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5. When is this equation valid? (1 + ε) ~ 1 + n ε A) For massless particles, but not massive B) For large values ofn C) For
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Answer #1

5) C (in time dilation we used this because we have \sqrt{1 -v\: ^{2}/c^{2}} in the denominator)

6) E (every quantity will increase)

7) C (in this condition denominator becomes imaginary that's why we take \gamma = 1)

8) B (we can see the object in x - direction )

9) E (by using velocity addition we can find it is c)

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