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The electric potential \(\mathrm{V}\) is given as a function of distance \(\mathrm{x}\) (meter) by \(\mathrm{V}=\left(5 \mathrm{x}^{2}+10 \mathrm{x}-9\right)\) volt. Value of electric field at \(\mathrm{x}=1\) is \(\ldots \ldots\) \((\mathrm{A})-20(\mathrm{v} / \mathrm{m})\) (B) \(6(\mathrm{v} / \mathrm{m})\) (C) \(11(\mathrm{v} / \mathrm{m})\) (D) \(-23(\mathrm{v} / \mathrm{m})\)

Short Answer

Expert verified
The electric field E at x = 1 is -20 V/m. The correct answer is (A) -20 V/m.

Step by step solution

01

Find the derivative dV/dx of the potential V(x)

To find the derivative of V(x) with respect to x, differentiate the function with respect to x: \(V(x) = 5x^2 + 10x - 9\) Taking the derivative, we get: \(E = -\frac{dV}{dx} = -\frac{d(5x^2 + 10x - 9)}{dx}\)
02

Simplify the expression of the electric field E

Now we need to simplify the expression for E: Applying differentiation rules: \(E = - (10x + 10)\) Now we have the electric field E as a function of distance x.
03

Evaluate the electric field E at x = 1

We are asked to find the value of the electric field at x = 1. To do this, substitute the value x = 1 in the equation we found in Step 2: \(E(1) = -(10(1) + 10) = -20\) The value of the electric field E at x = 1 is -20 V/m. The correct answer is (A) -20 V/m.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Electric Potential
Electric potential is a fundamental concept in physics that represents the ability of an electric field to do work on a charge. It is often expressed as a function of the position in space, such as distance (in meters). Electric potential is comparable to gravitational potential energy, which is dependent on an object’s position in a gravitational field. In the context of our exercise, we have the electric potential as a quadratic function of distance:
- \(V(x) = 5x^2 + 10x - 9\).
By examining this function, you can identify how the electric potential changes as you move through the electric field. Calculating the electric potential at various points can help you understand the nature of the field itself.
Derivative
The derivative is a mathematical tool that helps us understand how a function changes as its input changes. Specifically, it gives us the rate at which one quantity changes with respect to another. In our exercise, the derivative of the electric potential function with respect to distance (x) is used to find the electric field. This is due to the relationship:
  • The electric field (E) is the negative gradient (derivative) of the electric potential (V).
Writing the derivative of the given function \(V(x)\):
- First term: \(d(5x^2)/dx = 10x\)
- Second term: \(d(10x)/dx = 10\)
- Constant term: \(d(-9)/dx = 0\)
Understanding derivatives is crucial in many fields beyond physics, as it quantifies how one variable changes with respect to another.
Differentiation
Differentiation is the process of finding the derivative of a function. It's an essential technique in calculus used to find rates of change, slopes of curves, and optimizing functions. In the context of this exercise, differentiation is applied to the electric potential function \(V(x)\) to obtain the electric field.
Differentiation follows certain rules:
  • Power Rule: When differentiating a term \(ax^n\), the result is \(nax^{n-1}\).
  • Constant Rule: The derivative of a constant is zero.
Applying these rules to \(V(x) = 5x^2 + 10x - 9\), we arrive at the derivative \(dV/dx = 10x + 10\). Successfully applying differentiation techniques is important for solving complex problems across numerous disciplines of science and engineering.
Electric Field Calculation
The electric field is a vector quantity that represents the force per unit charge experienced by a charge in the presence of an electric potential. To calculate the electric field from the electric potential function in this exercise, we took the derivative \(dV/dx\) and inserted a negative sign:
\(E = -dV/dx\). This reflects how the field relates oppositely to the potential gradient.
Once the expression for the electric field is found as \(E(x) = -(10x + 10)\), we can calculate its value at a specific point, as required:
  • Substitute \(x = 1\) into \(E(x)\).

