AP Calculus AB › Integrals
A particle at the origin has an initial velocity of . If its acceleration is given by
, find the position of the particle after 1 second.
In this problem, letting denote the position of the particle and
denote the velocity, we know that
. Integrating and working backwards we have,
Plugging in our initial condition, , we see immediately that
.
Repeating the process again for , we find that
Plugging in our initial condition, (we started at the origin) we see that
. This gives us a final equation
. The problem asks for
which is simply
Solve the separable differential equation:
and at
To solve the separable differential equation, we must separate x and y to the same sides as their respective derivatives:
Next, we integrate both sides:
The integrals were solved using the following rules:
,
The two constants of integration were combined to make a single one.
Now, we exponentiate both sides to solve for y:
Using the properties of exponents, we can rearrange the integration constant:
(The exponential of the constant is itself a constant.)
Using the given condition, we can solve for C:
Our final answer is
Given that and
, solve for
. What is the value of
?
1
This is a separable differential equation. The simplest way to approach this is to turn into
, and then by abusing the notation, "multiplying by dx" on both sides.
We then group all the y terms with dy, and all the x terms with dx.
Integrating both sides, we find
Here, the first integral is found by using substitution of variables, setting . In addition, we have chosen to only put a +C on the second integral, as if we put it on both, we would just combine them in any case.
To solve for y, we multiply both sides by two and raise e to both sides to get rid of the natural logarithm.
(Note, C was multiplied by two, but it's still just an arbitrary constant. If you prefer, you may call the new C value .)
Now we drop our absolute value signs, and note that we can take out a factor of and stick in front of the right hand side.
As is just another arbitrary constant, we can relabel this as C, or
if you prefer. Solving for y gets us
Next, we plug in our initial condition to solve for C.
;
Leaving us with a final equation of
Plugging in x = 4, we have a final answer,
Find (dy/dx).
sin(xy) = x + cos(y)
dy/dx = (1 – ycos(xy))/(xcos(xy) + sin(y))
dy/dx = (1 – cos(xy))/(cos(xy) + sin(y))
dy/dx = (xcos(xy) + sin(y))/(1 – ycos(xy))
dy/dx = (cos(xy) + sin(y))/(1 – cos(xy))
None of the above
The first step of the problem is to differentiate with respect to (dy/dx):
cos(xy)\[(x)(dy/dx) + y(1)\] = 1 – sin(y)(dy/dx)
*Note: When differentiating cos(xy) remember to use the product rule. (xy' + x'y)
Step 2: Clean the differentiated problem up
cos(xy)(x)(dy/dx) + cos(xy)y = 1 – sin(y)(dy/dx)
cos(xy)(x)(dy/dx) + sin(y)(dy/dx) = 1 – cos(xy)y
Step 3: Solve for (dy/dx)
dy/dx = (1 – ycos(xy))/(xcos(xy) + sin(y))
Find the derivative:
To find the derivative, multiply the exponent by the coefficent in front of the x term and then decrease the exponent by 1:
Integrate:
To integrate, the following substitution was made:
Now, we rewrite the integral in terms of u and integrate:
The following rule was used for integration:
Finally, rewrite the final answer in terms of our original x term: