Thursday, December 7, 2017

Problem Based Learning in Basic Physics - VIII



Problem Based Learning in Basic Physics - VIII

 

                                                       A. K .Mody

C-14 Beverly Hills, Lam Road, Devlali, Nashik 422401, Maharashtra


H. C. Pradhan

HBCSE, TIFR, V. N. Purav Marg, Mankhurd
Mumbai – 400 088


[In this article- eighth in the series of articles we present problems for a problem based learning course based on dimensional analysis. We present the technique of dimensional analysis in the area of basic physics and what each problem tries to achieve with its solution. ]

The dimensions of physical quantity are the powers (or exponents) to which the base quantities are raised to represent that quantity.2

The applications of dimensional analysis are
1.      Checking the dimensional consistency of equations.
2.      Deducing relations among physical quantities.
The limitation of this is we cannot relate number of quantities that may result in number of equations less than number of unknowns. Thus number of quantities involved cannot be greater than number fundamental quantities whose dimensions are involved.
3.      To find dimensions of a new quantity.

Argument of a Function:
Most of the functions can be expanded into power series as shown below.
In such cases x have to be a dimensionless quantity otherwise we have right hand side of an equation in which each term has different dimension.
Now, consider famous equations like
(i)       from radioactive decay
(ii)     for charging of a capacitor in an RC circuit
(iii)  for growth of current in an LR circuit
In all of the cases, quantities in the exponent have to be dimensionless and thus  have dimensions of time and are called time constants. These quantities in some sense represent time scale at which changes occur in respective systems.

(iv)   for one-dimensional simple harmonic progressive wave has wavelength  which has dimensions of length and time period of oscillation  which has dimensions of time.


1.      Using dimensional analysis check the consistency of equation  of time period of a simple pendulum on mass m of its bob, length l of its length and acceleration due to gravity g.

2.      Excess (above atmospheric value) pressure inside a liquor id is expected to depend on depth h below its surface, density ρ, and gravity g. Using dimensional analysis, deduce relation between pressure P and h, ρ, g.

3.      Using dimensional analysis establish (i) dependence of potential energy of a particle of mass m, placed in the earth’s  gravitational field having acceleration due to gravity g at a height h above the earth’s surface (ii) dependence of kinetic energy of a particle of mass m, moving with velocity v.  (iii) In this it is not possible to determine constant of proportionality from dimensional analysis. However using 2 and 3 above with the law of conservation of energy, and kinematical equations, determine the ratio of proportionality constants in 2 and 3.

4.      Viscous force between two layers of liquid in motion is defined by newton’s formula as , where A is the area of contact between the two layers, and  is the velocity gradient in the liquid, i.e., velocity of the flow changes by dv in distance dz perpendicular to flow direction. What are the dimensions of η, known as coefficient of viscosity? When a spherical object of radius R flows through a viscous medium with speed v, it  experiences viscous drag (resistive force). Find an expression of this viscous force using dimensional analysis, assuming it to depend on η, R and v . In this case it is not possible to determine constant of proportionality which turns out to be 6π and the formula thus obtained is known as Stokes’ law.

5.      A great physicist of previous century (P. A. M. Dirac) loved playing with numerical values of fundamental constants of nature. By playing dimensionally with mass of electron me charge on electron e, Planck’s constant h, and gravitational constant G we may be able to obtain expressions for what is known as Planck length lP, Planck time tP and Planck mass mP. Obtain these expressions dimensionally and estimate value of these quantities. Particle Physicists and Cosmologists use these values in trying to understand evolution of our universe.

6.      From Coulomb’s formula  and Bio-Savart’s Law , find dimensions of ε0 and µ0. Show that  has dimensions of velocity. From the values of     ε0 = 8.85×10-12 SI units and µ0 = 4π×10 – 7 SI units, estimate value of this velocity .



