2021 SAJC H3 Physics Solution
Uploaded by hima Β· 3 June 2023
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Text from the first pagesQ1 (a) 4u(2000) = (4u+12u)Vcm Vcm= (4/16)2000 = 500 m/s [1] (b) [1] ππΌ,ππ = 2000 β 500 = 1500 ππ β1 [1] sin(πΌ) 500 = sin(30) 1500 , πΌ = 9.59π, total = 39.59 from horizontal ππΌ,πΏππ = β15002 + 5002 β 2 π₯ 1500π₯500π₯πππ (180 β 9.59 β 30) = 1912 ππ β1 [2] (c) ππΆ,ππ = 0 β 500 = β500 ππ β1 [1] Angle between C and Vcm= 180-39.6-(180-39.6)/2 =70.2o (opposite side of alpha) ππΆ,πππ = β5002 + 5002 β 2π₯500π₯500 cos(39.59) = 338.7 ππ β1 [2] Q2 (a) Let mass = M = ππ(4π 2 β π 2) = 3πππ 2 Circular sheet can be taken as a complete disc with density of π and radius 2R (mass of 4M/3), superimposed with a disc of R with density of β π or mass of -M/3 [1] 30 1500 500 1500 39.59 30 ππΌ,πΏππ =1912 500 VC, lab 500 500
X-position of CM = at vertical mid-line of circular disc Y-position of CM: Y = [(4π 3 )2π β(π 3 )3π ] π = 5π 3 from bottom of circular sheet. [1] (b) (i) Path shows normal projectile/parabolic path of the CM with loops in the forward direction. [1] The separation of the loops in the x-directions are equal. [1] The separation of the loops in the y-direction are closer nearer the top. [1] (ii) The horizontal position x= 22.6cos(45)t+(7R/3)sin(wt). The vertical position y= 22.6sin(45)t +(7R/3)cos(wt) + 5R/3- Β½ .9.81 t2 [1] Time of flight can be estimated by ignoring the 2nd and 3rd term y which are much smaller in magnitude Estimated time of flight = 2x 22.6sin(45) /9.81 = 3.3 s or 1.65 s to the highest point [1] The horizontal velocity is 22.6 cos(45) + 7π (5π) cos(5ππ‘) /3 = 16+21.98cos(5ππ‘) [1] Move backwards means horizontal velocity < 0 Solving for 16+21.98cos(5ππ‘) < 0, for t values less than 1.65 s, T = 0.4 gives t = 0.152s, 0.152+0.4=0.552, 0.552+0.4=0.952, 0.952+0.4=1.35, 1.35+0.4=1.75 (exceed) So the outer most edge moves back 4 times before reaching the top [1] (iii) At t = 0.152 s, vertical velocity = 22.6sin(45) -(7Rw/3)sin(wt) -9.81 t = 16 -15.08 -2.43 m/s = -1.51 m/s [1] Q3 (a)(i) Speed at start = 2x3.14x1.496x1011/3.256x107=29768 m/s Speed of venus orbit = 2x3.14 x 0.7233x1.496x1011/1.941x107= 35009 m/s [1] Semi-major axis of transfer orbit = (1+0.7233)/2 AU = 1.289 x 1011 m [1]
πΊππ π2 = ππ ( 4π2 π2 ) , πΊπ = 4π2π3 π2 = 1.326 π₯1020 At start of transfer 1 2 ππ£πΈ 2 β πΊππ 1.496π₯ 1011 = β πΊππ 2π₯1.289π₯1011 π£πΈ = β2πΊπ ( 1 1.497π₯1011 β 1 1.289π₯1011) = 27276 m/s Reduction of speed at LEO = 29768 β 27276 = 2490 m/s [1] At destination: 1 2 ππ£π 2 β πΊππ 0.7233π₯1.496π₯ 1011 = β πΊππ 2π₯1.289π₯1011 VV = 37711 m/s, Reduction in speed at venus orbit = 37711 -35009 = 2700 m/s [1] (b) Transfer time = 1 2 β4π2π3 πΊπ = 1 2 β4π₯3.142π₯(1.289π₯1011)3 β(πΊπ) =1.26x107s = 146 days [1] (c) Venus turn through angle of 360x(1.26x107/1.941 x 107) = 233.7 [1] Spacecraft from Earth turns through 180 degree Angle between Earth-Venus at start = 233.7 -180 = 53.7o [1] 4 (a) ππ = πΈ (1 β exp (β π‘ π πΆ)) πΈ 2 = πΈ (1 β exp (β π‘ π πΆ)) Simplifies to t = RC ln(2) [2] (b) (i) Effective inductance = 2L + 2M [1] π = 1 2πβ(2πΏ+2π)πΆ [1] (ii) (2πΏ + 2π) ( ππΌ ππ‘) + πΌπ + π πΆ = 0 [1] (2πΏ + 2π) ( π2π ππ‘2) + π ( ππ ππ‘) + π πΆ = 0
