QA 01

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course MTH 279

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Part I: The equation m x '' = - k x*********************************************

Question: `q001. Show whether each of the following functions all satisfy the equation m x '' = -k x:

x = cos(t)

x = sin( sqrt( k / m) * t)

x = 3 cos( sqrt( k / m) * t ) + 5 sin (sqrt(k / m) t)

x = B sin(sqrt(k / m) * t) + C cos( sqrt( k / m) * t + 3)

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Your solution:

x = cos(t)

x' = -sin(t)

x'' = -cos(t)

x'' = -k/m*x

-cos(t) = -k/m*cos(t)

No!

x = sin( sqrt( k / m) * t)

x' = sqrt(k/m)*cos( sqrt(k/m)* t)

x'' = -k/m*sin( sqrt(k/m) * t)

x'' = -k/m*x

-k/m*sin( sqrt(k/m) * t) = -k/m*sin( sqrt( k / m) * t)

Yes!

x = 3 cos( sqrt( k / m) * t ) + 5 sin (sqrt(k / m) t)

x' = -3 * sqrt(k/m) * sin( sqrt(k/m) * t) + 5 * sqrt(k/m) * cos( sqrt(k/m) * t)

x'' = -3 * (k/m) * cos( sqrt(k/m) * t) - 5 * (k/m) * sin( sqrt(k/m) * t)

x'' = -k/m*x

-3 * (k/m) * cos( sqrt(k/m) * t) - 5 * (k/m) * sin( sqrt(k/m) * t) = -k/m * [3 cos( sqrt( k / m) * t ) + 5 sin (sqrt(k / m) t)]

Yes!

x = B sin(sqrt(k / m) * t) + C cos( sqrt( k / m) * t + 3)

x' = B * sqrt(k/m) * cos( sqrt(k/m) * t) - C * sqrt(k/m) * sin( sqrt(k/m) * t + 3)

x'' = -B * (k/m) * sin( sqrt(k/m) * t) - C * (k/m) * cos( sqrt(k/m) * t + 3)

x'' = -k/m*x

-B * (k/m) * sin( sqrt(k/m) * t) - C * (k/m) * cos( sqrt(k/m) * t + 3) = -k/m * [B sin(sqrt(k / m) * t) + C cos( sqrt( k / m) * t + 3)]

Yes!

confidence rating #$&*:

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Given Solution:

If x = cos(t) then x ' = - sin(t) and x '' = - cos(t). Substituting the expressions for x and x '' into the equation we obtain

m * (-cos(t)) = - k * cos(t).

Dividing both sides by cos(t) we obtain m = k. If m = k, then the equation is satisfied. If m is not equal to k, it is not.

If x = sin(sqrt(k/m) * t) then x ' = sqrt(k / m) cos(sqrt(k/m) * t) and x '' = -k / m sin(sqrt(k/m) * t). Substituting this into the equation we have

m * (-k/m sin(sqrt(k/m) * t) ) = -k sin(sqrt(k/m) * t

Simplifying both sides we see that the equation is true.

The same procedure can and should be used to show that the third equation is true.

The question of the fourth equation is left to you.

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Self-critique (if necessary):

I saw that if m = k then that was the only way that equation would be true.

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Self-critique rating: 3

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Question:

`q002. An incorrect integration of the equation x ' = 2 x + t yields x = x^2 + t^2 / 2. After all the integral of x is x^2 / 2 and the integral of t is t^2 / 2.

Show that substituting x^2 + t^2 / 2 (or, if you prefer to include an integration constant, x^2 + t^2 / 2 + c) for x in the equation x ' = 2 x + t does not lead to equality.

Explain what is wrong with the reasoning given above.

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Your solution:

x ' = 2 x + t

2 x + t = 2( x^2 + t^2 / 2 ) + t

2 x + t = 2x^2 + t^2 + t two sides aren't equal

When integrating or deriving, you must keep in mind that you are doing it with respect to one variable. In the method above, the first part was integrated with respect to x and the second part was integrated with respect to t.

confidence rating #$&*:

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Given Solution:

The given function is a solution to the equation, provided its derivative x ' satisfies x ' = 2 x + t.

