FOLLOW US ON TWITTER
SHARE THIS PAGE ON FACEBOOK, TWITTER, WHATSAPP ... USING THE BUTTONS ON THE LEFT


YOUR PARTICIPATION FOR THE GROWTH OF PHYSICS REFERENCE BLOG

Thursday, November 23, 2017

Explain how a satellite may be in a circular orbit around a planet. The Earth and the Moon may be considered to be uniform spheres that are isolated in space.




Question 1
(a) Explain how a satellite may be in a circular orbit around a planet.                              [2]


(b) The Earth and the Moon may be considered to be uniform spheres that are isolated in space.
The Earth has radius R and mean density ρ. The Moon, mass m, is in a circular orbit about the Earth with radius nR, as illustrated in Fig. 1.1.

Fig. 1.1

The Moon makes one complete orbit of the Earth in time T.
Show that the mean density ρ of the Earth is given by the expression
ρ = 3πn3 / GT2  
[4]


(c) The radius R of the Earth is 6.38 × 103 km and the distance between the centre of the Earth and the centre of the Moon is 3.84 × 105 km.
The period T of the orbit of the Moon about the Earth is 27.3 days.
Use the expression in (b) to calculate ρ.                                                                         [3]
[Total: 9]





Reference: Past Exam Paper – June 2017 Paper 41 & 43 Q1





Solution:
(a) The gravitational force (of attraction between the satellite and the planet) provides / is the centripetal force (on the satellite about the planet)


(b)
{Density = Mass / Volume      and Volume of Earth (sphere) = (4/3) × πR3 }
Mass M = (4/3) × πR3 ρ                                         

{ω = 2 π / T                 or speed v = distance / time = circumference / period}
ω = 2π / T                  or v = 2πnR / T                    

{The gravitational force provides the centripetal force.
GMm / r2 = mrω2        or GMm / r2 = m v2 / r             where r is the radius of the orbit
The mass of the Moon m may be eliminated on both sides.
Radius of orbit r = nR

Replacing the equations for mass M and ω or v,}
GM / (nR)2 = nRω2       or v2 / nR                               

Consider GM / (nR)2 = nRω2
M = nRω2 × (nR)2  / G
M = ω2 × (n3R3 / G) 
M = ω2 × (n3R3 / G)
(4/3) × πR3 ρ= (2π / T)2 × (n3R3 / G)

substitution clear to give ρ = 3πn3 / GT2    


(c)
{ρ= 3πn3 / GT2 }
{nR = 3.84 × 105 km               and R = 6.38 × 103 km }
n = (3.84 × 105) / (6.38 × 103) = 60.19 or 60.2     
     
{T = 27.3 days = 27.3 × 24 × 3600 s}

ρ = 3π × 60.193 / [(6.67 × 10-11) × (27.3 × 24 × 3600)2]
ρ = 5.54 × 103 kg m-3                                                               

Tuesday, November 21, 2017

A ball is kicked towards goal posts from a position 20m from and directly in front of the posts.




Question 5

A ball is kicked towards goal posts from a position 20m from and directly in front of the posts. The ball takes 0.6s from the time it is kicked to pass over the cross-bar, 2.5m above the ground. The ball is at its maximum height as it passes over the cross-bar. You may ignore air resistance.
 
(a) Calculate the ball’s horizontal component of velocity. 
(b) Calculate the vertical component of the velocity of the ball immediately after it is kicked. 
(c) Determine the magnitude of the initial velocity of the ball immediately after it is kicked.
(d) Determine the angle above the horizontal at which the ball is kicked.





Reference: ???





Solution:
This is a question on projectile motion. The horizontal and vertical component can be considered independently.


(a)
There is no acceleration horizontal (as air resistance is negligible). The ball has a constant horizontal speed.
Speed = distance / time = 20 / 0.6 = 33.3 m s-1


(b)
Vertically: s = 2.5m                 t = 0.6 s           acceleration a = (-) 9.81 m s-2 u = ???
Since the ball is at its maximum point, it is n=momentarily at rest: v = 0
v2 = u2 + 2as
0 = u2 + 2 × –9.81 × 2.5          giving u = 7.0 m s-1


(c)
Component of initial velocity:


The initial velocity vi is the resultant of the 2 components.
vi2 = (33.3)2 + (7.0)2    giving vi = 34.0 m s-1


(d)
Angle θ above the horizontal = tan-1 (7/33.3) = 11.9°

Wednesday, November 15, 2017

A ball is released from rest above a horizontal surface and bounces several times. The graph shows how, for this ball, a quantity y varies with time.




Question 4
A ball is released from rest above a horizontal surface and bounces several times.
The graph shows how, for this ball, a quantity y varies with time.


What is the quantity y?
A acceleration
B displacement
C kinetic energy
D velocity





Reference: Past Exam Paper – June 2013 Paper 12 Q8





Solution:
Answer: B.
The ball is thrown from rest above a horizontal surface and it bounces several times. 

We know that the ball falls due to the acceleration due to gravity ‘g’. However, the value of g is constant (= 9.81 m s-2) and does not vary when there is no air resistance. [A is incorrect]


Consider choice B.
Let the displacement be taken from the position above the surface and take the positive direction to be downwards. The ball falls until it reaches the surface (this is the maximum displacement).

Now, the ball falls under gravity. It accelerates; that is, its speed increases. In a displacement-time graph, this is indicated by an increasing gradient. This is indeed indicated by the graph.

As it hits the surface, the ball rebounds. However, due to energy loss (in form of heat, sound …), the ball does not reach its original height. As the ball moves up, its displacement (taken from its original position above before the release) decreases but does not come to zero as the ball does not reach its original height. [B is correct]


Under careful consideration, it can be shown that ‘y’ cannot be kinetic energy nor velocity.
Currently Viewing: Physics Reference |