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A body oa mass M at rest explodes into t...

A body oa mass M at rest explodes into three pieces, two of which of mass (M/4) each are thrown- off in perpendicular directions with velocities of ` 6 ms^(-1)` and `8 ms^(-1)` respectively. The third piece will be thrown-off with a velocity of `

A

`1.5 ms^(-1)`

B

`2 ms^(-1)`

C

`5 ms^(-1)`

D

`3 ms^(-1)`

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To solve the problem step by step, we will apply the principle of conservation of momentum. ### Step 1: Understand the Problem We have a body of mass \( M \) that is initially at rest. Upon explosion, it breaks into three pieces: - Two pieces of mass \( \frac{M}{4} \) each. - One piece of mass \( \frac{M}{2} \) (since \( M - 2 \times \frac{M}{4} = \frac{M}{2} \)). The two pieces are thrown off in perpendicular directions with velocities \( 6 \, \text{m/s} \) and \( 8 \, \text{m/s} \). ### Step 2: Set Up the Conservation of Momentum Equation Since the initial momentum of the system is zero (the body is at rest), the final momentum must also equal zero: \[ \text{Initial Momentum} = \text{Final Momentum} \] \[ 0 = M_1 \vec{V_1} + M_2 \vec{V_2} + M_3 \vec{V_3} \] Where: - \( M_1 = \frac{M}{4} \), \( \vec{V_1} = 6 \, \text{m/s} \, \hat{i} \) - \( M_2 = \frac{M}{4} \), \( \vec{V_2} = 8 \, \text{m/s} \, \hat{j} \) - \( M_3 = \frac{M}{2} \), \( \vec{V_3} \) is unknown. ### Step 3: Write the Momentum Vectors Substituting the values into the momentum equation: \[ 0 = \left(\frac{M}{4} \cdot 6 \hat{i}\right) + \left(\frac{M}{4} \cdot 8 \hat{j}\right) + \left(\frac{M}{2} \vec{V_3}\right) \] This simplifies to: \[ 0 = \frac{6M}{4} \hat{i} + \frac{8M}{4} \hat{j} + \frac{M}{2} \vec{V_3} \] ### Step 4: Simplify the Equation Now, we can simplify the equation: \[ 0 = \frac{3M}{2} \hat{i} + 2M \hat{j} + \frac{M}{2} \vec{V_3} \] ### Step 5: Isolate \( \vec{V_3} \) Rearranging gives: \[ \frac{M}{2} \vec{V_3} = -\frac{3M}{2} \hat{i} - 2M \hat{j} \] Dividing through by \( \frac{M}{2} \) (assuming \( M \neq 0 \)): \[ \vec{V_3} = -3 \hat{i} - 4 \hat{j} \] ### Step 6: Calculate the Magnitude of \( \vec{V_3} \) To find the magnitude of \( \vec{V_3} \): \[ |\vec{V_3}| = \sqrt{(-3)^2 + (-4)^2} = \sqrt{9 + 16} = \sqrt{25} = 5 \, \text{m/s} \] ### Conclusion The third piece will be thrown off with a velocity of \( 5 \, \text{m/s} \). ---

To solve the problem step by step, we will apply the principle of conservation of momentum. ### Step 1: Understand the Problem We have a body of mass \( M \) that is initially at rest. Upon explosion, it breaks into three pieces: - Two pieces of mass \( \frac{M}{4} \) each. - One piece of mass \( \frac{M}{2} \) (since \( M - 2 \times \frac{M}{4} = \frac{M}{2} \)). The two pieces are thrown off in perpendicular directions with velocities \( 6 \, \text{m/s} \) and \( 8 \, \text{m/s} \). ...
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Knowledge Check

  • A body of mass M at rest explodes into three pieces, two of which of mass M//4 each are thrown off in prependicular directions eith velocities of 3//s and 4m//s respectively. The third piece willl be thrown off with a velocity of

    A
    `1.5m//s`
    B
    `2.0m//s`
    C
    `2.5m//s`
    D
    `3.0m//s`
  • A body of mass M at rest explodes into 3 pieces, A,B and C of masses M/4,M/4 and M/2 respectively. A and B move in perpendicular directions with velocities 5m/s and 12 m/s respectively. What is the speed of the third piece?

    A
    3.5m/s
    B
    5.5m/s
    C
    6.5m/s
    D
    8m/s
  • A body of mass 4m at rest explodes into three fragments. Two of the fragments each of mass m move with speed v in mutually perpendicular directions. Total energy released in the process is

    A
    `mv^2`
    B
    `3/2 mv^2`
    C
    `2mv^2`
    D
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