It would be tempting to say that the derivative of x^2 is 2 x, and the derivative of t^2 / 2 is t.

The problem with this is that the derivative of x^2 was taken with respect to x and the derivative of t^2 / 2 with respect to t.

We have to take both derivatives with respect to the same variable.

Similarly we can't integrate the expression 2 x + t by integrating the first term with respect to x and the second with respect to t.

Since in this context x ' represent the derivative of our solution function x with respect to t, the variable of integration therefore must be t.

We will soon see a method for solving this equation, but at this point we simply cannot integrate our as-yet-unknown x(t) function with respect to t.

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Self-critique (if necessary):

I don't know if I plugged into that equation correctly.

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Self-critique rating: 3

@&

Your work did show that the equation sdid not satisfy the given solution.

Very good.

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Question:

`q003. The general solution to the equation

m x '' = - k x

is of the form x(t) = A cos(omega * t + theta_0), where A, omega and theta_0 are constants. (There are reasons for using the symbols omega and theta_0, but for right now just treat these symbols as you would any other constant like b or c).

Find the general solution to the equation 5 x'' = - 2000 x:

Substitute A cos(omega * t + theta_0) for x in the given equation.

The value of one of the three constants A, omega and theta_0 is dictated by the numbers in the equation. Which is it and what is its value?

One of the unspecified constants is theta_0. Suppose for example that theta_0 = 0. What is the remaining unspecified constant?

Still assuming that theta_0 = 0, describe the graph of the solution function x(t).

Repeat, this time assuming that theta_0 = 3 pi / 2.

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Your solution:

x = A cos(omega * t + theta_0)

x' = -A*omega*sin(omega*t + theta_0)

x'' = -A*omega^2* cos(omega*t + theta_0)

5x'' = -2000x

5 [-A*omega^2* cos(omega*t + theta_0)] = -2000 [A cos(omega * t + theta_0)]

-5omega^2 = -2000 simplify

omega = 20

It appears omega is dependent upon the equation.

If theta_0 = 0, the remaining constant is A.

If theta_0 = 0, then the graph would be a cosine wave with amplitude A, passing through the point (0, -A) with a period of 2pi/20 or pi/10 and a frequency of 10/pi.

If theta_0 = 3pi/2, then the graph would be the same, but shifted horizontally 3pi/2 units to the left. It would have a point (-3pi/2 , -A)

In general, the solution would be

x = Acos(20t + theta_0)

confidence rating #$&*:

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Given Solution:

If x = A cos(omega * t + theta_0) then x ' = - omega A sin(omega * t + theta_0) and x '' = -omega^2 A cos(omega * t + theta_0).

Our equation therefore becomes

m * (-omega^2 A cos(omega * t + theta_0) ) = - k A cos(omega * t + theta_0).

Rearranging we obtain

-m omega^2 A cos(omega * t + theta_0) = -k A cos(omega * t + theta_0)

so that

-m omega^2 = - k

and

omega = sqrt(k/m).

Thus the constant omega is determined by the equation.

The constants A and theta_0 are not determined by the equation and can therefore take any values.

No matter what values we choose for A and theta_0, the equation will be satisfied as long as omega = sqrt(k / m).

Our second-order equation

m x '' = - k x

therefore has a general solution containing two arbitrary constants.

In the present equation m = 5 and k = 2000, so that omega = sqrt(k / m) = sqrt(2000 / 5) = sqrt(400) = 20.

Our solution x(t) = A cos(omega * t + theta_0) therefore becomes

x(t) = A cos(20 t + theta_0).

If theta_0 = 0 the function becomes x(t) = A cos( 20 t ). The graph of this function will be a 'cosine wave' with a 'peak' at the origin, and a period of pi / 10.

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Self-critique (if necessary):

I understand that the points I specified would be at +A, not -A. I was looking at the equation x'' where the coeffiecient of A was negative, and not the solution equation that I should've been looking at.

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Self-critique rating: 3

@&

Very good.