7.      A dense collection of equal number of electrons and positive ions is called neutral plasma. Certain solids containing fixed positive ions surrounded by free electrons can be treated as neutral plasma. Let ‘N’ be the number density of free electrons, each of mass ‘m’. When electrons are subjected to electric field, they are displaced relatively away from the heavy positive ions. If the electric field becomes zero, the electrons begin to oscillate about the positive ions with a natural angular frequency ‘ωp’, which is called plasma frequency. To sustain the oscillations, a time varying electric field needs to be applied that has an angular frequency ω, where a part of energy is absorbed and a part of it is reflected. As ω approaches ωp, all the free electrons are set to resonate together and all the energy is reflected. This is explanation of highly reflective metals.

(i)     Taking the electronic charge as ‘e’ and the permittivity as ‘ε0’, use dimensional analysis to determine the correct expression for ωp.
(a)                      (b)               (c)             (d)
(ii)   Estimate the wavelength at which plasma reflection will occur for a metal having the density of electrons N = 4×1027 m – 3. Take ε0 ≈ 10 – 11 and m ≈ 10 – 30, where these quantities are in proper SI units.
(a)     800 nm     (b)  600 nm             (c) 300 nm           (d) 200 nm                       [JEE 2011]




Hints, Solution, Answers:
1.      [l] = [L]1  [g] = [L]1[T] -2.  Thus .
The given equation is dimensionally correct.

2.      Let  .  Here [P] = [F/A] = [M1L1T – 2]/[L2] = [M]1[L] – 1[T] – 2
[h] = [L]1,  [ρ] = [M]1[L] – 3  and [g] = [L]1 [T] – 2
Taking [P] = [h]x [ρ] y [g]z, and equating dimensions of m, L, and T, we get
(power of [M])  :   y = 1,
(power of [L])  :   x – 3y + z = -1
(power of [T])  :   -2z = - 2
This gives us z = 1 and x = 1  and we have 

3.      We get  and  using conservation of energy and kinematical equation
If we choose system of units such that  then

4.         and 
Matching the powers on two sides, this gives us x = 1,  y = 1 and z = 1.
Thus , ,  the constant of proportionality 6π is determined from some other method.

5.      We get ,      and

6.                  Taking   [q] = [I1 T1], [E] = [F]/[q]    and [B] = [F]/[q][v], we get
[E] = [M1 L1 T - 3 I -1]    and  [B] = [M1 T - 2 I - 1 ]
This gives us  [ε0] = [M - 1 L-3 T  4 I  2]    and [µ0] = [M1 L1 T -2 I -2]
Thus,    and from the given values   = 3×108 m/s.

7.                  [Ans: (i) -  (c) ,     (ii) -  (b)]



References:

  1. JEE - Joint Entrance Examination for admission to IIT

  1. Physics Textbook for class XI part-I,  NCERT New Delhi (2006)


Problem Based Learning in Basic Physics - VII



Problem Based Learning in Basic Physics - VII

 

                                                       A. K .Mody

C-14 Beverly Hills, Lam Road, Devlali, Nashik 422401, Maharashtra


H. C. Pradhan

HBCSE, TIFR, V. N. Purav Marg, Mankhurd
Mumbai – 400 088



[In this article- seventh in the series of articles we present problems for a problem based learning course from the area of material properties. We present the learning objectives in this area of basic physics and what each problem tries to achieve with its solution. ]

In this article, seventh in the series of Problem Based Learning in Basic Physics, we present problems on material properties. Methodology and philosophy of selecting these problems are already discussed. (Pradhan 2009, Mody 2011)


To review methodology in brief, we note here that this PBL (Problem Based Learning) starts after students have been introduced to formal structure of Physics. Ideally students would attempt only main problem. If they find it difficult, then depending upon their area of difficulty, right auxiliary problem have to be introduced by teacher who is expected to be a constructivist facilitator. Teacher may choose as per his/her requirement or may construct questions on the spot to guide student to right idea and method.

Material Properties: Elasticity of solids and fluids as well as mechanics of fluids
Learning objectives:
1.      To understand the role that property of elasticity of solid, liquid and gases plays within material according to Hooke’s law along with laws of physics and how it works in known situations.

