Problem 63
Question
The charge flowing through a resistance \(R\) varies with time \(t\) as \(Q=a t-b t^{2} .\) The total heat produced in \(R\) from \(t=0\) to the time when value of \(Q\) becomes again zero is (A) \(\frac{a^{3} R}{6 b}\) (B) \(\frac{a^{3} R}{3 b}\) (C) \(\frac{a^{3} R}{2 b}\) (D) \(\frac{a^{3} R}{b}\)
Step-by-Step Solution
Verified Answer
The total heat produced in the resistance from \(t=0\) to the time when the value of \(Q\) becomes again zero is \(\frac{a^{3} R}{6 b}\).
1Step 1: Calculate the current
First, we need to find the current flowing through the resistance. Knowing that \(i(t)=\frac{dQ}{dt}\), we differentiate the given equation of \(Q(t)\) with respect to time:
\(i(t) = \frac{dQ}{dt} = \frac{d(at - bt^2)}{dt} = a - 2bt\)
2Step 2: Calculate the power
Now, we will find the instantaneous power being dissipated through the resistance using the formula \(P = i^2R\):
\(P(t) = i^2(t)R = (a - 2bt)^2R\)
3Step 3: Determine the time when the value of Q is zero again
To find when the charge becomes zero again, we have to solve the equation \(Q(t) = 0\) for \(t\):
\(at - bt^2 = 0\)
Which gives, \(t(at - bt) = 0\)
The two solutions are \(t=0\) and \(t = \frac{a}{b}\). Since we already know that \(t=0\) is the starting time, the second solution, \(t=\frac{a}{b}\), is the time when the charge becomes zero again.
4Step 4: Calculate the total heat produced
To find the total heat produced in the resistance, we integrate the instantaneous power over the time interval \(t=0\) to \(t=\frac{a}{b}\):
\[
H = \int_0^\frac{a}{b} P(t)dt = R \int_0^\frac{a}{b}(a - 2bt)^2dt
\]
5Step 5: Evaluate the integral
Evaluate the integral to get the total heat produced:
\[
H = R \int_0^\frac{a}{b}(a^2 - 4abt + 4b^2t^2)dt = R \left[ a^2t - \frac{4}{3}abt^2 + \frac{4}{3}b^2t^3 \right]_0^\frac{a}{b}
\]
6Step 6: Plug in the values
Substitute the values (\(t = \frac{a}{b}\)) into the integral and simplify:
\[
H = R \left( a^2 \cdot \frac{a}{b} - \frac{4}{3}ab \cdot \left(\frac{a}{b}\right)^2 + \frac{4}{3}b^2 \cdot \left(\frac{a}{b}\right)^3 \right)
\]
After simplification, we get
\[
H = \frac{a^3 R}{6b}
\]
So the correct answer is (A).
Other exercises in this chapter
Problem 54
\(n\) identical cells, each of emf \(\varepsilon\) and internal resistance \(r\), are joined in series to form a closed circuit. The potential difference across
View solution Problem 62
If \(\mathrm{EMF}\) in a thermocouple is \(\varepsilon=\alpha T+\beta T^{2}\), then the neutral temperature of the thermocouple is (A) \(-\beta /(2 \alpha)\) (B
View solution Problem 65
The charge flowing through a resistance \(R\) varies with time \(t\) as \(Q=a t-b t^{2} .\) The total heat produced in \(R\) from \(t=0\) to the time when value
View solution Problem 70
In the given circuit, find the equivalent resistance between points \(A\) and \(B\). (A) \(18 \Omega\) (B) \(12 \Omega\) (C) \(20 \Omega\) (D) \(27 \Omega\)
View solution