However the horizontal shift resulting from theta_0 = 3 pi / 2 is incorrect.

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t is not replaced by t + theta_0.

omega t + theta_0 = omega * (t + theta_0 / omega).

t has been replaced by t + theta_0 / omega, and the shift is -theta_0 / omega.

If theta_0 = 3 pi / 2, then the argument of the cosine would be 20 * (t + 3 pi / 40) and the horizontal shift would be -3 pi / 40.

See also notes I inserted in your last document.

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Question:

`q004. In the preceding equation we found the general solution to the equation 5 x'' = - 2000 x. Assuming SI units, this solution applies to a simple harmonic oscillator of mass 5 kg, which when displaced to position x relative to equilibrium is subject to a net force F = - 2000 N / m * x. With these units, sqrt(k / m) has units of sqrt( (N / m) / kg), which reduce to radians / second. Our function x(t) describes the position of our oscillator relative to its equilibrium position.

Evaluate the constants A and theta_0 for each of the following situations:

The oscillator reaches a maximum displacement of .3 at clock time t = 0.

The oscillator reaches a maximum displacement of .3 , and at clock time t = 0 its position is x = .15.

The oscillator has a maximum velocity of 2, and is at its maximum displacement of .3 at clock time t = 0.

The oscillator has a maximum velocity of 2, which occurs at clock time t = 0. (Hint: The velocity of the oscillator is given by the function x ' (t) ).

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Your solution:

1. A = .3 and theta_0 = 0, 2pi, 4 pi, etc.

Max. displacement is = to amplitude and since t = 0, you need cos theta_0 = 1 for x = A

2. A = .3 and theta_0 = pi/3

Again, we know max. displacement is A. x = .15, so arccos(.15/.3) will give us thata_0

3. A = .3 and theta_0 = 0, 2pi, etc

Looking at the velocity equation:

Even though a velocity is specified, max x occurs when v = 0, so you really don't need that piece of information.

4. A = 1/10 and theta_0 = pi/2, 5pi/2, etc.

A would be greatest when sin(theta_0) = 1...I think? Maybe it would be when sin(theta_0) was = -1 because there is a negative in the equation. But I don't think so.

confidence rating #$&*:

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Given Solution:

As seen in the preceding problem, a general solution to the equation is

x = A cos(omega * t + theta_0),

where omega = sqrt(k / m). For the current equation 5 x '' = -2000 x, this gives us omega = 20. In the current context omega = 20 radians / second.

So

x(t) = A cos( 20 rad / sec * t + theta_0 ).

Maximum displacement occurs at critical values of t, values at which x ' (t) = 0.

Taking the derivative of x(t) we obtain

x ' (t) = - 20 rad / sec * A sin( 20 rad/sec * t + theta_0).

The sine function is zero when its argument is an integer multiple of pi, i.e., when

20 rad/sec * t + theta_0 = n * pi, where n = 0, +-1, +-2, ... .

A second-derivative test shows that whenever n is an even number, our x(t) function has a negative second derivative and therefore a maximum value.

We can therefore pick any even number n and we will get a solution.

If maximum displacement occurs at t = 0 then we have

20 rad / sec * 0 + theta_0 = n * pi

so that

theta_0 = n * pi, where n can be any positive or negative even number.

We are free to choose any such value of n, so we make the simplest choice, n = 0. This results in theta_0 = 0.

Now if x = .3 when t = 0 we have

A cos(omega * 0 + theta_0) = .3

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Self-critique (if necessary):

I remember using the first and second derivative tests to find critical numbers and that they can correspond to max and min's, determining concavity, etc. I didn't think to use that in this question because that knoweldge was overshadowed by the way I learned how to play with this particular equation in physics class.

???? In the 4th scenario, do you pick an arbitrary value for theta_0 that makes sin = 1 in order to come up with a value for A?

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Self-critique rating: 3

@&

In a word, yes.

The reason is that you are looking for the maximum possible value of the function. Since the magnitude of the value of the function is proportional to the magnitude of the sine, and the maximum magnitude of the sine is 1, the maximum magnitude of A will occur when | sin(theta) | = 1.

