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Assertion Force constant, \(k=\frac{Y A}{l}\), where \(Y\) is Young's modulus, \(A\) is area and \(l\) is original length of the given spring. Reason Force constant in case of a given spring is called spring constant.

Short Answer

Expert verified
Both the assertion and reason are true; the reason correctly explains the terminology 'spring constant.'

Step by step solution

01

Understanding the Assertion

The assertion states that the force constant of a spring is given by the formula \(k = \frac{Y A}{l}\), where \(Y\) is Young's modulus, \(A\) is the cross-sectional area, and \(l\) is the original length. In physics, this form of \(k\) denotes the spring's resistance to deformation when an axial force is applied, which depends on material properties and dimensions.
02

Understanding the Reason

The reason provided asserts that the term 'force constant' in the context of a spring is often referred to as the 'spring constant.' The spring constant measures a spring's stiffness, the proportionality factor in Hooke's law, which relates the force exerted by the spring and its displacement: \(F = kx\).
03

Evaluating the Assertion and Reason

Both the assertion and the reason address the concept of a spring constant. The assertion provides a specific formula for calculating the spring constant based on material properties, while the reason clarifies the terminology, identifying the force constant with the more commonly known term, 'spring constant.' Both statements are true, and the reason accurately explains why the term 'force constant' is also known as 'spring constant' in the context of springs.

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Key Concepts

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

Young's Modulus
Young's modulus is a measure of the stiffness of a solid material. It is a fundamental property of materials in physics and engineering and helps describe how a material will deform under stress. When force is applied to a material, it can either stretch or compress. The stress is the force applied divided by the area it acts on, and the strain is how much the material deforms divided by its original length. Young's modulus is the ratio of stress to strain:\[ Y = \frac{\text{Stress}}{\text{Strain}} = \frac{F / A}{\Delta L / L_0} \]where:
  • \( F \) is the force applied,
  • \( A \) is the cross-sectional area,
  • \( \Delta L \) is the change in length (deformation),
  • \( L_0 \) is the original length.
Young’s modulus shows how much a material will stretch or compress for a given amount of stress. A higher Young's modulus indicates a stiffer material that doesn't tend to deform much. By using Young's modulus in the formula for the spring constant, we relate the material's inherent property to the spring's ability to resist deformation.
Hooke's Law
Hooke's Law is a principle in physics that explains the relationship between the force applied to a spring and the extension or compression of the spring. It is usually expressed in the formula:\[ F = kx \]where:
  • \( F \) is the force exerted by the spring,
  • \( x \) is the displacement of the spring from its equilibrium position,
  • \( k \) is the spring constant, or force constant, which measures the spring's stiffness.
According to Hooke's Law, the force needed to either compress or extend a spring by a certain distance is proportional to that distance. This law is valid as long as the spring is not stretched beyond its elastic limit, where it would not return to its original shape. Hooke's Law is crucial for understanding how springs behave under force, and it can also be generalized to describe other elastic bodies in physics. By using Hooke's Law, we can calculate how much force is needed to move a spring a certain distance, which is important in designing systems that use springs.
Force Constant
The force constant of a spring, also known as the spring constant, denotes the spring's stiffness, essentially determining how much force is needed to extend or compress the spring by a certain length. In the context of the formula \( k = \frac{Y A}{l} \), the force constant \( k \) depends on Young’s modulus \( Y \), the cross-sectional area \( A \), and the original length \( l \) of the spring:
  • Young's modulus \( Y \) provides information about the material's intrinsic stiffness.
  • The area \( A \) affects how the force is distributed across the spring.
  • The length \( l \) determines how much the spring can stretch or compress.
This formula derives from the theory that the force constant is directly proportional to the material's rigidity and size while being inversely proportional to its length. Thus, shorter and more rigid springs with larger cross-sections will have higher force constants, indicating they are stiffer and require more force for the same amount of displacement compared to longer, less rigid springs. The force constant is crucial in determining the behavior of springs in mechanical systems and plays a key role in applications ranging from automotive suspension systems to simple toys.

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Most popular questions from this chapter

Two identical wires are suspended from the same rigid support but one is of copper and the other is of iron. Young's modulus of iron is thrice that of copper. The weights to be added on copper and iron wires so that the ends are on the same level must be in the ratio of (a) \(1: 3\) (b) \(2: 1\) (c) \(3: 1\) (d) \(4: 1\)

The force constant of a wire is \(k\) and that of another wire of the same material is \(2 k\). When both the wires are stretched, then work done is (a) \(W_{2}=1.5 W_{1}\) (b) \(W_{2}=2 W_{1}\) (c) \(W_{2}=W_{1}\) (d) \(W_{2}=0.5 \mathrm{~W}_{1}\)

A wire extends by \(1 \mathrm{~mm}\) when a force is applied. Double the force is applied to another wire of same material and length but half the radius of cross-section. The elongation of the wire in mm will be (a) 8 (b) 4 (c) 2 (d) 1

Two wires, one made of copper and other of steel are joined end to end (as shown in figure). The area of cross-section of copper wire is twice that of steel wire. They are placed under compressive force of magnitudes \(F\). The ratio for their lengths such that change in lengths of both wires are same is \(\left(Y_{s}=2 \times\right.\) \(10^{11} \mathrm{Nm}^{-2}\) and \(Y_{C}=1.1 \times 10^{11} \mathrm{Nm}^{-2}\) ) (a) \(2.1\) (b) \(1.1\) (c) \(1.2\) (d) 2

Consider two cylindrical rods of identical dimensions, one of rubber and the other of steel. Both the rods are fixed rigidly at one end to the roof. A mass \(M\) is attached to each of the free ends at the centre of the rods. (a) Both the rods will clongate but there shall be no perceptible change in shape (b) The stecl rod will elongate and change shape but the rubber rod will only elongate (c) The steel rod will elongate without ary perceptible change in shape, but the rubber rod will elongate and the shape of the bottom edge will change to an ellipse. (d) The steel rod will clongate, without any perceptible change in shape, but the rubber rod will elongate with the shape of the bottom edge tapered to a tip at the centre

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