The calculation gives \(E(1) = -(10(1) + 10) = -20\).
Thus, the electric field strength at \(x = 1\) meters is \(-20\) V/m, matching the solution's requirement. Calculating electric fields is vital in predicting how charges will move within fields, thus crucial in understanding physical phenomena at both macroscopic and atomic scales.

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Most popular questions from this chapter

In Millikan's oil drop experiment an oil drop carrying a charge Q is held stationary by a p.d. \(2400 \mathrm{v}\) between the plates. To keep a drop of half the radius stationary the potential difference had to be made \(600 \mathrm{v}\). What is the charge on the second drop? (A) \([(3 Q) / 2]\) (B) \((\mathrm{Q} / 4)\) (C) \(Q\) (D) \((\mathrm{Q} / 2)\)

Two point masses \(\mathrm{m}\) each carrying charge \(-\mathrm{q}\) and \(+\mathrm{q}\) are attached to the ends of a massless rigid non-conducting rod of length \(\ell\). The arrangement is placed in a uniform electric field \(\mathrm{E}\) such that the rod makes a small angle \(5^{\circ}\) with the field direction. The minimum time needed by the rod to align itself along the field is \(\ldots \ldots .\) (A) \(t=\pi \sqrt{[}(2 M \ell) /(3 q E)]\) (B) \(\mathrm{t}=(\pi / 2) \sqrt{[}(\mathrm{M} \ell) /(2 \mathrm{q} \mathrm{E})]\) (D) \(t=2 \pi \sqrt{[}(M \ell / E)]\)

A \(5 \mu \mathrm{F}\) capacitor is charged by a \(220 \mathrm{v}\) supply. It is then disconnected from the supply and is connected to another uncharged \(2.5 \mu \mathrm{F}\) capacitor. How much electrostatic energy of the first capacitor is lost in the form of heat and electromagnetic radiation ? (A) \(0.02 \mathrm{~J}\) (B) \(0.121 \mathrm{~J}\) (C) \(0.04 \mathrm{~J}\) (D) \(0.081 \mathrm{~J}\)

The electric Potential \(\mathrm{V}\) at any Point \(0(\mathrm{x}, \mathrm{y}, \mathrm{z}\) all in meters \()\) in space is given by \(\mathrm{V}=4 \mathrm{x}^{2}\) volt. The electric field at the point \((1 \mathrm{~m}, 0.2 \mathrm{~m})\) in volt meter is \(\ldots \ldots .\) (A) 8 , along negative \(\mathrm{x}\) - axis (B) 8 , along positives \(\mathrm{x}\) - axis (C) 16 , along negative \(\mathrm{x}\) -axis (D) 16 , along positives \(\mathrm{x}\) -axis

The electric Potential at a point \(\mathrm{P}(\mathrm{x}, \mathrm{y}, \mathrm{z})\) is given by \(\mathrm{V}=-\mathrm{x}^{2} \mathrm{y}-\mathrm{x} \mathrm{z}^{3}+4\). The electric field \(\mathrm{E}^{\boldsymbol{T}}\) at that point is \(\ldots \ldots\) (A) \(i \wedge\left(2 \mathrm{xy}+\mathrm{z}^{3}\right)+\mathrm{j} \wedge \mathrm{x}^{2}+\mathrm{k} \wedge 3 \mathrm{xz}^{2}\) (B) \(i \wedge 2 \mathrm{xy}+\mathrm{j} \wedge\left(\mathrm{x}^{2}+\mathrm{y}^{2}\right)+\mathrm{k} \wedge\left(3 \mathrm{xy}-\mathrm{y}^{2}\right)\) (C) \(i \wedge z^{3}+j \wedge x y z+k \wedge z^{2}\) (D) \(i \wedge\left(2 x y-z^{3}\right)+j \wedge x y^{2}+k \wedge 3 z^{2} x\)

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