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Last year all my University Physics students were my taking differential equations course at the same time, so we were actually able to do this, which saved a lot of time when working with AC circuits. Those students are at UVA now and some have come by to visit. They tell me this picture made their subsequent courses much easier.

Having played with these equations in physics, you'll be well prepared later in the course where we put it all into the context of differential equations. That greatly simplifies the topic, and will provide you with a valuable tool for more advanced courses.

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Question:

`q005. Describe the motion of the oscillator in each of the situations of the preceding problem. SI units for position and velocity are respectively meters and meters / second.

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Your solution:

In the first scenario, we start the clock at maximum displacement .3 m, which corresponds to the amplitude of the sinusoid. Max x also corresponds to a velocity of 0 m/s.

In the second scenario, we are looking at an oscillator that has a max x of .3 m, but at the point in time we started to measure the motion of the oscillator, its displacement was .15 m, which is half of its maximum value. It has a velocity of -3sqrt(3) m/s at this point.

In the third scenario, we know that the oscillator would have a maximum velocity of 2 m/s when x = 0. At the point in time we are looking at it, though, it has a velocity of 0 m/s and a position = A = .3 m.

In the fourth scenario, we know that the velocity is 2 m/s. If that is its maximum value, we know that its position at this point is 0 m.

confidence rating #$&*:

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Given Solution:

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

Part II: Solutions of equations requiring only direct integration.

`q006. Find the general solution of the equation x ' = 2 t + 4, and find the particular solution of this equation if we know that x ( 0 ) = 3.

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Your solution:

x = t^2 + 4t + C

x(0) = t^0 + 4*0 + C = 3

C = 3

x = t^2 + 4t + 3

confidence rating #$&*:

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Given Solution:

Integrating both sides we obtain

x(t) = t^2 + 4 t + c,

where c is an arbitrary constant.

The condition x(0) = 3 becomes

x(0) = 0^2 + 4 * 0 + c = 3,

so that c = 3 and our particular solution is

x(t) = t^2 + 4 t + 3.

We check our solution.

Substituting x(t) = t^2 + 4 t + 3 back into the original equation:

(t^2 + 4 t + 3) ' = 2 t + 4 yields

2 t + 4 = 2 t + 4,

verifying the general solution.

The particular solution satisfies x(0) = 3:

x(0) = 0^2 + 4 * 0 + 3 = 3.

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q007. Find the general solution of the equation x ' ' = 2 t - .5, and find the particular solution of this equation if we know that x ( 0 ) = 1, while x ' ( 0 ) = 7.

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Your solution:

x'' = 2t - .5

x' = t^2 - .5t + C

x = t^3/3 - t^2/4 + Ct + D

x = t^3/3 - t^2/4 + 7t + 1

confidence rating #$&*:

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Given Solution:

Integrating both sides we obtain

x ' = t^2 - .5 t + c_1,

where c_1 is an arbitrary constant.

Integrating this equation we obtain

x = t^3 / 3 - .25 t^2 + c_1 * t + c_2,

where c_2 is an arbitrary constant.

Our general solution is thus

x(t) = t^3 / 3 - .25 t^2 + c_1 * t + c_2.

The condition x(0) = 1 becomes

x(0) = 0^3 / 3 - .25 * 0^2 + c_1 * 0 + c_2 = 1

so that c_2 = 1.

x ' (t) = t^2 - .5 t + c_1, so our second condition x ' (0) = 7 becomes

x ' (0) = 0^2 - .5 * 0 + c_1 = 7

so that c_1 = 7.

For these values of c_1 and c_2, our general solution x(t) = t^3 / 3 - .25 t^2 + c_1 * t + c_2 becomes the particular solution

x(t) = t^3 / 3 - .25 t^2 + 7 t + 1.

You should check to be sure this solution satisfies both the given equation and the initial conditions.

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q008. Use the particular solution from the preceding problem to find x and x ' when t = 3. Interpret your results if x(t) represents the position of an object at clock time t, assuming SI units.

