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A bullet fired into a fixed target loses...

A bullet fired into a fixed target loses half of its velocity after penetrating 3cm. How much further it will penetrate before coming to rest assuming that it faces constant resistance to motion?

A

(a) 2.0cm

B

(b) 3.0cm

C

(c) 1.0cm

D

(d) 1.5cm

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The correct Answer is:
To solve the problem, we will apply the work-energy theorem, which states that the work done on an object is equal to the change in its kinetic energy. ### Step-by-Step Solution: 1. **Understanding the Initial Conditions**: - Let the initial velocity of the bullet be \( V \). - After penetrating 3 cm into the target, the bullet's velocity reduces to \( \frac{V}{2} \). 2. **Applying the Work-Energy Theorem**: - The work done by the resistive force \( F \) while the bullet penetrates the target can be expressed as: \[ W = F \cdot S \] - The change in kinetic energy as the bullet penetrates 3 cm (0.03 m) is given by: \[ \Delta KE = KE_{\text{initial}} - KE_{\text{final}} = \frac{1}{2} m V^2 - \frac{1}{2} m \left(\frac{V}{2}\right)^2 \] - Simplifying the kinetic energy change: \[ \Delta KE = \frac{1}{2} m V^2 - \frac{1}{2} m \frac{V^2}{4} = \frac{1}{2} m V^2 \left(1 - \frac{1}{4}\right) = \frac{1}{2} m V^2 \cdot \frac{3}{4} = \frac{3}{8} m V^2 \] 3. **Setting Up the Equation for Work Done**: - The work done by the resistive force over the distance \( S_1 = 3 \, \text{cm} = 0.03 \, \text{m} \) is: \[ W = F \cdot S_1 = F \cdot 0.03 \] - According to the work-energy theorem: \[ F \cdot 0.03 = \frac{3}{8} m V^2 \] - Rearranging gives: \[ F = \frac{3 m V^2}{8 \cdot 0.03} \] 4. **Finding Further Penetration**: - Now, we need to find how much further the bullet penetrates before coming to rest. Let this additional distance be \( S_2 \). - The initial velocity for this phase is \( \frac{V}{2} \) and the final velocity is 0. - The change in kinetic energy for this phase is: \[ \Delta KE = \frac{1}{2} m \left(\frac{V}{2}\right)^2 - 0 = \frac{1}{2} m \frac{V^2}{4} = \frac{1}{8} m V^2 \] - The work done while penetrating \( S_2 \) is: \[ W = F \cdot S_2 \] - Setting the work done equal to the change in kinetic energy gives: \[ F \cdot S_2 = \frac{1}{8} m V^2 \] 5. **Relating the Two Work Equations**: - From the first part, we have \( F = \frac{3 m V^2}{8 \cdot 0.03} \). - Substitute \( F \) into the second equation: \[ \frac{3 m V^2}{8 \cdot 0.03} \cdot S_2 = \frac{1}{8} m V^2 \] - Cancel \( m V^2 \) from both sides: \[ \frac{3 S_2}{8 \cdot 0.03} = \frac{1}{8} \] - Rearranging gives: \[ 3 S_2 = 0.03 \quad \Rightarrow \quad S_2 = \frac{0.03}{3} = 0.01 \, \text{m} = 1 \, \text{cm} \] 6. **Final Answer**: - The bullet will penetrate an additional distance of **1 cm** before coming to rest.

To solve the problem, we will apply the work-energy theorem, which states that the work done on an object is equal to the change in its kinetic energy. ### Step-by-Step Solution: 1. **Understanding the Initial Conditions**: - Let the initial velocity of the bullet be \( V \). - After penetrating 3 cm into the target, the bullet's velocity reduces to \( \frac{V}{2} \). ...
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