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PHIL 200 Lecture 6: Nozick’s Trading Theory of Knowledge

Factive: p is true, s believes that p, if p weren"t true, s wouldn"t believe p tracking, if p were true, s would believe p. If the temp were different the thermometer would read differently. Know stuff even if you cant prove it. Unknown to you, the clock stopped exactly 24 h ago. Jtb: you do know its 10:29: fails in russell"s clock case. If the conservatives hadn"t won the last election, the ndp would have. Close to the real/closest scenario (next closest to the winning one) P: ticket # 324 is a loser-million ticket lottery. Does s know ticket #324 is a loser. Even if it is a loser, you don"t know it. Condition 3 fails because if you did have the winning ticket, you wouldn"t believe you had a winning ticket before announcement. Nozick: s doesn"t know ticket #324 is a loser.

Canada

Introduction to Philosophy 1

Philosophy

Michael Blome Tillmann

McGill University

Management in Global Context

World of Chemistry: Food

Macroeconomic Policy

Greek Mythology

Introduction to East Asian History

Modern East Asian History

Health and the Healer in Western History

History of Communication

Introduction to Financial Accounting

Introduction to Organizational Behaviour

Business Statistics

Information Systems

Principles of Marketing

Operations Management

Marketing Strategy

Brand Management

Consumer Behaviour

Integrated Mktg Communications

International Marketing Management

Basic Materials: Western Music

The Art of Listening

The Milky Way Inside and Out

Expressive Analysis for Management

Current Economic Problems: Topics

<p>&lt;p&gt;A velocity selector is designed to only allow particles toenter a mass spectrometer if they are traveling at precisely 8.0km/s. The magnetic field within the mass spectrometer has astrength 100 mT. The particles in the mass spectrometer travelthrough a semi circle and strike a detector 2.00 cm away from theentrance slit. Which atom is the most likely identity of theseparticles? (1 atomic mass unit=1.67 x10&lt;sup&gt;-27&lt;/sup&gt;kg)&lt;/p&gt;<br>&lt;p&gt;a. &lt;sup&gt;2&lt;/sup&gt;H&lt;/p&gt;<br>&lt;p&gt;b. &lt;sup&gt;12&lt;/sup&gt;C&lt;/p&gt;<br>&lt;p&gt;c. &lt;sup&gt;24&lt;/sup&gt;Mg&lt;/p&gt;<br>&lt;p&gt;d. &lt;sup&gt;56&lt;/sup&gt;Fe&lt;/p&gt;<br>&lt;p&gt;Please show steps to solve.&lt;/p&gt;</p>

<p>The rms speed of molecules in a gas is 678 m/s<br><br>What will be the rms speed if the gas pressure and volume are bothdoubled?<br><br><br><br>Vrms = â(3KbT/M) = (1/3)(N/V)v^2rms=P</p> <p>678m/s= 2(P*V)</p>

<picture><source srcset="https://prealliance-textbook-qa.oneclass.com/qa_images/homework_help/question/qa_images/154/15445876.jpeg" type="image/webp"></source><img src="https://prealliance-textbook-qa.oneclass.com/qa_images/homework_help/question/qa_images/154/15445876.jpeg" alt=""></picture><div>QUESTION: How do I derive Equations 3, 4a, and 4b? Helpandexplanations are greatly appreciated!</div> <div id="flg" class="hidden">Consider an elastic(H) collision between two particles moving in ID. We have particles m1 and m2 moving with velocities mu 1 and mu 2 before the collision and v1 , v2 after the collision. We know that kinetic energy (KE) and linear momentum (P) are conserved, as Delta P = (Pf-Pi) = 0 Eq. 1 Delta KE = (KEf - KEi) = 0 Eq.2 It is also useful to formulate these fundamental relations in terms of velocities (see your phyl21 textbook). Thus we have (for elastic collisions) (v2-v1)(mu 2-u1)=-1 eq.3 or in other words "the relative velocities after/before are equal but opposite". This is true for any mass values. A somewhat more restrictive case is for mu 2 = 0 (stationary "target" m2). Then it can be shown that v1 = (m 1 -m2)u 1 /(m 1 +m2) Eq. 4a v2 = (2m 1 )u 1 /(m 1 +m2). Eq. 4b Note that the ratio r = v1/v2 is constant here where u2=0.</div>

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PHIL 200 Lecture 6: Nozick’s Trading Theory of Knowledge

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