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Your solution:

x = 3^3/3 - 3^2/4 + 7*3 + 1

x = 28.75 m

x' = 3^2 -3/3 + 7

x' = 14.5 m/s

confidence rating #$&*:

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Given Solution:

Our solution was

x(t) = t^3 / 3 - .25 t^2 + 7 t + 1.

Thus

x ' (t) = t^2 - .5 t + 7.

When t = 3 we obtain

x(3) = 3^3 / 3 - .25 * 3^2 + 7 * 3 + 1 = 28.75

and

x ' (3) = 3^2 - .5 * 3 + 7 = 14.5.

A graph of x vs. t would therefore contain the point (3, 28.75), and the slope of the tangent line at that point would be 14.5.

x(t) would represent the position of an object. x(3) = 28.75 represents an object whose position with respect to the origin is 28.75 meters when the clock reads 3 seconds.

x ' (t) would represent the velocity of the object. x ' (3) = 14.5 indicates that the object is moving at 14.5 meters / second when the clock reads 3 seconds.

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q009. The equation x '' = -F_frict / m - c / m * x ', where the derivative is understood to be with respect to t, is of at least one of the forms listed below. Which form(s) are appropriate to the equation?

x '' = f(x, x')

x '' = f(t)

x '' = f(x, t)

x '' = f(x', t)

x '' = f(x, x ' t)

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Your solution:

x'' = f(x, x', t)

confidence rating #$&*:

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Given Solution:

The right-hand side of the equation includes the function x ' but does not include the variable t or the function x.

So the right-hand side can be represented by any function which includes among its variables x '. That function may also include x and/or t as a variable.

The forms f(t) and f(x, t) fail to include x ', so cannot be used to represent this equation.

All the other forms do include x ' as a variable, and may therefore be used to represent the equation.

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Self-critique (if necessary):

I'm usually bad with definitions, so I'd like to see if I'm understanding this in my words:

You don't have to write t because it is implied. This same follows for x because you have x' in the equation. You must, however, include x' since it encompasses these terms and to do otherwise would leave out a vital piece of information.

@&

Right. Very good.

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Self-critique rating: 2

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Question:

`q010. If F_frict is zero, then the function x in the equation

x '' = -F_frict / m - c / m * x '

represents the position of an object of mass m, on which the net force is - c * x '.

Explain why the expression for the net force is -c * x '.

Explain what happens to the net force as the object speeds up.

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Your solution:

Original equation:

x '' = -F_frict / m - c / m * x '

When F_f = 0 :

x'' = -c/m * x'

Equivalent expressions:

a = -c/m * v

Rearranging:

ma = -c * v

From Newton's 2nd Law:

F_net = ma

Therefore:

F_net = -c * v = -c * x'

As the object speeds up (or accelerates), the net force also increases. We can see this eaily using F_net = ma (since m is constant for an object, as a increases, F also increases.

confidence rating #$&*:

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Given Solution:

Newton's Second Law gives us the general equation

m x '' = F_net

so that

x '' = F_net / m.

It follows that

x '' = -F_frict / m - c / m * x '

represents an object on which the net force is -F_frict - c x '.

If F_frict = 0, then it follows that the net force is -c x '.

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q011. We continue the preceding problem.

If w(t) = x '(t), then what is w ' (t)?

If x '' = - b / m * x ', then if we let w = x ', what is our equation in terms of the function w?

Is it possible to integrate both sides of the resulting equation?

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Your solution:

w' (t) = x'' (t)

w' = -b/m * w

I should think we would be able to integrate both sides of the equation, since both w and w' are both functions of t.

confidence rating #$&*:

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Given Solution:

If w(t) = x ' (t) then w ' (t) = (x ' (t) ) ' = x '' ( t ).

If x '' = - b / m * x ', then if w = x ' it follows that x '' = w ', so our equation becomes

w ' (t) = - b / m * w (t)

The derivative is with respect to t, so if we wish to integrate both sides we will get

w(t) = integral ( - b / m * w(t) dt),

The variable of integration is t, and we don't know enough about the function w(t) to perform the integration on the right-hand side.