Substitute π = ππ exp(βπΎπ‘) sin (ππ‘ + π) into above equation: [1] Group terms in cos: πΎ = π 2(2πΏ+2π) [1] Group terms in sin: πΎ2 β π2 β π 2πΏ+2π πΎ + 1 (2πΏ+2π)πΆ = 0 π = β 1 (2πΏ+2π)πΆ β π 2 4(2πΏ+2π)2 [1] 5(a) E=Β½ CV2= 1 2 πππ΄ π π2 [1] = 6.91 x 10-7 J [1] (b) πΈ = 1 2 πππ΄ π π2 β 1 π , new E = 6.91 x 10-7/2 = 3.45 x 10-7J [1] Less energy stored. Work done by hand and energy lost by capacitor because charge flows back to charge battery. [1] (c) Energy = Β½ Q2/C = Β½ (CoV)/( Co/2) = 1.38 x 10-6J [1] The increase in energy is accounted for by the work done in pulling the capacitor plates. [1] (d) Energy stored decrease because of higher capacitance [1] Energy stored reduces because work is done by the capacitor plates to attract the dielectric into the plates. [1] (Work has to be done to pull out the dielectric, to restored back the energy stored in the capacitor) (6)(a)(i) The wavelength of sound sent out by siren = c/f The speed of sound relative to the observer = u + c Frequency heard by observer = (u+c)/(c/f) = (u+c)f/c [2] (ii)As the motorcyclist if far away from the siren, its velocity is almost parallel to the velocity of sound and add on to it. So the observed frequency is higher than f by (c+u)f/c [1] As the motorcyclist approaches the siren, the component of velocity in the direction of the wave becomes smaller π’πππ (π), π€βπππ π is the angle between the original direction and the current position. So the frequency is now (c+ π’πππ (π)π/π, which decreases as π increase [1] As π becomes 90, the observed frequency drops to f. [1] As π increase beyond 90, the relative speed decrease to c-| π’πππ (π)|, so the frequency decrease till (c-u)f/c [1]
(b) In unit time, if the source is moving with a speed vs, the f waves occupy a distance of (c- vs), so the wavelength is now shorter in value, given by (c- vs)/f. [1] The speed of sound remains the same. So the observed frequency = c/[(c- vs)/f] or π πβπ£π π [1] (c) Answer: ππ = π+π’ πβπ£π f (d) The velocity of air relative to ground = vw Velocity of sound sound relative to air = c Therefore velocity of sound wave relative to ground = vw+ c [1] So have to replace c by vw+ c in the expression in part (c) [1] (e) π«π π = ππβπ π = [( π πβππ )πβπ] π = π πβππ π β π = (π + ππ π + ππππππ πππππ) β π = ππ π [1] (ii) πΏπ π = π£ π = 2ππ ππ [1] Or π = 2ππ ππ π . The side moving towards Earth will have f+ πΏπ, and the side moving away from the Earth has π β πΏπ [1] (iii) Volume = 4ππ 3 3 = 2.0 π₯ 1030 1.4 π₯ 103 , R = 6.99 x 108 [1] Ξ΄f/f = 6.91 x 10-6 [1] (iv) Line width = 2Ξπ, 2ΞΞ» π = 2Ξπ π = 2π£ π = 8 π₯ 10β5, [1] v = 12000 m/s =β3ππ π , T = 5800 K [1] 7(a) Take pivot at contact point: πππ π = 2π 3π , πππ = 2π/3 [1] (b) Take contact as pivot, πΌ = πππ 2π = 2π 3 2π = π 3π = 13.3a [2] (if take CM as pivot, πΌ = πβ2π 3 π = π 3π) (c) 2Mg -T = 2Ma force equation for M [1] T + f β Mg sin(30) = M(2a/3) force equation for yoyo [1]
(d) Net torque about centre of mass = I x angular acceleration [1] Tr β 2fr = Mr2(a/(3r)) [1] (e) Solving 3 equations T =16 Mg/23 = 0.696 Mg a = 15g/23 = 0.652 g f = 51Mg/46 = 0.239 Mg [3] (f) f = ππππππ (30) [1] π = 11 23β3 = 0.276 [1] (g) πΌ = π 3π = 0.652π 3π = 85.3 [1] π = 1 2 πΌπ‘2 = 10.7 πππ [1] (h) (i) Translational KE + rotational KE = mgh Consider centre of mass as reference: v = 2x2.5/3, π = 2.5/3π 1 2 π ( 2π₯2.5 3 ) 2 + 1 2 ππ2 ( 2.5 3π) 2 = ππβ [1] Solving gives h = 0.177 m [1] (ii) Distance travelled by centre of mass along slope = 0.177/sin(30) = 0.354 m [1] π = π£+π’ 2 π‘ = 0+2π₯2.5 3 2 π‘ , t = 0.425 s [1] (iii) Linear retardation of centre of mass = (2π₯2.5 3 ) 2 2π₯0.354 = 3.92 [1] πΌ = 3.92 2π = 3.92 0.050 = 78.4 ππππ β2 [1] Or use πΌ = Ξπ π‘ = 0β 2.5 3π₯0.025 0.425 =78.4 8(a)(i)Treat the cylinder as a summation of I flowing out of page in the outer cylinder superimposed on a current flowing into the page in the hole. The B-field due to outer cylinder inside the hole circulates in anticlockwise with magnitude that
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