2.      To understand behavior of fluids according to Archimedes principle, equation of continuity and Bernoulli’s principle.
Problems:
1.      A sphere of mass 1 kg is suspended at the end of 2 m long steel wire whose other end is fixed to the ceiling. The wire has a cross-sectional area of 1 mm2. The sphere is raised by some height and then dropped to give sudden jerk to the wire. Find the maximum height to which the ball can be raised so that wire doesn’t break. [Given: Ysteel = 2×1011 N/m2 and breaking stress for steel = 1.1×109 N/m2]

Tasks involved in this problem are:
a.       To relate spring constant with elastic modulus.
b.      To apply conservation of energy to the wire to find its extension assuming the model of elastic spring.
c.       To calculate stress based on extension of the wire.
d.      To estimate maximum height that will not allow stress to exceed is breaking limit.

Fig. P(2)
2.      A rod of length 1.05 m having negligible mass is supported at its ends by two wires, A of steel and B of aluminium of equal lengths as shown in figure. The cross-section areas of wires A and B are 1.0 mm2 and 2.0 mm2 respectively. At what point along the rod should a mass m be suspended in order to produce (a) equal stress and (b) equal strains in bith the wires.[Given: Ysteel = 20×1010 N/m2 Yaluminium = 7×1010 N/m2]                               [NCERT XI]
                                                                     
Tasks involved in this problem are:
a.       To apply condition of equilibrium under given situation.

b.      To calculate position where mass to be hanged to meet the required condition.
3.      A wire of density 9 gm/cm3 is stretched between two clamps 100 cm apart, while subjected to an extension of 0.05 cm. What is the lowest frequency of transverse vibrations in the wire, assuming Young’s modulus of the material to be 9×1011 dyne/cm2.                    [JEE  1975]

Tasks involved in this problem are:
a.   To calculate tension due to stretching of wire.
b.   To calculate fundamental frequency of vibration based on this tension.

Fig. P(4)
4.      A rail track made of steel having length 10 m is clamped on a railway line at its two ends. On a summer day due to rise in temperature by 20oC, it is deformed as shown in the figure. Find x, (displacement of the centre) if αsteel = 1.2×10 – 5 /oC and Ysteel = 20×1010 N/m2]                       
                                                                                                                           [NCERT EP XI]                                                                                                     
Tasks involved in this problem are:
a.       To calculate increase in length in accordance with property of thermal expansion.

b.      To find geometric deformation.

Fluids:
5.      A piece of brass (alloy of copper and zinc) weighs 12.9 g in air. When completely immersed in water it weighs 11.3 g. What is the mass of copper contained in the alloy? Specific gravity of copper and zinc, are 8.9 and 7.1 respectively.                                                   [JEE 1966]
[Note:  This is the problem similar to what Archimedes must have faced when he was assigned the task to estimate gold in the crown.]

Tasks involved in this problem are:
a.       To frame the equations for total mass and loss of weight.
b.      To realize that it is volume of the body that decides the weight of the liquid displaced and hence loss of weight.
c.       Solve the two equations  for volume of one of the constituent and hence estimate the masses.
[Here auxiliary problems are given to assist in realizing formation of simple equation for loss of mass and how it relates to volume of the object.]

Auxilliary Problems:
A.    What percentage of volume of ice remains submerged while it is floating on the water surface? Ice has specific gravity is 0.91.

B.     A piece of copper having an internal cavity weighs 264 g in air and 221 g in water. Find the volume of the cavity. Density of copper = 8.8 g cm – 3.                                            [JEE 1963]

6.      A boat carrying number of large stones is floating in a water tank that is about to overflow. If the stones are unloaded into the water tank, what will happen to water level in water tank? Will water in the tank over flow? Give scientific explanation based on Archimedes principle.

Tasks involved in this problem are:
This is not necessarily a mathematical problem. However one can write conditions to arrive at the conclusion. One can also argue qualitatively.

7.      A cylindrical vessel of height 500 mm has an orifice (small hole) at its bottom. The orifice is initially closed and water is filled in it up to height H. Now the top is completely sealed with a cap and the orifice at the bottom is opened. Some water comes out from the orifice and the water level in the vessel becomes steady with height of water column being 200 mm. Find the fall in the height (in mm) of water level due to opening of the orifice. [Take atmospheric pressure = 1.0×105 N/m2, density of water = 1000 kg/m3 and g = 10 m/s2. Neglect any effect of surface tension.]                                                                                                    [JEE 2009]



Tasks involved in this problem are:
a.       To realize and write equation for the condition that has to be satisfied once the orifice is opened for liquid to stop flowing out.
b.      To understand the thermodynamic condition of air trapped above the water.
c.       To solve the two conditions to estimate the loss of height of water.

Fig. P(8)
8.      Water in a cylinder is being rotated at constant angular speed ω about the axis of the cylinder (see the figure). Ignore effect of surface tension and find the equation of the surface of water. Can you identify the surface?

Tasks involved in this problem are:
a.        To find the net force direction on a mass element on the liquid surface so that surface assumes position perpendicular to the force.
b.      Geometrically finding the angle to arrive at equation of the surface.

Fig. P(9)
9.      A non-viscous liquid of constant density 1000 kg/m3 flows in a streamline motion along a tube of variable cross-section. The tube is kept inclined in the vertical plane as shown in the figure. The area of cross-section of the tube at two points P and Q at heights of 2 metre and    5 metre are respectively 4×10 – 3m2 and 8×10 – 3m2. The velocity of the liquid at point P is         1 m/s. Find the work done per unit volume by the pressure and the gravity forces as the fluid flows from point P to Q.                                                                                                  [JEE 1997]

Tasks involved in this problem are:
a.       Apply equation of continuity to estimate speed of the fluid at the other end.
b.      Calculate pressure  difference at the two ends using Bernoulli’s principle.
c.       To estimate the work/energy accordingly.

Fig. P(10)

10.  A uniform wire having mass per unit length λ is placed over a liquid surface. The wire causes the liquid to depress by y (y << a) as shown in the figure. Find the surface tension of the liquid. Neglect end effect.                                                                                [JEE 2004]

Tasks involved in this problem are:
a.       To understand using free body diagram as how does the force of surface tension support this object to float on the liquid surface.
b.      To understand how and why small angle approximation have to be applied to solve the equations obtained in part ‘a’ to get the expression for surface tension.

Fig. P(11)
11.  A soap bubble having surface tension T and radius R is formed on a ring of radius b                             (b << R). Air is blown inside tube with velocity v as shown. The air molecules collide perpendicularly with the wall of the bubble and stops. Calculate the radius at which the bubble separates from the ring.                                                     [JEE 2003]

Tasks involved in this problem are:
a.       To apply Bernoulli’s principle inside and outside the bubble.
b.      To use excess pressure inside the bubble concept to understand why bubble would separate from the ring. [Remember this is a popular toy based problem which children play with.]

12.  Eight droplets of mercury, each of radius 1 mm, coalesce into a single drop. Find (i) the radius of the single drop formed (assuming all the droplets and the drop to be spherical in shape), (ii) the change in the surface energy of the mercury drop, (iii) the change in the temperature of the mercury. [Surface tension of mercury = 0.465 J/m2,                                   Density of mercury = 13.6×103 kg/m3, Specific heat of mercury = 140 J Kg - 1 K - 1]                                             [Ans: (i) 2 mm  (ii) 2.337×10 – 5 J (iii) 3.663×10 – 4 K]



Tasks involved in this problem are:
a.       To understand that volume /mass of the liquid drop/s remain same when they combine or breakup.
b.      To understand need for energy in breaking or release of energy when drops combine.
c.       To realize what happens to excess (surface) energy in accordance with energy conservation principle.
Solutions:
1.      Let the sphere be raised to height h. When it reaches the bottom, the gravitational P.E. at the bottom point gets converted in to elastic P.E. due to extension of the wire.
i.e.,  mgh = ½ kx2 where x is the extension of the wire. [Here  from Solution of P(2) above.]
This strain causes . To prevent breaking this has to be less than breaking stress SB. Which gives the condition .
Fig. P(2)