[ Optional Preview:

There is a way around this, which provides a preview of a technique we will study soon. It isn't too hard to understand so here's a preview:

w ' (t) means dw / dt, where w is understood to be a function of t.

So our equation is dw/dt = -b / m * w.

It turns out that in this context we can sort of treat dw and dt as algebraic quantities, so we can rearrange this equation to read

dw / w = -b / m * dt.

Integrating both sides we get

integral (dw / w) = -b / m integral( dt )

so that

ln | w | = -b / m * t + c.

In exponential form this is

w = e^(-b / m * t + c).

There's more, but this is enough for now ... ].

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Self-critique (if necessary):

I see that there isn't enough information to perform the actual integration, even though they are both functions of t.

@&

@&

You can't integrate both sides, but if you rearrange the equation to w ' / w = -b / m, you can then do so, as indicated in the given solution.

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Self-critique rating: 3

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Question:

Part III: Direction fields and approximate solutions

`q012. Consider the equation x ' = (2 x - .5) * (t + 1). Suppose that x = .3 when t = .2.

If a solution curve passes through (t, x) = (.2, .3), then what is its slope at that point?

What is the equation of its tangent line at this point?

If we move along the tangent line from this point to the t = .4 point on the line, what will be the x coordinate of our new point?

If a solution curve passes through this new point, then what will be the slope at the this point, and what will be the equation of the new tangent line?

If we move along the new tangent line from this point to the t = .6 point, what will be the x coordinate of our new point?

Is is possible that both points lie on the same solution curve? If not, does each tangent line lie above or below the solution curve, and how much error do you estimate in the t = .4 and t = .5 values you found?

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Your solution:

x' at (.2, .3) = slope at (.2, .3) = .12

tangent line equation at (.2, .3):

x - x_1 = m( t - t_1)

x - .3 = .12 (t - .2)

x = .12( t - .2) + .3

new x coordinate at t = .4

x = .12( .4 - .2) + .3 = .324

x' at (.4 , .324) = 0.2072

tangent line equation at (.4, .324):

x = .2072( t - .4) + .324

new x coordinate at t = .6

x = .36544

I think, based upon the amount of change in the t coordinate, that the points wouldn't lie upon the same solution curve.

Since our approximations appear to be sloping much more gently than the actual curve, I'd say that the calculated approximations are less than the actual slope. Since the slope of the tangent line equation we used to calculate the slope at t = .4 was .12 and the actual x' value at this location was about .21, there's an error of almost 200% (if I'm thinking correctly. It's almost double). At the t = .6 point, we used an equation with a slope of .21, while the actual x' value was .37. Again, this error is almost double.

confidence rating #$&*:

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Given Solution:

At the point (.2, .3) in the (t, x) plane, our value of x ' is

x ' = (2 * .3 - .5) * (.2 + 1) = .12, approximately.

This therefore is the slope of any solution curve which passes through the point (.2, .3).

The equation of the tangent plane is therefore

x - .3 = .12 * (t - .2)

so that

x = .12 t - .24.

If we move from the t = .2 point to the t = .4 point our t coordinate changes by `dt = .2, so that our x coordinate changes by `dx = (slope * `dt) = .12 * .2 = .024. Our new x coordinate will therefore be .3 + .024 = .324.

This gives us the new point (.4, .324).

At this point we have

x ' = (2 * .324 - .5) * (.4 + 1) = .148 * 1.4 = .207.

If we move to the t = .6 point our change in t is `dt = .2. At slope .207 this would imply a change in x of `dx = slope * `dt = .207 * .2 = .041. Our new x coordinate will therefore be .324 + .041 = .365.

Our t = .6 point is therefore (.6, .365).

From our two calculated slopes, the second of which is significantly greater than the first, it appears that in this region of the x-t plane, as we move to the right the slope of our solution curve in fact increases. Our estimates were based on the assumption that the slope remains constant over each t interval. We conclude that our estimates of the changes in x are probably a somewhat low, so that our calculated points lie a little below the solution curve.

