Download Obtain (i) the velocity and acceleration at any time, (ii)

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Woodward effect wikipedia , lookup

Coriolis force wikipedia , lookup

Centrifugal force wikipedia , lookup

Gravity wikipedia , lookup

Momentum wikipedia , lookup

Torque wikipedia , lookup

Lorentz force wikipedia , lookup

Mechanics of planar particle motion wikipedia , lookup

Velocity-addition formula wikipedia , lookup

Fictitious force wikipedia , lookup

Relativistic quantum mechanics wikipedia , lookup

Weightlessness wikipedia , lookup

Relativistic angular momentum wikipedia , lookup

Inertia wikipedia , lookup

Free fall wikipedia , lookup

Centripetal force wikipedia , lookup

Transcript
COLLEGE OF SCIENCES
DEPARTMENT OF MATHEMATICAL AND PHYSICAL SCIENCES
PHY 214 ANALYTICAL MECHANICS
2016/17 SESSION TUTORIAL QUESTIONS
(TO BE SUBMITTED ON/BEFORE THURSDAY 15TH JUNE 2017)
1.
(a)
(b)
(c)
What is rectilinear motion? Hence, for a particle traveling along the π‘₯-axis,
write the expressions which describe its (i) average velocity, (ii)
instantaneous velocity, (iii) average acceleration, and (iv) instantaneous
acceleration.
A particle’s position at any time 𝑑 is given by: π‘₯ = (2𝑑 4 + 5𝑑 2 + 3𝑑 )π‘š.
Obtain (i) the velocity and acceleration at any time, (ii) the position, the
velocity and acceleration at 𝑑 = 2𝑠 π‘Žπ‘›π‘‘ 3𝑠, and (iii) the average velocity
and average acceleration between 𝑑 = 2𝑠 π‘Žπ‘›π‘‘ 3𝑠.
If the particle in (b) above moves under the influence of a constant force 𝐹
and its initial speed is π‘‰π‘œ , show that the speed of the particle at any position
π‘₯ is given by:
2𝐹
𝑉 = βˆšπ‘‰π‘œ2 + ( ) π‘₯
π‘š
where π‘š is the mass of the particle.
2.
(a)
(b)
(c)
What is referred to as a freely falling body? Write the differential equation
from Newton’s second law for such body.
An object of mass π‘š is thrown vertically upward from the earth’s surface
with speed π‘‰π‘œ . Find (i) the position at any time, (ii) the time taken to reach
the highest point, (iii) the maximum height reached
Given that a uniform force with linear frictional damping acts on mass m in
𝑑𝑣
(b) above, such that its equation of motion is π‘š = βˆ’π‘šπ‘” βˆ’ 𝛽𝑉, show that
𝑑𝑑
the position of m at any time is:
𝛽
π‘š
π‘š
π‘š
𝑧 = (π‘‰π‘œ + 𝑔) (1 βˆ’ 𝑒 βˆ’π‘šπ‘‘ ) βˆ’ 𝑔𝑑
𝛽
𝛽
𝛽
Page 1 of 3
3.
(a)
(b)
When is a particle said to be in equilibrium?
A particle of mass π‘š is suspended in equilibrium by two inelastic strings of
lengths π‘Ž and 𝑏 which are separated by a distance 𝑐 apart as shown below.
Find the tension in each string.
4.
(a)
Show that the magnitude of centripetal acceleration of a particle undergoing
circular motion is:
𝑉2
π‘Ž=
π‘Ÿ
A particle moves so that its position vector is given by π‘Ÿβƒ— = cos πœ”π‘‘ 𝑖̂ +
βƒ—βƒ— of the particle
sin πœ”π‘‘ 𝑗̂ where πœ” is a constant. Show that (π‘Ž) the velocity 𝑉
is perpendicular to π‘Ÿβƒ—, (𝑏) the acceleration π‘Žβƒ— is directed toward the origin
βƒ—βƒ— =
and has magnitude proportional to the distance from the origin, (𝑐 ) π‘Ÿβƒ— × π‘‰
π‘Ž π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘ π‘£π‘’π‘π‘‘π‘œπ‘Ÿ.
(b)
5.
6.
(a)
(i)
(ii)
(iii)
(b)
(i)
(ii)
(a)
(b)
Describe a constrained motion?
A particle 𝑃 of mass π‘š slides without rolling down a frictionless plane
inclined at angle 𝛼. If it starts from rest at the top of the incline, find (𝑖) the
acceleration, (𝑖𝑖) the velocity, and (𝑖𝑖𝑖) the distance traveled after time 𝑑.
Suppose the incline in (b) has a coefficient of friction πœ‡. Find (i) the
acceleration, (ii) the speed, and (iii) the distance travelled by the particle
after time 𝑑.
(c)
7.
(a)
State and prove the work-energy theorem.
Under what conditions is a force field said to be conservative.
Apply the conditions in (ii) to show that
𝐹⃗ = (𝑦 2 𝑧 3 βˆ’ 6π‘₯𝑧 2 )𝑖̂ + 2π‘₯𝑦𝑧 3 𝑗̂ + (3π‘₯𝑦 2 𝑧 2 βˆ’ 6π‘₯ 2 𝑧)π‘˜Μ‚
is a conservative force field
State and prove the principle of conservation of angular momentum
βƒ—βƒ—βƒ—.
Obtain the relationship between Torque πœβƒ— and angular momentum Ξ©
The equation of motion of a simple harmonic oscillator is given by
𝑑2 π‘₯
π‘š 2 𝑖̂ = βˆ’π‘˜π‘₯𝑖̂
𝑑𝑑
Page 2 of 3
(i)
(ii)
(b)
(c)
8.
(a)
(b)
Obtain the general solution to the equation and the boundary
conditions.
Obtain the period (P) and frequency (f) of the motion.
Assuming the harmonic oscillator in (a) above has a damping force
βƒ—βƒ— acting on it. Obtain the solutions for the following cases
𝐹⃗𝐷 = βˆ’π›½π‘‰
(𝑖) Over-damped motion (𝑖𝑖) Critically damped motion, and (𝑖𝑖𝑖) Underdamped motion
Show that the system π‘₯̈ + 4π‘₯Μ‡ + 3π‘₯ = 0 is over-damped.
Distinguish between Constrained motion and Free fall motion
At time 𝑑 = 0 a parachutist having weight of magnitude π‘šπ‘” is located at
𝑧 = 0 and is travelling vertically downward with speed π‘‰π‘œ . If the force or
air resistance acting on the parachute is proportional to the instantaneous
speed, find
(𝑖) the speed at any time 𝑑 > 0,
(𝑖𝑖) the distance travelled at any time 𝑑 > 0,
(𝑖𝑖𝑖) the acceleration at any time 𝑑 > 0, and
π‘šπ‘”
(𝑖𝑣) show that the parachutist approaches a limiting speed given by
⁄𝛽.
Page 3 of 3