(a) To Prove: When light source is moving obliquely towards Q, the observed frequency is f o b s = f s c e ( 1 − β cos θ ) γ .

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Answer 1

Question

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

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A planar double pendulum consists of two point masses \[m_1 = 1.00~\mathrm{kg}, \qquad m_2 = 1.00~\mathrm{kg}\]connected by massless, rigid rods of lengths \[L_1 = 1.00~\mathrm{m}, \qquad L_2 = 1.20~\mathrm{m}.\]The upper rod is hinged to a fixed pivot; gravity acts vertically downward with\[g = 9.81~\mathrm{m\,s^{-2}}.\]Define the generalized coordinates \(\theta_1,\theta_2\) as the angles each rod makes with thedownward vertical (positive anticlockwise, measured in radians unless stated otherwise).At \(t=0\) the system is released from rest with \[\theta_1(0)=120^{\circ}, \qquad\theta_2(0)=-10^{\circ}, \qquad\dot{\theta}_1(0)=\dot{\theta}_2(0)=0 .\]Using the exact nonlinear equations of motion (no small-angle or planar-pendulumapproximations) and assuming the rods never stretch or slip, determine the angle\(\theta_2\) at the instant\[t = 10.0~\mathrm{s}.\]Give the result in degrees, in the interval \((-180^{\circ},180^{\circ}]\).

What are the expected readings of the ammeter and voltmeter for the circuit in the figure below? (R = 5.60 Ω, ΔV = 6.30 V) ammeter I =

simple diagram to illustrate the setup for each law- coulombs law and biot savart law

Answer 2

Question

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Expert Solution & Answer

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Check out a sample textbook solution

See solution

Answer 3

Question

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Expert Solution & Answer

Want to see the full answer?

Check out a sample textbook solution

See solution

Answer 4

Question

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Expert Solution & Answer

Want to see the full answer?

Check out a sample textbook solution

See solution

Answer 5

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Answer 6

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

Answer 7

Chapter 1, Problem 1.53P

To determine

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

Answer 8

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Answer 9

To determine

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Answer 10

Expert Solution & Answer

Answer 11

Expert Solution & Answer

Answer 12

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Answer 13

Ch. 1 - Prob. 1.1P Ch. 1 - Prob. 1.2P Ch. 1 - Prob. 1.3P Ch. 1 - Prob. 1.4P Ch. 1 - Prob. 1.5P Ch. 1 - Prob. 1.6P Ch. 1 - Prob. 1.7P Ch. 1 - Prob. 1.8P Ch. 1 - Prob. 1.9P Ch. 1 - Prob. 1.10P

(a) To Prove: When light source is moving obliquely towards Q, the observed frequency is f o b s = f s c e ( 1 − β cos θ ) γ .

Solution Summary: The author calculates the frequency of light moving from the source towards the observer located at point Q.

Videos

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Want to see the full answer?

Chapter 1 Solutions

(a) To Prove: When light source is moving obliquely towards Q, the observed frequency is f o b s = f s c e ( 1 − β cos θ ) γ .

Solution Summary: The author calculates the frequency of light moving from the source towards the observer located at point Q.

Videos

(a) To Prove: When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

(b) To Prove: When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .

Want to see the full answer?

Chapter 1 Solutions

(a)

To Prove:

When light source is moving obliquely towards Q, the observed frequency is fobs=fsce(1−βcosθ)γ .

(b)

To Prove:

When the source is moving direct head on towards the observer, the observed frequency is fobs=fsce(1−β)γ .