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q013. Consider once more the equation x ' = (2 x - .5) * (t + 1).

Note on notation:

The points on the grid

(0, 0), (0, 1/4), (0, 1/2), (0, 3/4), (0, 1)

(1/4, 0), (1/4, 1/4), (1/4, 1/2), (1/4, 3/4), (1/4, 1)

(1/2, 0), (1/2, 1/4), (1/2, 1/2), (1/2, 3/4), (1/2, 1)

(3/4, 0), (3/4, 1/4), (3/4, 1/2), (3/4, 3/4), (3/4, 1)

(1, 0), (1, 1/4), (1, 1/2), (1, 3/4), (1, 1)

can be specified succinctly in set notation as

{ (t, x) | t = 0, 1/4, ..., 1, x = 0, 1/4, ..., 1}.

( A more standard notation would be { (i / 4, j / 4) | 0 <= i <= 4, 0 <= j <= 4 } )

Find the value of x ' at every point of this grid and sketch the corresponding direction field. To get you started the values corresponding to the first, second and last rows of the grid are

-.5, -.625, -.75, -.875, -1

0, 0, 0, 0, 0

...

...

1.5, 1.875, 2.25, 2.625, 3

So you will only need to calculate the values for the third and fourth rows of the grid.

List your values of x ' at the five points (0, 0), (1/4, 1/4), (1/2, 1/2), (3/4, 3/4) and (1, 1).

Sketch the curve which passes through the point (t, x) = (.2, .3).

Describe your curve. Is it increasing or decreasing, and is it doing so at an increasing or decreasing rate?

According to your curve, what will be the value of x when t = 1?

Sketch the curve which passes through the point (t, x) = (.5, .7). According to your curve, what will be the value of x when t = 1?

Describe your curve and compare it with the curve you sketched through the point (.2, .3).

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Your solution:

x' = -.5, 0, .75, 1.75, 3 respectively

It is increasing at an increasing rate. It looks like x = 1.125 when t = 1

On the second curve, it looks like x = 1.5

The second curve is also increasing at an increasing rate, but it looks like it is increasing faster than the first curve sketched.

confidence rating #$&*:

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Given Solution:

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q014. We're not yet done with the equation x ' = (2 x - .5) * (t + 1).

x ' is the derivative of the x(t) function with respect to t, so this equation can be written as

dx / dt = (2 x - .5) * (t + 1).

Now, dx and dt are not algebraic quantities, so we can't multiply or divide both sides by dt or by dx. However let's pretend that they are algebraic quantities, and that we can. Note that dx is a single quantity, as is dt, and we can't divide the d's.

Rearrange the equation so that expressions involving x are all on the left-hand side and expressions involving t all on the right-hand side.

Put an integral sign in front of both sides.

Do the integrals. Remember that an integration constant is involved.

Solve the resulting equation for x to obtain your general solution.

Evaluate the integration constant assuming that x(.2) = .3.

Write out the resulting particular solution.

Sketch the graph of this function for 0 <= t <= 1. Describe your graph.

How does the value of your x(t) function at t = 1 compare to the value your predicted based on your previous sketch?

How do your values of x(t) at t = .4 and t = .6 compare with the values you estimated previously?

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Your solution:

dx / dt = (2 x - .5) * (t + 1)

dx/ (2x - .5) = (t + 1) dt

1/2 ln( abs(2x - .5) = t^2/2 + t + C

ln( abs( 2x - .5) = t^2 + 2t + C

2x - .5 = e^(t^2 + 2t + C)

2x - .5 = e^(t^2 + 2t)C

x = e^(t^2 + 2t)K + .25

.3 = e^(.2^2 + 2*.2)K + .25

K = .05/e^.44

x = (.05/e^.44) * e^(t^2 + 2t) + .25

x(1) = 0.9 It looks like my approximation was a little high compared to the actual value.

x(.4) = .33

x(.6) = .40

The previous approximations appear pretty good. They were .324 and .365, respectively.

confidence rating #$&*:

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Given Solution:

The equation is easily rearranged into the form

dx / (2 x - .5) = (t + 1) dt.

