A particle P of mass 0.5 kg is attached to a fixed point O by a light elastic string of natural length 1 m and modulus of elasticity 16N. The particle P is projected vertically upwards from O with speed 6ms¯¹. A resisting force of magnitude 0.1x² N acts on P when P has displacement x m above O. After projection the upwards velocity of P is v m s¯¹.
- (i)Show that, before the string becomes taut, v(dv/dx) = -10 - 0.2x².[2]
- (ii)Find the velocity of P at the instant the string becomes taut.[4]
- (iii)Find an expression for the acceleration of P while it is moving upwards after the string becomes taut.[2]
- (iv)Verify that P comes to instantaneous rest before the extension of the string is 0.5 m.[4]
Mark scheme
Marking points from the official mark scheme (May/June 2019). The mark or mark type is shown in brackets.
- [M1] Use Newton's Second Law vertically
- [A1] v(dv/dx) = -10 - 0.2x²
- [M1] Attempt to integrate the expression in part (i)
- [A1] v²/2 = -10x - 0.2x³/3 + c
- [M1] Either use limits or find c and put x = 1
- [A1] v = 3.98 (329...) ms⁻¹
- [M1] Use Newton's Second Law vertically when string becomes taut
- [A1] v(dv/dx) = -10 - 0.2x² - 32x + 32 = 22 – 32x – 0.2x²
- [M1] Attempt to integrate after the string becomes taut
- [A1] v²/2 = 22x - 32x²/2 - 0.2x³/3 + k
- [M1] Either use limits or find k and put x = 1.5
- [A1] As v²/2 cannot be negative, P comes to rest before the extension of the string is 0.5.
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