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To find the coefficient of \( x^3 \) in the function \( h(x) = f(x+1) - g(x+2) \), we first need to expand each component.
Step 1: Expand \( f(x+1) \)
Starting with \( f(x+1) = a_1 + 10(x+1) + a_2(x+1)^2 + a_3(x+1)^3 + (x+1)^4 \), expand each term:
1. \( 10(x+1) = 10x + 10 \)
2. \( a_2(x+1)^2 = a_2(x^2 + 2x + 1) = a_2x^2 + 2a_2x + a_2 \)
3. \( a_3(x+1)^3 = a_3(x^3 + 3x^2 + 3x + 1) = a_3x^3 + 3a_3x^2 + 3a_3x + a_3 \)
4. \( (x+1)^4 = x^4 + 4x^3 + 6x^2 + 4x + 1 \)
Collecting terms for the \( x^3 \) coefficient in \( f(x+1) \):
\( a_3x^3 + 4x^3 = (a_3 + 4)x^3 \)
Step 2: Expand \( g(x+2) \)
Next, expand \( g(x+2) = b_1 + 3(x+2) + b_2(x+2)^2 + b_3(x+2)^3 + (x+2)^4 \):
1. \( 3(x+2) = 3x + 6 \)
2. \( b_2(x+2)^2 = b_2(x^2 + 4x + 4) = b_2x^2 + 4b_2x + 4b_2 \)
3. \( b_3(x+2)^3 = b_3(x^3 + 6x^2 + 12x + 8) = b_3x^3 + 6b_3x^2 + 12b_3x + 8b_3 \)
4. \( (x+2)^4 = x^4 + 8x^3 + 24x^2 + 32x + 16 \)
Collecting terms for the \( x^3 \) coefficient in \( g(x+2) \):
\( b_3x^3 + 8x^3 = (b_3 + 8)x^3 \)
Step 3: Calculate the coefficient of \( x^3 \) in \( h(x) \)
The coefficient of \( x^3 \) in \( h(x) = f(x+1) - g(x+2) \) is:
\((a_3 + 4) - (b_3 + 8) = a_3 + 4 - b_3 - 8 = a_3 - b_3 - 4\)
Step 4: Conclusion
Since \( f(x) \neq g(x) \) for any \( x \), it implies \( a_3 \neq b_3 \), the specific values don't make a difference to the meaning of this expression, the coefficient remains constant as:-4
The number of zeroes of a polynomial \( y = p(x) \) as shown below is:
In the circuit below, \( M_1 \) is an ideal AC voltmeter and \( M_2 \) is an ideal AC ammeter. The source voltage (in Volts) is \( v_s(t) = 100 \cos(200t) \). What should be the value of the variable capacitor \( C \) such that the RMS readings on \( M_1 \) and \( M_2 \) are 25 V and 5 A, respectively?
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):
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Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
A conducting square loop of side $ L $, mass $ M $, and resistance $ R $ is moving in the $ XY $ plane with its edges parallel to the $ X $ and $ Y $ axes. The region $ y \geq 0 $ has a uniform magnetic field, $ \vec{B} = B_0 \hat{k} $. The magnetic field is zero everywhere else. At time $ t = 0 $, the loop starts to enter the magnetic field with an initial velocity $ v_0 \hat{j} \, \text{m/s} $, as shown in the figure. Considering the quantity $ K = \frac{B_0^2 L^2}{RM} $ in appropriate units, ignoring self-inductance of the loop and gravity, which of the following statements is/are correct: