We are given the differential equation:
\[ (t + 1) \frac{dx}{dt} = 2x + (t + 1)^4 \]
To solve this, divide both sides by \((t + 1)\):
\[ \frac{dx}{dt} = \frac{2x}{t + 1} + (t + 1)^3 \]
Now, separate the variables:
\[ \frac{dx}{2x} = \frac{1}{t + 1} dt + (t + 1)^2 dt \]
We can now integrate both sides:
\[ \int \frac{1}{2x} dx = \int \left(\frac{1}{t + 1} + (t + 1)^2\right) dt \]
The left-hand side gives:
\[ \frac{1}{2} \ln |x| \]
For the right-hand side, integrate each term:
\[ \int \frac{1}{t + 1} dt = \ln |t + 1| \quad \text{and} \quad \int (t + 1)^2 dt = \frac{(t + 1)^3}{3} \]
Thus, we have:
\[ \frac{1}{2} \ln |x| = \ln |t + 1| + \frac{(t + 1)^3}{3} + C \]
Exponentiate both sides:
\[ |x| = e^{2 \ln |t + 1| + \frac{2(t + 1)^3}{3} + 2C} \]
Simplify:
\[ x = A(t + 1)^2 e^{\frac{2(t + 1)^3}{3}} \]
Now, use the initial condition \(x(0) = 2\):
\[ x(0) = A(1)^2 e^0 = 2 \implies A = 2 \]
Thus, the solution is:
\[ x = 2(t + 1)^2 e^{\frac{2(t + 1)^3}{3}} \]
Finally, calculate \(x(1)\):
\[ x(1) = 2(1 + 1)^2 e^{\frac{2(2)^3}{3}} = 2(2)^2 e^{\frac{16}{3}} = 2 \times 4 \times e^{\frac{16}{3}} \approx 14 \]
Find \( x(1) \) given the differential equation \( (t + 1) dx = \left(2x + (t + 1)^4\right) dt \), with initial condition \( x(0) = 2 \).
This is a first order linear differential equation. The standard form is \( \frac{dx}{dt} + P(t)x = Q(t) \). The solution is found using the integrating factor method, where the integrating factor (I.F.) is \( e^{\int P(t) dt} \). The general solution is then given by \( x \cdot \text{(I.F.)} = \int Q(t) \cdot \text{(I.F.)} dt + C \).
Step 1: Rewrite the given differential equation in the standard linear form.
\[ (t + 1) dx = \left(2x + (t + 1)^4\right) dt \] \[ \frac{dx}{dt} = \frac{2x + (t + 1)^4}{t + 1} \] \[ \frac{dx}{dt} = \frac{2}{t+1}x + (t+1)^3 \] \[ \frac{dx}{dt} - \frac{2}{t+1}x = (t+1)^3 \]
This is now in the form \( \frac{dx}{dt} + P(t)x = Q(t) \), where \( P(t) = -\frac{2}{t+1} \) and \( Q(t) = (t+1)^3 \).
Step 2: Find the Integrating Factor (I.F.).
\[ \text{I.F.} = e^{\int P(t) dt} = e^{\int -\frac{2}{t+1} dt} = e^{-2 \ln|t+1|} = e^{\ln((t+1)^{-2})} = (t+1)^{-2} \]
Step 3: Multiply the standard form equation by the Integrating Factor.
\[ (t+1)^{-2} \frac{dx}{dt} - \frac{2}{(t+1)^3}x = (t+1)^3 \cdot (t+1)^{-2} \] \[ \frac{d}{dt}\left[ x \cdot (t+1)^{-2} \right] = (t+1) \]
The left side is the derivative of \( x \cdot \text{(I.F.)} \).
Step 4: Integrate both sides with respect to \( t \).
\[ \int \frac{d}{dt}\left[ x \cdot (t+1)^{-2} \right] dt = \int (t+1) dt \] \[ x \cdot (t+1)^{-2} = \frac{(t+1)^2}{2} + C \]
Where \( C \) is the constant of integration.
Step 5: Apply the initial condition \( x(0) = 2 \) to find the constant \( C \).
\[ 2 \cdot (0+1)^{-2} = \frac{(0+1)^2}{2} + C \] \[ 2 \cdot 1 = \frac{1}{2} + C \] \[ 2 - \frac{1}{2} = C \implies C = \frac{3}{2} \]
Step 6: Write the particular solution of the differential equation.
\[ x \cdot (t+1)^{-2} = \frac{(t+1)^2}{2} + \frac{3}{2} \] \[ x = (t+1)^{2} \left( \frac{(t+1)^2}{2} + \frac{3}{2} \right) \] \[ x = \frac{(t+1)^4 + 3(t+1)^2}{2} \]
Step 7: Substitute \( t = 1 \) to find \( x(1) \).
\[ x(1) = \frac{(1+1)^4 + 3(1+1)^2}{2} \] \[ x(1) = \frac{(2)^4 + 3(2)^2}{2} \] \[ x(1) = \frac{16 + 3 \cdot 4}{2} = \frac{16 + 12}{2} = \frac{28}{2} = 14 \]
Hence, the value of \( x(1) \) is 14.
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
