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MASTER OF ARTS (GEOGRAPHY) Study Guide - Tombolo, Ria, Focus Ii

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University of Delhi - DU
Department
Geography
Course
MASTER OF ARTS (GEOGRAPHY)
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Document Summary

Sea waves, aided by winds, currents, tides, and storms carry on the erosional and depositional processes. In their forward surge, waves splashing against the coast may enter the joints and crevices in the rocks: the air imprisoned inside is immediately compressed but when the waves retreat, the compressed air expands with explosive violence. Hydraulic action: hydraulic action is the erosion that occurs when the motion of water against a rock on the surface produces mechanical weathering. It is a mechanical process, in which the moving water current flows against the banks and bed of a river, thereby removing rock particles. Headlands and bays: cliffs along the coastline do not erode at the same pace. When a stretch of coastline is formed from different types of rock, headlands and bays can form: bands of soft rock such as clay and sand are weaker therefore they can be eroded quickly.

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Related Questions

Consider a traveling wave described by the formula

y_1(x,t) = A \sin(k x - \omega t).

This function might represent the lateral displacement of a string, a local electric field, the position of the surface of a body of water, or any of a number of other physical manifestations of waves.

Part A  
Which one of the following statements about the wave described in the problem introduction is correct?
ANSWER:
  The wave is traveling in the +x direction.
The wave is traveling in the -x direction.
The wave is oscillating but not traveling.
The wave is traveling but not oscillating.		  
Part B  
Which of the expressions given is a mathematical expression for a wave of the same amplitude that is traveling in the opposite direction? At time t=0 this new wave should have the same displacement as y_1(x,t), the wave described in the problem introduction.
ANSWER:
  A \cos (k x - \omega t)
A \cos (k x + \omega t)
A \sin (k x - \omega t)
A \sin (k x + \omega t)		  

 

 

The principle of superposition states that if two functions each separately satisfy the wave equation, then the sum (or difference) also satisfies the wave equation. This principle follows from the fact that every term in the wave equation is linear in the amplitude of the wave.

Consider the sum of two waves y_1(x,t)+y_2(x,t), where y_1(x,t) is the wave described in Part A and y_2(x,t) is the wave described in Part B. These waves have been chosen so that their sum can be written as follows:

y_{\rm s}(x,t) = y_{\rm e}(x) y_{\rm t}(t).

This form is significant because y_e(x), called the envelope, depends only on position, and y_t(t) depends only on time. Traditionally, the time function is taken to be a trigonometric function with unit amplitude; that is, the overall amplitude of the wave is written as part of y_e(x).

Part C  
Find y_e(x) and y_t(t). Keep in mind that y_t(t) should be a trigonometric function of unit amplitude.

A boy in a wheelchair (total mass 50.5 kg) has a speed of 1.40 m/s at the crest of a slope 2.40 m high and 12.4 m long. At the bottom of the slope, his speed is 6.50 m/s. Assume air resistance and rolling resistance can be modeled as a constant friction force of 41.0 N. Find the work he did in pushing forward on his wheels during the downhill ride.

 

 
 
 

2 Answers

Relevance
  • electron1
    Lv 7
    4 years ago

    There are two forces that cause the wheelchair to accelerate. These two forces are the component of the wheelchair’s weight that is parallel to the hill and the force the boy exerts. The net force on the wheelchair is equal to the sum of these two forces minus the friction force. Let’s use the following equation to determine the acceleration.

     

    vf2 = vi^2 + 2 * a * d

    6.5^2 = 1.4^2 + 2 * a * 12.4

    24.8 * a = 40.29

    a = 40.29 ÷ 24.8

    This is approximately 1.62 m/s^2.

     

    Net force = 50.5 * 40.29 ÷ 24.8 = 2034.645 ÷ 24.8

    This is approximately 82 N.

     

    Force parallel = 50.5 * 9.8 * 2.40 ÷ 12.4 = 1187.76 ÷ 12.4

     

    This is approximately 95.8 N. This force and the force that the boy exerts are the forces that cause the wheelchair to accelerate.

     

    Net force = F + (1187.76 ÷ 12.4) – 41

    Set the two net forces equal to each other.

     

    F + (1187.76 ÷ 12.4) – 41 = 2034.645 ÷ 24.8

    F = 41 + (2034.645 ÷ 24.8) – (1187.76 ÷ 12.4)

    F is approximately 27.3 N

     

    Work = [41 + (2034.645 ÷ 24.8) – (1187.76 ÷ 12.4)] * 12.4 = 337.9625 J

     
  • JupiterSky
    Lv 6
    4 years ago

    His change in kinetic energy is due to gravitational- and his own work,

    while the friction does negative work.

     

    ∆K = ∆U +∆W + ∆Wf

    ½m(Vf²−Vi²) = mgh + ∆W + Ff*d

    ∆W = ½m(Vf²−Vi²) − mgh − Ff*d

    ∆W = ½*50.5(6.5²−1.4²) − (50.5*9.8*2.4) − (−41*12.4)

    ∆W = 508 J

     
Still have questions? Get your answers by asking now.
 
 
Next Question
---
asked in Science & MathematicsPhysics · 8 years ago

What is the spring constant? please help me!!!!?

A block of mass 487 g is pushed against the

spring (located on the left-hand side of the

track) and compresses the spring a distance

4.7 cm from its equilibrium position (as shown

in the figure below). The block starts from

rest, is accelerated by the compressed spring,

and slides across a frictionless horizontal track

(as shown in the figure below). It leaves the

track horizontally, flies through the air, and

subsequently strikes the ground.

acceleration = 9.81

 

A) What is the spring constant?

B)What is the speed v of the block when it leaves

the track?

C) What is the total speed of the block when it

hits the ground?

...Show more
Update:

Height Above ground = 1.9 m

Lands = 4.59m away

 
What is the spring constant? please help me!!!!?

3 Answers

Relevance
  • Jánošík
    Lv 7
    8 years ago
    Favorite Answer

    I'm sure there is some crucial information in "the figure below" !!!

     

    Edit:

    OK... now we got something to work with ... ;-)

     

    Time needed to fall a vertical distance of 1.9 m is:

    t = √( 2h / g )

    t = √[ 2×(1.9 m) / (9.81 m/s²) ]

    t = 0.6224 s

     

    In that time, the block must travel a horizontal distance of 4.59 m, so the horizontal velocity is:

    r = v×t

    (4.59 m) = v×(0.6224 s)

    v = 7.37 m/s < - - - - - - - - - - - - - - - - - answer B

     

    That is also the speed of the block as it leaves the spring.

    Its kinetic energy at that time is:

    KE = m×v²/2

    KE = (0.487 kg)×(7.3749 m/s)²/2

    KE = 13.244 J

     

    That is also the elastic potential energy stored in the spring at maximum compression. So the spring constant is:

    KE = PEe = k×d²/2

    (13.244 J) = k×(0.047 m)²/2

    k = 12 N/m < - - - - - - - - - - - - - - - - - - answer A

     

    The gravitational potential energy of the block on the table is:

    PEg = m×g×h

    PEg = (0.487 kg)×(9.81 m/s²)×(1.9)

    PEg = 9.077 J

     

    The total energy of the block on the table is:

    TE = PEg + PEe

    TE = (9.077 J) + (13.244 J)

    TE = 22.32 J

     

    When hitting the ground, all that energy is converted to kinetic energy, so

    TE = KE = m×v²/2

    (22.32 J) = (0.487 kg)×v²/2

    v = 9.57 m/s < - - - - - - - - - - - - - - - - - - answer C

    ...Show more
     
  • Technobuff
    Lv 7
    8 years ago

    There must be a height above ground and a distance from the end of the track on the "as shown in the figure below".??

