1. The acceleration of the oscillator is
directly proportional to the B1
displacement (the term displacement to be included and spelled correctly
to gain the mark).
with the acceleration always directed to a fixed / equilibrium point B1
displacement (the term displacement to be included and spelled correctly
to gain the mark).
with the acceleration always directed to a fixed / equilibrium point B1
[2]
2. (a) arrow towards centre of planet 1
(b) (i) g
= GM/R2 1
(ii) gS/gO = R2/25R2; gS = 40/25 (= 1.6 N kg–1) 2
(iii) gC/gO = R2/16R2 giving gS = 40/16 (= 2.5 N kg–1) 1
(iv) average g = (2.5 + 1.6)/2 = 2.(05) (1)
Δp.e. (= mgavR) = 3.0 × 103 × 2.05 × 2.0 × 107; = 1.2 × 1011 (J) (2) 3
Δp.e. (= mgavR) = 3.0 × 103 × 2.05 × 2.0 × 107; = 1.2 × 1011 (J) (2) 3
(c) g
= v2/r; = 4π2(5R)/T2 (2)
1.6 = 4 × 9.87 × 1.0 × 108/T2 giving T2 = 24.7 × 108 and T = 5.0 × 104 (s) (2) 4
1.6 = 4 × 9.87 × 1.0 × 108/T2 giving T2 = 24.7 × 108 and T = 5.0 × 104 (s) (2) 4
[12]
3. (a) (i) Fig.
1 : x and a in opposite directions/acceleration towards
equilibrium point/AW; (1)
Fig. 2 : proportional graph between x and a/AW (1) 2
Figures not identified max. of 1 mark
equilibrium point/AW; (1)
Fig. 2 : proportional graph between x and a/AW (1) 2
Figures not identified max. of 1 mark
(ii) a
= 4π2f2x; 50 = 4π2f2.50
× 10–3; giving f2 = 25 and f = 5.0 Hz 3
(iii) cosine
wave with initial amplitude 25 mm; decreasing amplitude; (2)
correct period of 0.2 s (for minimum of 2.5 periods); (1) 3
correct period of 0.2 s (for minimum of 2.5 periods); (1) 3
(b) (i) the acceleration towards A/centripetal
acceleration or force;
is constant 2
is constant 2
(ii) a
= v2/r; so 50 = v2/10; v2 = 500 giving v = 22.4 m s–1 3
[13]
4. (a) (i) v
= 2πrf = 2π × 0.015 × 50; = 4.7 (m s–1) 2
(ii) a
= v2/r = 4.72/0.015; = 1.5 × 103 (m s–2) ecf(a)(i) 2
(iii) the
belt tension is insufficient to provide the centripetal force; (1)
so the belt does not ‘grip’ the pulley/does not hold the belt against
the pulley/there is insufficient friction to pull/push/move the belt. (1) 2
alternative argument the belt does not ‘grip’ the pulley/there is
insufficient friction to pull/push/move the belt; because of its
inertia/insufficient to provide force for acceleration of (belt)-drum
so the belt does not ‘grip’ the pulley/does not hold the belt against
the pulley/there is insufficient friction to pull/push/move the belt. (1) 2
alternative argument the belt does not ‘grip’ the pulley/there is
insufficient friction to pull/push/move the belt; because of its
inertia/insufficient to provide force for acceleration of (belt)-drum
(b) resonance
occurs; when the natural frequency of vibration of the (1)
panel = rotational frequency of the motor (1) 2
panel = rotational frequency of the motor (1) 2
[8]