Question:

An object at rest suddenly explodes into three parts of equal masses. Two of the away at right angles to each other with equal speed of 10 m/s. The speed of the just after the explosion will be: 

Updated On: Apr 7, 2025
  •  10 m/s

  •  20 m/s

  •  2\(\sqrt{10}\) m/s

  •  0

  •  10√2 m/s

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Approach Solution - 1

Given:

  • An object at rest explodes into three equal masses (\( m \)).
  • Two parts move at right angles with speed \( 10 \, \text{m/s} \) each.

Step 1: Momentum Conservation

Initial momentum = 0 (object at rest).

Let the third part have velocity \( \vec{v}_3 \). Momentum conservation requires:

\[ \vec{p}_1 + \vec{p}_2 + \vec{p}_3 = 0 \]

Given \( \vec{p}_1 = m \cdot 10 \, \hat{i} \) and \( \vec{p}_2 = m \cdot 10 \, \hat{j} \), the third momentum must satisfy:

\[ \vec{p}_3 = -(\vec{p}_1 + \vec{p}_2) = -m (10 \, \hat{i} + 10 \, \hat{j}) \]

Thus, the speed of the third part is:

\[ v_3 = \sqrt{10^2 + 10^2} = 10\sqrt{2} \, \text{m/s} \]

The speed of the third part is \( 10\sqrt{2} \, \text{m/s} \).

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Approach Solution -2

1. Apply the principle of conservation of momentum:

Since the object is initially at rest, the total momentum before the explosion is zero. The total momentum after the explosion must also be zero. Momentum is a vector quantity.

2. Set up the momentum equations:

Let the three parts have equal mass m. Let the velocities of the first two parts be \(v_1 = 10\hat{i}\) m/s and \(v_2 = 10\hat{j}\) m/s (since they move at right angles to each other with equal speeds). Let the velocity of the third part be \(v_3\). The conservation of momentum equation is:

\[mv_1 + mv_2 + mv_3 = 0\]

Since the masses are equal, we can simplify:

\[v_1 + v_2 + v_3 = 0\]

3. Solve for the velocity of the third part:

\[v_3 = -(v_1 + v_2) = -(10\hat{i} + 10\hat{j}) = -10\hat{i} - 10\hat{j}\]

4. Calculate the speed of the third part:

The speed is the magnitude of the velocity vector:

\[|v_3| = \sqrt{(-10)^2 + (-10)^2} = \sqrt{100 + 100} = \sqrt{200} = 10\sqrt{2} \, \text{m/s}\]

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Concepts Used:

Conservation of Energy

In physics and chemistry, the law of conservation of energy states that the total energy of an isolated system remains constant; it is said to be conserved over time.

It also means that energy can neither be created nor destroyed; rather, it can only be transformed or transferred from one form to another. For instance, chemical energy is converted to kinetic energy when a stick of dynamite explodes.

So, mathematically we can represent the law of energy conservation as the following,

The amount of energy spent in a work = The amount of Energy gained in the related work

Now, the derivation of the energy conservation formula is as followed,

Ein − Eout = Δ Esys

We know that the net amount of energy which is transferred in or out of any system is mainly seen in the forms of heat (Q), mass (m) or work (W). Hence, on re-arranging the above equation, we get,

Ein − Eout = Q − W

Now, on dividing all the terms into both the sides of the equation by the mass of the system, the equation represents the law of conservation of energy on a unit mass basis, such as

Q − W = Δ u

Thus, the conservation of energy formula can be written as follows,

Q – W = dU / dt

Here,

Esys = Energy of the system as a whole

Ein = Incoming energy

Eout = Outgoing energy

E = Energy

Q = Heat

M = Mass

W = Work

T = Time