_{2,0} = 0
    Initial velocity u2=2ghu_2 = \sqrt{2gh}
    Position at time tt: y2(t)=(2gh)t12gt2y_2(t) = (\sqrt{2gh})t - \frac{1}{2}gt^2

Let tct_c be the time of collision and ycy_c be the height of collision. At collision, y1(tc)=y2(tc)y_1(t_c) = y_2(t_c):

h12gtc2=(2gh)tc12gtc2h - \frac{1}{2}gt_c^2 = (\sqrt{2gh})t_c - \frac{1}{2}gt_c^2
h=(2gh)tch = (\sqrt{2gh})t_c
tc=h2gh=h2gh=h2g=h2gt_c = \frac{h}{\sqrt{2gh}} = \frac{h}{\sqrt{2}\sqrt{g}\sqrt{h}} = \frac{\sqrt{h}}{\sqrt{2g}} = \sqrt{\frac{h}{2g}}

Now, calculate the height of collision ycy_c:

yc=h12gtc2=h12g(h2g)2=h12g(h2g)=hh4=3h4y_c = h - \frac{1}{2}gt_c^2 = h - \frac{1}{2}g\left(\sqrt{\frac{h}{2g}}\right)^2 = h - \frac{1}{2}g\left(\frac{h}{2g}\right) = h - \frac{h}{4} = \frac{3h}{4}

So, the collision occurs at a height of 3h4\frac{3h}{4} from the ground.

Step 2: Velocities just before collision

  • Velocity of Particle 1 (v1v_1) just before collision: (downward is negative)
    v1=u1+atc=0gtc=gh2g=g2h2g=gh2v_1 = u_1 + at_c = 0 - gt_c = -g\sqrt{\frac{h}{2g}} = -\sqrt{\frac{g^2h}{2g}} = -\sqrt{\frac{gh}{2}}

  • Velocity of Particle 2 (v2v_2) just before collision: (upward is positive)
    v2=u2+atc=2ghgtc=2ghgh2gv_2 = u_2 + at_c = \sqrt{2gh} - gt_c = \sqrt{2gh} - g\sqrt{\frac{h}{2g}}
    v2=2ghg2h2g=2ghgh2v_2 = \sqrt{2gh} - \sqrt{\frac{g^2h}{2g}} = \sqrt{2gh} - \sqrt{\frac{gh}{2}}
    We can write 2gh=4gh2=2gh2\sqrt{2gh} = \sqrt{4 \cdot \frac{gh}{2}} = 2\sqrt{\frac{gh}{2}}.
    So, v2=2gh2gh2=gh2v_2 = 2\sqrt{\frac{gh}{2}} - \sqrt{\frac{gh}{2}} = \sqrt{\frac{gh}{2}}

Step 3: Velocity of combined mass after inelastic collision

Since the collision is completely inelastic, the two particles stick together and move as a single combined mass (m+m=2mm+m=2m). Let VV be the common velocity after collision. By conservation of momentum:

m1v1+m2v2=(m1+m2)Vm_1v_1 + m_2v_2 = (m_1+m_2)V
m(gh2)+m(gh2)=(m+m)Vm\left(-\sqrt{\frac{gh}{2}}\right) + m\left(\sqrt{\frac{gh}{2}}\right) = (m+m)V
0=2mV0 = 2mV
V=0V = 0

The combined mass momentarily comes to rest immediately after the collision.

Step 4: Time taken for the combined mass to reach the ground

The combined mass is at height yc=3h4y_c = \frac{3h}{4} and its initial velocity after collision is V=0V=0. It will now fall freely under gravity.
Let tft_f be the time taken for the combined mass to reach the ground from this point.
Using the equation of motion y=y0+v0t+12at2y = y_0 + v_0t + \frac{1}{2}at^2: (taking ground as y=0y=0 and upward as positive, a=ga=-g)

0=yc+Vtf+12(g)tf20 = y_c + V t_f + \frac{1}{2}(-g)t_f^2
0=3h4+0tf12gtf20 = \frac{3h}{4} + 0 \cdot t_f - \frac{1}{2}gt_f^2
12gtf2=3h4\frac{1}{2}gt_f^2 = \frac{3h}{4}
gtf2=3h2gt_f^2 = \frac{3h}{2}
tf2=3h2gt_f^2 = \frac{3h}{2g}
tf=3h2gt_f = \sqrt{\frac{3h}{2g}}

The question asks for the time in units of hg\sqrt{\frac{h}{g}}.

tf=32hgt_f = \sqrt{\frac{3}{2}} \sqrt{\frac{h}{g}}

The value is 32\sqrt{\frac{3}{2}}.

Upon comparing this result with the given options:

(1) 12\frac{1}{2} (2) 12\frac{1}{\sqrt{2}} (3) 43\sqrt{\frac{4}{3}} (4) 23\sqrt{\frac{2}{3}}

None of the options exactly match 32\sqrt{\frac{3}{2}}. This indicates a potential error in the question's options. However, if forced to choose the closest, 321.224\sqrt{\frac{3}{2}} \approx 1.224 and 431.154\sqrt{\frac{4}{3}} \approx 1.154. But this is not a valid method for exact science problems. Based on the rigorous derivation, the value is 32\sqrt{\frac{3}{2}}.