Integrating the left-hand side we obtain 1/2 ln | 2 x - .5 |

Integrating the right-hand side we obtain t^2 / 2 + 4 t + c, where the integration constant c is regarded as a combination of the integration constants from the two sides.

Thus our equation becomes

1/2 ln | 2 x - 5 | = t^2 / 2 + t + c.

Multiplying both sides by 2, then taking the exponential function of both sides we get

exp( ln | 2 x - 5 | ) = exp( t^2 + 2 t + c ),

where as before c is an arbitrary constant.

Since the exponential and natural log are inverse functions the left-hand side becomes | 2 x + .5 |.

The right-hand side can be written e^c * e^(t^2 + 8 t), where c is still an arbitrary constant. e^c can therefore be any positive number, and we replace e^c with A, understanding that A is a positive constant.

Our equation becomes

| 2 x - .5 | = A e^(t^2 + 2 t).

For x > -.25, as is the case for our given value x = .3 when t = .2, we have

2 x - .5 = A e^(t^2 + 2 t)

so that

x = A e^(t^2 + 2 t) + .25.

Using x = .3 and t = .2 we find the value of A:

.05 = A e^(.2^2 + 2 * .2)

so that

A = .05 / e^(.44) = .03220, approx..

Our solution function is therefore

x(t) = .05 / e^(.44) * e^(t^2 + 2 t) + .25, or approximately

x(t) = .03220 e^(t^2 + 2 t) + .25

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Question:

`q015. OK, this time we are really going to be done with this equation. Again, x ' = (2 x - .5) * (t + 1)

Along what line or curve is x ' = 1?

Along what line or curve is x ' = 0?

Along what line or curve is x ' = 2?

Along what line or curve is x ' = -1?

Sketch these three lines and/or curves for 0 <= t <= 1.

Along each of these lines x ' is constant. Along each sketch 'slope segments' with slopes equal to the corresponding value of x '.

How consistent is your sketch with your previous sketch of the direction field?

Sketch a solution curve through the point (.2, .25), and estimate the coordinates of the t = 1 point on this curve.

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Your solution:

(2 x - .5) * (t + 1) = 1

x = 1/[2(t + 1)] + .25

(2 x - .5) * (t + 1) = 0

x = .25

(2 x - .5) * (t + 1) = 2

x = 1/(t+1) + .25

(2 x - .5) * (t + 1) = -1

x = -1/ [2(t + 1)] + .25

The sketches seem very consistent with the direction field previously sketch. Comparing points they have in common, such as (0, .25), (0, .75) , (1, .25) , (1, .75), the slopes from the earlier computation are the same as the slopes from the curves.

As for the last question, sketching a curve through (.2, .25), I don't know how you can sketch a curve through an asymptote. To my knowledge, the curve would be undefined at this point.

confidence rating #$&*:

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Given Solution:

x ' = 1 when

(2 x - .5) * (t + 1) = 1.

Solving for x we obtain

x = 1/2 ( 1 / (t + 1) + .5) = 1 / (2(t + 1)) + .25.

The resulting curve is just the familiar curve x = 1 / t, vertically compressed by factor 2 then shifted -1 unit in the horizontal and .25 unit in the vertical direction, so its asymptotes are the lines t = -1 and x = .25. The t = 0 and t = 1 points are (0, .75) and (1, .5).

Similarly we find the curves corresponding to the other values of x ':

For x ' = 0 we get the horizontal line x = .25. Note that this line is the horizontal asymptote to the curve obtained in the preceding step.

For x ' = 2 we get the curve 1 / (t + 1) + .25, a curve with asymptotes at t = -1 and x = .25, including points (0, 1.25) and (1, .75).

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Self-critique (if necessary): OK

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Self-critique rating: OK

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Self-critique (if necessary):

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Self-critique rating:

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Excellent work. Do check my notes.

You appear to have a good background in physics, which you will find helpful in this course. This course will also expand your understanding of the physics of oscillating electrical and mechanical systems, and more.

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