What are the challenges of solving partial derivative problems in mathematics?

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The discussion addresses challenges in solving partial derivative problems in mathematics, focusing on two specific homework questions. The first problem involves finding the first partial derivatives of the function f(x, y) = ∫(y to x) cos(t^2) dt, which can be solved using the Fundamental Theorem of Calculus without direct integration. The second problem applies Ohm's Law to determine how current changes in an electrical circuit as voltage and resistance vary, utilizing the Quotient Rule for differentiation. The solution for the current change is calculated as approximately -3.1 x 10^(-5) Amps/sec. Overall, the conversation emphasizes understanding the application of calculus principles rather than simply providing answers.
tandoorichicken
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Two homework problems I can't get.

(1) The question is find the first partial derivatives of the function. The problem is that the function in this problem is
f(x, y) = \int_{y}^{x} \cos{t^2} dt
The main obstacle is getting past this function. I can't integrate it and neither can my calculator. Is there a way to do this problem without integrating, or how do you integrate this function?

(2) The voltage V in a simple electrical circuit is slowly decreasing as the battery wears out. The resistance R is slowly increasing as the resistor heats up. Use Ohm's Law, V = IR, to find how the current I is changing at the moment when R = 400\Omega, I = 0.08 A, \frac{dV}{dt} = -0.01 V/s, and \frac{dR}{dt} = 0.03 \Omega/s.
 
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1.How about applying the fundamental theorem of calculus...??Both parts of it.

2.Differentiate wrt time the Ohm's law and plug in tht #-s.

Daniel.
 
tandoorichicken said:
Two homework problems I can't get.

(1) The question is find the first partial derivatives of the function. The problem is that the function in this problem is
f(x, y) = \int_{y}^{x} \cos{t^2} dt
The main obstacle is getting past this function. I can't integrate it and neither can my calculator. Is there a way to do this problem without integrating, or how do you integrate this function?

(2) The voltage V in a simple electrical circuit is slowly decreasing as the battery wears out. The resistance R is slowly increasing as the resistor heats up. Use Ohm's Law, V = IR, to find how the current I is changing at the moment when R = 400\Omega, I = 0.08 A, \frac{dV}{dt} = -0.01 V/s, and \frac{dR}{dt} = 0.03 \Omega/s.

{#1}

NO integration needed here. Use the Fundamental Theorem of Calculus:

f(x, y) = \int_{y}^{x} \cos{t^2} dt

\frac {\partial f(x,y)} {\partial x} = \cos{x^2}

\frac {\partial f(x,y)} {\partial y} = -\cos{y^2}


Incidentally, in the more general case, we have:

f(x, y) = \int_{y}^{g(x)} h(t) dt

\frac {\partial f(x,y)} {\partial x} = h(g(x))*g'(x)


{#2}

V = I*R
-----> I = V/R
Using the Quotient Rule:
(dI/dt) = {(dV/dt)*R - V*(dR/dt)}/(R^2)
(dI/dt) = {(dV/dt)*R - (I*R)*(dR/dt)}/(R^2)
(dI/dt) = {(dV/dt) - (I)*(dR/dt)}/(R)

Placing given values into the above equation, we get:
(dI/dt) = {(-0.01 V/s) - (0.08 A)*(0.03 ohm/s)}/(400 ohm)
(dI/dt) = (-3.1)x10^(-5) Amps/sec
~
 
Last edited:
Well,the general idea of this specific forum is not to solve his problems entirely,but to help him solve them by himself.
I hope u'l get it.

Daniel.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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