     
  • STALKER
    Lv 4
    8 years ago

    use f=kl

     

    where k is the spring constant and l is extension from the natural length.

     

    k=f/l

     

    since you have mass in grams. use w=mg

     

    w=0.487 x 9.8 = 4.77N

     

    Now use the equation,

     

    k=4.77/4.7

     

    k=1.012

     

    Note: my answer could be wrong since I do not know the springs original length from the diagram shown. But, the method of working out spring constant is same.

    ...Show more
     
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Next Question
ひいらぎ
Lv 5
asked in Science & MathematicsPhysics · 1 decade ago

Physics Momentum, Rolling?

Pat builds a track for his model car out of wood. The track is 10.00 cm wide and 3.00 m long, and is solid. The runway is cut such that it forms a parabola by the equation y=(x - 3)^2/9. Locate the horizontal position of the center of gravity of this track.

 

A washing machine load in the "spin" cycle, (much like a centrifuge used to separate fluids), can be modeled as a cylinder which has zero density toward the center, and starting from some inner radius where the clothes (or fluids) begin, increases in density as you move radially outward. The washing machine has density of clothes (in SI units) of p=14r+5, a height of 0.51 m, and only has clothes present from inner radius 0.2m out to 0.7m from the center.

-What is the moment of Inertia of the wash load?

-What is the power of motor that drives the clothes from rest up to 4 rev/sec, in 14 seconds if the basin has moment of Inertia of 4 kg*.m2

...Show more
 
Physics Momentum, Rolling?

1 Answer

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  •  
    Anonymous
    1 decade ago
    Favorite Answer
     

    I can't visualize the first problem.

     

    The second: Moment of inertia is I = m r^2. In a shell of thickness dr there is a mass of p * 2 * pi * r * h * dr. The moment of inertia of the shell is 2 pi h p r^3 dr. Now integrate this from r = 0.2m to r = 0.7m.

     

    Kinetic energy is 1/2 m v^2. In rotations the moment of inertia is like the mass and the angular velocity is like the velocity, so rotational energy is 1/2 I omega^2. Omega is in rad/s. The total inertia of the system is the sum of the inertia of the clothes and the basin. Divide the energy by the time needed to get the power.

    ...Show more
     
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Next Question
AZ
asked in Science & MathematicsPhysics · 1 decade ago

Physics:You and your friends push a 75-kg...Help!?

You and your friends push a 75-kg greased pig up an aluminum slide at the county fair, starting from the low end of the slide. The coefficient of kinetic friction between the pig and the slide is 0.070.

 

(a) All of you pushing together (parallel to the incline) manage to accelerate the pig from rest at the constant rate of 4.9 m/s2 over a distance of 1.8 m, at which point you release the pig. The pig continues up the slide, reaching a maximum vertical height above its release point of 50 cm. What is the angle of inclination of the slide? __degree

 

(b) At the maximum height the pig turns around and begins to slip down the slide, how fast is it moving when it arrives at the low end of the slide? __m/s

...Show more
 
Physics:You and your friends push a 75-kg...Help!?

1 Answer

Relevance
  •  
    Anonymous
    1 decade ago
    Favorite Answer
     

    ♣the distance the pig was pushed up is

    s=0.5*a*t^2, where s=1.8m, a=4.9m/s^2, t is time of push-up;

    speed of the pig gained after s=1.8m is v=a*t; thus v^2=2as;

    ♠ kinetic energy of the pig at the moment it’s released after push-up is

    E=0.5*m*v^2, which is enough for the pig to move by itself L distance more along the ramp, where L=h/sin(b), h=50cm=0.5m, b is angle in question;

    ♦pig’s potential energy at vertex (when stopped) is E1=mgh;

    the energy E2=E-E1 is gone on friction, that is E2=f*L is work of friction, where

    f=μ*w1, w1=mg*cos(b) is component of pig’s weight normal to the aluminum ramp; or;

    f= μ*mg*cos(b);