2.      Let TA and TB represent tensions in string A (steel) and B (aluminum) respectively, then

(a)    For equal stress :      and for torque around point of suspension of weight to be in equilibrium, TA x = TB (L – x)
Solving the above two gives
(b)   For equal strain : ΔlA = ΔlB   which gives   and for torque around point of suspension of weight to be in equilibrium, TA x = TB (L – x)-
Solving the two equations gives
3.      For a wire extended under tension,  and frequency of vibrating string  where m is mass per unit length of the wire.
In terms of given quantities, m = ρA which gives
Fig. P(4)

4.      Referring to the figure given and applying Pythagoras,
 (neglecting higher order term of ΔL we get x2 = ½ LΔL,
Which gives  

5.      Let 1 denote Copper and 2 denote zinc.
The given information than gives m1 +m2 = ρ 1V1 + ρ2V2 = 12.9 gm
and  ρW (V1 + V2)  = 1.6 gm 
Substituting appropriate specific gravities (note ρW = 1) , we get m1 = 7.61 gm


Auxilliary Solutions:
A.    For the floating ice, let V be the volume of ice and V’ be the volume of the submerged portion.
Weight of the ice = weight of the water displaced
\ ρiceVg = ρwaterV’g
\

B.   Let V  be the volume of the metal piece and V0 be that of cavity.
Then we have ρ(V – V0) = 264    and ρWV = 264  - 221 = 43
Solving which we get V0 = 13 cm3.

6.       Volume of water displaced = (weight of the stone)/(ρwaterg)
and   volume of stone = ρstoneVstoneg
this gives   and since ρwater   < ρstone   we get Vstone < Vwater
The tank will not over flow.
 
Fig. P(7)
7.         Initially the pressure of air above the liquid is PA : the atmospheric pressure
   after the orifice is opened, the pressure of air above the liquid is P = PA – hρg
   and also  PA (L – H) A = P (L – h) A where A is the area of cross-section of the cylinder and        
   L =500 mm and h = 200 mm.    finding P and solving the equations we get H = 206 mm so
   that    H  -  h  = 6 mm.
Fig. P(8)
8.      Referring to figure above,   for a small element of mass m at (x, y)
Integration yields,    ,    which is equation of parabola.

Fig. P(9)
9.      From equation of continuity vpAp = vqAq      that gives vq = ½ m/s.
Work done by gravity = ρgh = 29.4×103 J/m3
From Bernoulli’s equation we have Pp + ½ ρvp2 = Pq + ½ ρvq2 + ρgh
This gives work by pressure force = Pp – Pq =  ρgh   - (½ ρvp2  -  ½ ρvq2) = 29.03×103 J/m3
Fig. P(10)
10.  Referring to the figure, when the needle is in equilibrium,   and 2Tsinθ = λg 
in small angle approximation : tanθ ≈ sinθ       wihich gives 
Fig. P(11)
11.  Referring to figure : and using Bernoulli’s equation for outside the bubble and inside the bubble, we get  Pout + ½ ρvout2 = Pin + ½ ρvin2
 where T is the surface tension  and vin = 0  yields  

12.  When drops coalesce into one, the total volume remains constant : i.e.,    which gives R = 2r = 2 mm
Also loss of surface energy results in rise in temperature of the drop.
i.e.,  ΔUsurface = msΔθ      here                                which gives Δθ = 3.663×10 – 4 K

References:
  1. Mody A. K. & Pradhan H. C., ‘Problem Based Learning in Basic Physics – I, School Science 49 (3) Sept 2011

  1. Pradhan H.C. & Mody A. K., ‘Constructivism applied to physics teaching for                                     capacity building of undergraduate students’, University News, 47 (21) 4-10, (2009)

  1. JEE - Joint Entrance Examination for admission to IIT

  1. Physics Textbook for class XI part-I,  NCERT New Delhi (2006)

  1. NCERT EP XI : Physics Exemplar Problems class XI, NCERT New Delhi (2009)