    ♦Thus E2=E-E1; or; f*L = 0.5*m*v^2 –mgh; or;

    (μ*mg*cos(b)) * (h/sin(b)) =0.5*m* 2as –mgh; or;

    μ*gh*cos(b)/sin(b) =as –gh, hence cot(b) =(as –gh)/(μ*gh), hence

    (a); b=atan(μ*gh/(as-gh))= atan(0.07*9.8*0.5/(4.9*1.8 -9.8*0.5)) =5°;

     

    ♥ pig’s potential energy above the low end of the ramp is

    W= mg*(s*sin(b) +h); pig’s ramp position is p=s +L = s + h/sin(b);

    Pig’s final kinetic energy is W1=W-W2, where W2=f*p is work of friction;

    and W1=0.5*m*v^2; thus

    0.5*m*v^2 = mg*(s*sin(b) +h) – μ*mg*cos(b)*(s + h/sin(b));

    v^2 =2g*(s*sin(b) +h)*(1 –μ*cot(b)) =2.575;

    (b); v =1.605 m/s;

    ...Show more
     
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3. 3 Stratosphere-troposphere exchange

The rate of exchange of air between the troposphere and thestratosphere is critical for determining the potential of variouspollutants emitted from the surface to reach the stratosphere andaffect the stratospheric ozone layer. One of the first estimates ofthis rate was made in the 1960s using measurements of strontium-90(90Sr) in the stratosphere. Strontium-90 is a radioactive isotope(half-life 28 years) produced in nuclear explosions. It has nonatural sources. Large amounts of 90Sr were injected into thestratosphere in the 1950s by above-ground nuclear tests. Thesetests were banned by international treaty in 1962. Following thetest ban the stratospheric concentrations of 90Sr began to decreaseas 90Sr was transferred to the troposphere. In the troposphere,90Sr is removed by wet deposition with a lifetime of 10 days (bycontrast there is no rain, and hence no wet deposition, in thestratosphere). An intensive stratospheric measurement network wasoperated in the 1960s to monitor the decay of 90Sr in thestratosphere. We interpret these observations here using a 2-boxmodel for stratosphere-troposphere exchange with transfer rateconstants kTS and kST (yr-1) between the tropospheric andstratospheric reservoirs. The reservoirs are assumed to beindividually well-mixed.



Let mS and mT represent the masses of 90Sr in the stratosphere andin the troposphere respectively. Observations of the decrease inthe stratospheric inventory for the period 1963-1967 can be fittedto an exponential mS(t) = mS(0)exp(-kt) where k = 0.77 yr-1.

1. Write mass balance equations for mS and mT in the 1963-1967period.

2. Assuming that transfer of 90Sr from the troposphere to thestratosphere is negligible (we will verify this assumption later),show that the residence time of air in the stratosphere is tS =1/kST = 1.3 years.

3. Let m'T and m'S represent the total masses of air in thetroposphere and the stratosphere, respectively. Show that theresidence time of air in the troposphere is tT = tS (m'T/m'S) = 7.4years. Conclude as to the validity of your assumption in question2.

4. Hydrochlorofluorocarbons (HCFCs) have been adopted asreplacement products for the chlorofluorocarbons (CFCs), which werebanned by the Montreal protocol because of their harmful effect onthe ozone layer. In contrast to the CFCs, the HCFCs can be oxidizedin the troposphere, and the oxidation products washed out byprecipitation, so that most of the HCFCs do not penetrate into thestratosphere to destroy ozone. Two common HCFCs have trade namesHCFC-123 and HCFC-124; their lifetimes against oxidation in thetroposphere are 1.4 years and 5.9 years, respectively. There are noother sinks for these species in the troposphere. Using our 2-boxmodel, determine what fractions of the emitted HCFC-123 andHCFC-124 penetrate the stratosphere.